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Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improv The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improv The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improv The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improv The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improv The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improv The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years. The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^-$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively. CLIC uses a two-beam acceleration scheme, in which 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept has been refined using improved software tools. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations and parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25-30 years. Burrows, P.N.; Catalan Lasheras, N.; Linssen, L.; Petrič, M.; Robson, A.; Schulte, D.; Sicking, E.; Stapnes, S.; Charles, T.K.; Giansiracusa, P.J.; Lucas, T.G.; Rassool, R.P.; Volpi, M.; Balazs, C.; Afanaciev, K.; Makarenko, V.; Patapenka, A.; Zhuk, I.; Collette, C.; Boland, M.J.; Abusleme Hoffman, A.C.; Diaz, M.A.; Garay, F.; Chi, Y.; He, X.; Pei, G.; Pei, S.; Shu, G.; Wang, X.; Zhang, J.; Zhao, F.; Zhou, Z.; Chen, H.; Gao, Y.; Huang, W.; Kuang, Y.P.; Li, B.; Li, Y.; Meng, X.; Shao, J.; Shi, J.; Tang, C.; Wang, P.; Wu, X.; Zha, H.; Ma, L.; Han, Y.; Fang, W.; Gu, Q.; Huang, D.; Huang, X.; Tan, J.; Wang, Z.; Zhao, Z.; Uggerhøj, U.I.; Wistisen, T.N.; Aabloo, A.; Aare, R.; Kuppart, K.; Vigonski, S.; Zadin, V.; Aicheler, M.; Baibuz, E.; Brücken, E.; Djurabekova, F.; Eerola, P.; Garcia, F.; Haeggström, E.; Huitu, K.; Jansson, V.; Kassamakov, I.; Kimari, J.; Kyritsakis, A.; Lehti, S.; Meriläinen, A.; Montonen, R.; Nordlund, K.; Österberg, K.; Saressalo, A.; Väinölä, J.; Veske, M.; Farabolini, W.; Mollard, A.; Peauger, F.; Plouin, J.; Bambade, P.; Chaikovska, I.; Chehab, R.; Delerue, N.; Davier, M.; Faus-Golfe, A.; Irles, A.; Kaabi, W.; LeDiberder, F.; Pöschl, R.; Zerwas, D.; Aimard, B.; Balik, G.; Blaising, J.-J.; Brunetti, L.; Chefdeville, M.; Dominjon, A.; Drancourt, C.; Geoffroy, N.; Jacquemier, J.; Jeremie, A.; Karyotakis, Y.; Nappa, J.M.; Serluca, M.; Vilalte, S.; Vouters, G.; Bernhard, A.; Bründermann, E.; Casalbuoni, S.; Hillenbrand, S.; Gethmann, J.; Grau, A.; Huttel, E.; Müller, A.-S.; Peiffer, P.; Perić, I.; Saez de Jauregui, D.; Emberger, L.; Graf, C.; Simon, F.; Szalay, M.; van der Kolk, N.; Brass, S.; Kilian, W.; Alexopoulos, T.; Apostolopoulos, T.; Gazis, E.N.; Gazis, N.; Kostopoulos, V.; Kourkoulis, S.; Heilig, B.; Lichtenberger, J.; Shrivastava, P.; Dayyani, M.K.; Ghasem, H.; Hajari, S.S.; Shaker, H.; Ashkenazy, Y.; Popov, I.; Engelberg, E.; Yashar, A.; Abramowicz, H.; Benhammou, Y.; Borysov, O.; Borysova, M.; Levy, A.; Levy, I.; Alesini, D.; 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Monogr." name="citation_journal_title" /> <meta content="2" name="citation_volume" /> <meta content="2018/12/14" name="citation_publication_date" /> <meta name="citation_online_date" content="2018/12/18"> <meta content="CERN-2018-005-M" name="citation_technical_report_number" /> <meta content="arXiv:1812.06018" name="citation_technical_report_number" /> <meta content="CERN-2018-005" name="citation_technical_report_number" /> <meta content="CERN-2018-005-M" name="citation_technical_report_number" /> <meta content="CERN-2018-005" name="citation_technical_report_number" /> <meta content="9789290835066" name="citation_isbn" /> <meta content="9789290835073" name="citation_isbn" /> <meta content="10.23731/CYRM-2018-002" name="citation_doi" /> <meta name="citation_pdf_url" content="https://cds.cern.ch/record/2652188/files/CLICSummaryReport.pdf" /> <meta name="citation_pdf_url" content="https://cds.cern.ch/record/2652188/files/66-67-PB.pdf" /> <meta name="citation_pdf_url" content="https://cds.cern.ch/record/2652188/files/1812.06018.pdf" />  <meta content="The Compact Linear Collider (CLIC) - 2018 Summary Report" property="og:title" /> <meta content="arXiv" property="og:title" /> <meta content="website" property="og:type" /> <meta content="website" property="og:type" /> <meta content="website" property="og:type" /> <meta content="https://cds.cern.ch/record/2652188" property="og:url" /> <meta name="twitter:image" content="https://cds.cern.ch/record/2652188/files/66-67-PB.gif?subformat=icon" /> <meta property="og:image" content="https://cds.cern.ch/record/2652188/files/66-67-PB.gif?subformat=icon" /> <meta property="og:image:secure_url" content="https://cds.cern.ch/record/2652188/files/66-67-PB.gif?subformat=icon" /> <meta property="og:image" content="https://cds.cern.ch/record/2652188/files/Front cover.png?subformat=icon-180" /> <meta property="og:image:secure_url" content="https://cds.cern.ch/record/2652188/files/Front cover.png?subformat=icon-180" /> <meta property="og:image" content="https://cds.cern.ch/record/2652188/files/Front cover.png" /> <meta property="og:image:secure_url" content="https://cds.cern.ch/record/2652188/files/Front cover.png" /> <meta property="og:image" content="https://cds.cern.ch/record/2652188/files/66-67-PB.jpg?subformat=icon-180" /> <meta property="og:image:secure_url" content="https://cds.cern.ch/record/2652188/files/66-67-PB.jpg?subformat=icon-180" /> <meta property="og:image" content="https://cds.cern.ch/record/2652188/files/66-67-PB.gif?subformat=icon" /> <meta property="og:image:secure_url" content="https://cds.cern.ch/record/2652188/files/66-67-PB.gif?subformat=icon" /> <meta property="og:image" content="https://cds.cern.ch/record/2652188/files/66-67-PB.jpg?subformat=icon-700" /> <meta property="og:image:secure_url" content="https://cds.cern.ch/record/2652188/files/66-67-PB.jpg?subformat=icon-700" /> <meta property="og:image" content="https://cds.cern.ch/record/2652188/files/Front cover.gif?subformat=icon" /> <meta property="og:image:secure_url" content="https://cds.cern.ch/record/2652188/files/Front cover.gif?subformat=icon" /> <meta property="og:image" content="https://cds.cern.ch/record/2652188/files/Front cover.png?subformat=icon-180" /> <meta property="og:image:secure_url" content="https://cds.cern.ch/record/2652188/files/Front cover.png?subformat=icon-180" /> <meta property="og:image" content="https://cds.cern.ch/record/2652188/files/Front cover.png?subformat=icon-700" /> <meta property="og:image:secure_url" content="https://cds.cern.ch/record/2652188/files/Front cover.png?subformat=icon-700" /> <meta content="CERN Document Server" property="og:site_name" /> <meta content="The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^-$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively. CLIC uses a two-beam acceleration scheme, in which 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept has been refined using improved software tools. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations and parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25-30 years." property="og:description" /> <meta content="arXiv" property="og:description" /> <meta content="The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years." property="og:description" /> <meta content="The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improv" property="og:description" />  <meta content="summary" name="twitter:card" /> <meta content="summary" name="twitter:card" /> <style></style> </head> <body class="CERN32Document32Server search" lang="en">  <div id="cern-toolbar"> <h1><a href="http://cern.ch" title="CERN">CERN <span>Accelerating science</span></a></h1> <ul> <li class="cern-accountlinks"><a class="cern-account" href="https://cds.cern.ch/youraccount/login?ln=en&referer=https%3A//cds.cern.ch/record/2652188" title="Sign in to your CERN account">Sign in</a></li> <li><a class="cern-directory" href="http://cern.ch/directory" title="Search CERN resources and browse the directory">Directory</a></li> </ul> </div>   <div role="banner" class="clearfix" id="header"> <div class="header-inner inner"> <hgroup class="clearfix"> <h2 id="site-name"> <a rel="home" title="Home" href="/"><span>CERN Document Server</span></a> </h2> <h3 id="site-slogan">Access articles, reports and multimedia content in HEP</h3> </hgroup> <div role="navigation" id="main-navigation" class="cdsmenu"> <h2 class="element-invisible">Main menu</h2><ul class="links inline clearfix"> <li class="menu-386 first active-trail"><a class="active-trail" href="https://cds.cern.ch/?ln=en">Search</a></li> <li class="menu-444 "><a class="" title="" href="https://cds.cern.ch/submit?ln=en">Submit</a></li> <li class="menu-426 "><a class="" href="https://cds.cern.ch/help/?ln=en">Help</a></li> <li class="leaf hassubcdsmenu"> <a hreflang="en" class="header" href="https://cds.cern.ch/youraccount/display?ln=en">Personalize</a> <ul class="subsubcdsmenu"><li><a href="https://cds.cern.ch/youralerts/list?ln=en">Your alerts</a></li><li><a href="https://cds.cern.ch/yourbaskets/display?ln=en">Your baskets</a></li><li><a href="https://cds.cern.ch/yourcomments?ln=en">Your comments</a></li><li><a href="https://cds.cern.ch/youralerts/display?ln=en">Your searches</a></li></ul></li> </ul> </div> </div> </div>  <table class="navtrailbox"> <tr> <td class="navtrailboxbody"> <a href="/?ln=en" class="navtrail">Home</a> > The Compact Linear Collider (CLIC) - 2018 Summary Report </td> </tr> </table> </div> <div class="pagebody"><div class="pagebodystripemiddle"> <div class="detailedrecordbox"> <div class="detailedrecordtabs"> <div> <ul class="detailedrecordtabs"><li class="on first"><a href="/record/2652188/?ln=en">Information </a></li><li class=""><a href="/record/2652188/files?ln=en">Files </a></li></ul> <div id="tabsSpacer" style="clear:both;height:0px"> </div></div> </div> <div class="detailedrecordboxcontent"> <div class="top-left-folded"></div> <div class="top-right-folded"></div> <div class="inside">  <abbr class="unapi-id" title="2652188"></abbr> <style type="text/css">  </style> <script type="text/javascript" src="/js/pdf-previewer-append-to-table.js"></script> <table class="formatRecordTableFullWidth" > <tr> <td class="formatRecordHeader" style="background-image: url('https://cds.cern.ch/img/journals.jpg');" colspan="2"> Report </td> </tr> <tr><td class="formatRecordLabel"> Report number </td><td style="padding-left:5px;"><a href="http://arxiv.org/abs/arXiv:1812.06018">arXiv:1812.06018</a> ; CERN-2018-005-M ; CERN-2018-005 ; CERN-2018-005-M ; CERN-2018-005</td></tr> <tr><td class="formatRecordLabel"> Title </td><td style="padding-left:5px;"><b>The Compact Linear Collider (CLIC) - 2018 Summary Report</b></td></tr> <tr><td class="formatRecordLabel"></td><td style="padding-left:5px;"> <style> .yr_cover { position: absolute; display: none; z-index: 9999; margin-left: 2px; -moz-box-shadow: 2px 2px 6px gray; -webkit-box-shadow: 2px 2px 6px gray; -o-box-shadow: 2px 2px 6px gray; box-shadow: 2px 2px 6px gray; } </style> <script> $(window).bind("load", function() { $("#yr_cover_2652188_target").mouseover(function() { $("body").append("<div id='yr_cover_2652188' class='yr_cover'><img style='max-height: 640px; max-width: 480px;' src='https://cds.cern.ch/record/2652188/files/Front cover.png' /></div>"); $("#yr_cover_2652188").css('top', $("#yr_cover_2652188_target").offset().top + 'px'); $("#yr_cover_2652188").css('left', ($("#yr_cover_2652188_target").offset().left + $("#yr_cover_2652188_target").outerWidth()) + 'px'); 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toggle_authors_visibility(); } </script> <a name="show_hide" /><p id="more" style=""><a href="https://cds.cern.ch/search?f=author&p=Burrows%2C%20P.N.&ln=en">Burrows, P.N.</a> (ed.) (JAI, UK) ; <a href="https://cds.cern.ch/search?f=author&p=Catalan%20Lasheras%2C%20N.&ln=en">Catalan Lasheras, N.</a> (ed.) (CERN) ; <a href="https://cds.cern.ch/search?f=author&p=Linssen%2C%20L.&ln=en">Linssen, L.</a> (ed.) (CERN) ; <a href="https://cds.cern.ch/search?f=author&p=Petri%C4%8D%2C%20M.&ln=en">Petrič, M.</a> (ed.) (CERN) ; <a href="https://cds.cern.ch/search?f=author&p=Robson%2C%20A.&ln=en">Robson, A.</a> (ed.) (Glasgow U.) ; <a href="https://cds.cern.ch/search?f=author&p=Schulte%2C%20D.&ln=en">Schulte, D.</a> (ed.) (CERN) ; <a href="https://cds.cern.ch/search?f=author&p=Sicking%2C%20E.&ln=en">Sicking, E.</a> (ed.) (CERN) ; <a href="https://cds.cern.ch/search?f=author&p=Stapnes%2C%20S.&ln=en">Stapnes, S.</a> (ed.) (CERN) ; <a href="https://cds.cern.ch/search?f=author&p=Charles%2C%20T.K.&ln=en">Charles, T.K.</a> (Melbourne U.) ; <a href="https://cds.cern.ch/search?f=author&p=Giansiracusa%2C%20P.J.&ln=en">Giansiracusa, P.J.</a> (Melbourne U.) ; <a href="https://cds.cern.ch/search?f=author&p=Lucas%2C%20T.G.&ln=en">Lucas, T.G.</a> (Melbourne U.) ; <a href="https://cds.cern.ch/search?f=author&p=Rassool%2C%20R.P.&ln=en">Rassool, R.P.</a> (Melbourne U.) ; <a href="https://cds.cern.ch/search?f=author&p=Volpi%2C%20M.&ln=en">Volpi, M.</a> (Melbourne U.) ; <a href="https://cds.cern.ch/search?f=author&p=Balazs%2C%20C.&ln=en">Balazs, C.</a> (Monash U.) ; <a href="https://cds.cern.ch/search?f=author&p=Afanaciev%2C%20K.&ln=en">Afanaciev, K.</a> (Belarus State U.) ; <a href="https://cds.cern.ch/search?f=author&p=Makarenko%2C%20V.&ln=en">Makarenko, V.</a> (Belarus State U.) ; <a href="https://cds.cern.ch/search?f=author&p=Patapenka%2C%20A.&ln=en">Patapenka, A.</a> (Joint Inst. Power Nucl. Res., Minsk) ; <a href="https://cds.cern.ch/search?f=author&p=Zhuk%2C%20I.&ln=en">Zhuk, I.</a> (Joint Inst. Power Nucl. Res., Minsk) ; <a href="https://cds.cern.ch/search?f=author&p=Collette%2C%20C.&ln=en">Collette, C.</a> (Brussels U.) ; <a href="https://cds.cern.ch/search?f=author&p=Boland%2C%20M.J.&ln=en">Boland, M.J.</a> (Saskatchewan U.) ; <a href="https://cds.cern.ch/search?f=author&p=Abusleme%20Hoffman%2C%20A.C.&ln=en">Abusleme Hoffman, A.C.</a> (Chile U., Catolica) ; <a href="https://cds.cern.ch/search?f=author&p=Diaz%2C%20M.A.&ln=en">Diaz, M.A.</a> (Chile U., Catolica) ; <a href="https://cds.cern.ch/search?f=author&p=Garay%2C%20F.&ln=en">Garay, F.</a> (Chile U., Catolica) ; <a href="https://cds.cern.ch/search?f=author&p=Chi%2C%20Y.&ln=en">Chi, Y.</a> (Beijing, Inst. High Energy Phys.) ; <a href="https://cds.cern.ch/search?f=author&p=He%2C%20X.&ln=en">He, X.</a> (Beijing, Inst. High Energy Phys.) ; <a href="https://cds.cern.ch/search?f=author&p=Pei%2C%20G.&ln=en">Pei, G.</a> (Beijing, Inst. High Energy Phys.) ; <a href="https://cds.cern.ch/search?f=author&p=Pei%2C%20S.&ln=en">Pei, S.</a> (Beijing, Inst. High Energy Phys.) ; <a href="https://cds.cern.ch/search?f=author&p=Shu%2C%20G.&ln=en">Shu, G.</a> (Beijing, Inst. High Energy Phys.) ; <a href="https://cds.cern.ch/search?f=author&p=Wang%2C%20X.&ln=en">Wang, X.</a> (Beijing, Inst. High Energy Phys.) ; <a href="https://cds.cern.ch/search?f=author&p=Zhang%2C%20J.&ln=en">Zhang, J.</a> (Beijing, Inst. High Energy Phys.) ; <a href="https://cds.cern.ch/search?f=author&p=Zhao%2C%20F.&ln=en">Zhao, F.</a> (Beijing, Inst. High Energy Phys.) ; <a href="https://cds.cern.ch/search?f=author&p=Zhou%2C%20Z.&ln=en">Zhou, Z.</a> (Beijing, Inst. High Energy Phys.) ; <a href="https://cds.cern.ch/search?f=author&p=Chen%2C%20H.&ln=en">Chen, H.</a> (Tsinghua U., Beijing) ; <a href="https://cds.cern.ch/search?f=author&p=Gao%2C%20Y.&ln=en">Gao, Y.</a> (Tsinghua U., Beijing) ; <a href="https://cds.cern.ch/search?f=author&p=Huang%2C%20W.&ln=en">Huang, W.</a> (Tsinghua U., Beijing) ; <a href="https://cds.cern.ch/search?f=author&p=Kuang%2C%20Y.P.&ln=en">Kuang, Y.P.</a> (Tsinghua U., Beijing) ; <a href="https://cds.cern.ch/search?f=author&p=Li%2C%20B.&ln=en">Li, B.</a> (Tsinghua U., Beijing) ; <a href="https://cds.cern.ch/search?f=author&p=Li%2C%20Y.&ln=en">Li, Y.</a> (Tsinghua U., Beijing) ; <a href="https://cds.cern.ch/search?f=author&p=Meng%2C%20X.&ln=en">Meng, X.</a> (Tsinghua U., Beijing) ; <a href="https://cds.cern.ch/search?f=author&p=Shao%2C%20J.&ln=en">Shao, J.</a> (Tsinghua U., Beijing) ; <a href="https://cds.cern.ch/search?f=author&p=Shi%2C%20J.&ln=en">Shi, J.</a> (Tsinghua U., Beijing) ; <a href="https://cds.cern.ch/search?f=author&p=Tang%2C%20C.&ln=en">Tang, C.</a> (Tsinghua U., Beijing) ; <a href="https://cds.cern.ch/search?f=author&p=Wang%2C%20P.&ln=en">Wang, P.</a> (Tsinghua U., Beijing) ; <a href="https://cds.cern.ch/search?f=author&p=Wu%2C%20X.&ln=en">Wu, X.</a> (Tsinghua U., Beijing) ; <a href="https://cds.cern.ch/search?f=author&p=Zha%2C%20H.&ln=en">Zha, H.</a> (Tsinghua U., Beijing) ; <a href="https://cds.cern.ch/search?f=author&p=Ma%2C%20L.&ln=en">Ma, L.</a> (Shandong U.) ; <a href="https://cds.cern.ch/search?f=author&p=Han%2C%20Y.&ln=en">Han, Y.</a> (Shandong U.) ; <a href="https://cds.cern.ch/search?f=author&p=Fang%2C%20W.&ln=en">Fang, W.</a> (SINAP, Shanghai) ; <a href="https://cds.cern.ch/search?f=author&p=Gu%2C%20Q.&ln=en">Gu, Q.</a> (SINAP, Shanghai) ; <a href="https://cds.cern.ch/search?f=author&p=Huang%2C%20D.&ln=en">Huang, D.</a> (SINAP, Shanghai) ; <a href="https://cds.cern.ch/search?f=author&p=Huang%2C%20X.&ln=en">Huang, X.</a> (SINAP, Shanghai) ; <a href="https://cds.cern.ch/search?f=author&p=Tan%2C%20J.&ln=en">Tan, J.</a> (SINAP, Shanghai) ; <a href="https://cds.cern.ch/search?f=author&p=Wang%2C%20Z.&ln=en">Wang, Z.</a> (SINAP, Shanghai) ; <a href="https://cds.cern.ch/search?f=author&p=Zhao%2C%20Z.&ln=en">Zhao, Z.</a> (SINAP, Shanghai) ; <a href="https://cds.cern.ch/search?f=author&p=Uggerh%C3%B8j%2C%20U.I.&ln=en">Uggerhøj, U.I.</a> (Aarhus U.) ; <a href="https://cds.cern.ch/search?f=author&p=Wistisen%2C%20T.N.&ln=en">Wistisen, T.N.</a> (Aarhus U.) ; <a href="https://cds.cern.ch/search?f=author&p=Aabloo%2C%20A.&ln=en">Aabloo, A.</a> (Tartu State U.) ; <a href="https://cds.cern.ch/search?f=author&p=Aare%2C%20R.&ln=en">Aare, R.</a> (Tartu State U.) ; <a href="https://cds.cern.ch/search?f=author&p=Kuppart%2C%20K.&ln=en">Kuppart, K.</a> (Tartu State U.) ; <a href="https://cds.cern.ch/search?f=author&p=Vigonski%2C%20S.&ln=en">Vigonski, S.</a> (Tartu State U.) ; <a href="https://cds.cern.ch/search?f=author&p=Zadin%2C%20V.&ln=en">Zadin, V.</a> (Tartu State U.) ; <a href="https://cds.cern.ch/search?f=author&p=Aicheler%2C%20M.&ln=en">Aicheler, M.</a> (Helsinki Inst. of Phys.) ; <a href="https://cds.cern.ch/search?f=author&p=Baibuz%2C%20E.&ln=en">Baibuz, E.</a> (Helsinki Inst. of Phys.) ; <a href="https://cds.cern.ch/search?f=author&p=Br%C3%BCcken%2C%20E.&ln=en">Brücken, E.</a> (Helsinki Inst. of Phys.) ; <a href="https://cds.cern.ch/search?f=author&p=Djurabekova%2C%20F.&ln=en">Djurabekova, F.</a> (Helsinki Inst. of Phys.) ; <a href="https://cds.cern.ch/search?f=author&p=Eerola%2C%20P.&ln=en">Eerola, P.</a> (Helsinki Inst. of Phys.) ; <a href="https://cds.cern.ch/search?f=author&p=Garcia%2C%20F.&ln=en">Garcia, F.</a> (Helsinki Inst. of Phys.) ; <a href="https://cds.cern.ch/search?f=author&p=Haeggstr%C3%B6m%2C%20E.&ln=en">Haeggström, E.</a> (Helsinki Inst. of Phys.) ; <a href="https://cds.cern.ch/search?f=author&p=Huitu%2C%20K.&ln=en">Huitu, K.</a> (Helsinki Inst. of Phys.) ; <a href="https://cds.cern.ch/search?f=author&p=Jansson%2C%20V.&ln=en">Jansson, V.</a> (Helsinki Inst. of Phys.) ; <a href="https://cds.cern.ch/search?f=author&p=Kassamakov%2C%20I.&ln=en">Kassamakov, I.</a> (Helsinki Inst. of Phys.) ; <a href="https://cds.cern.ch/search?f=author&p=Kimari%2C%20J.&ln=en">Kimari, J.</a> (Helsinki Inst. of Phys.) ; <a href="https://cds.cern.ch/search?f=author&p=Kyritsakis%2C%20A.&ln=en">Kyritsakis, A.</a> (Helsinki Inst. of Phys.) ; <a href="https://cds.cern.ch/search?f=author&p=Lehti%2C%20S.&ln=en">Lehti, S.</a> (Helsinki Inst. of Phys.) ; <a href="https://cds.cern.ch/search?f=author&p=Meril%C3%A4inen%2C%20A.&ln=en">Meriläinen, A.</a> (Helsinki Inst. of Phys.) ; <a href="https://cds.cern.ch/search?f=author&p=Montonen%2C%20R.&ln=en">Montonen, R.</a> (Helsinki Inst. of Phys.) ; <a href="https://cds.cern.ch/search?f=author&p=Nordlund%2C%20K.&ln=en">Nordlund, K.</a> (Helsinki Inst. of Phys.) ; <a href="https://cds.cern.ch/search?f=author&p=%C3%96sterberg%2C%20K.&ln=en">Österberg, K.</a> (Helsinki Inst. of Phys.) ; <a href="https://cds.cern.ch/search?f=author&p=Saressalo%2C%20A.&ln=en">Saressalo, A.</a> (Helsinki Inst. of Phys.) ; <a href="https://cds.cern.ch/search?f=author&p=V%C3%A4in%C3%B6l%C3%A4%2C%20J.&ln=en">Väinölä, J.</a> (Helsinki Inst. of Phys.) ; <a href="https://cds.cern.ch/search?f=author&p=Veske%2C%20M.&ln=en">Veske, M.</a> (Helsinki Inst. of Phys.) ; <a href="https://cds.cern.ch/search?f=author&p=Farabolini%2C%20W.&ln=en">Farabolini, W.</a> (Saclay) ; <a href="https://cds.cern.ch/search?f=author&p=Mollard%2C%20A.&ln=en">Mollard, A.</a> (Saclay) ; <a href="https://cds.cern.ch/search?f=author&p=Peauger%2C%20F.&ln=en">Peauger, F.</a> (Saclay) ; <a href="https://cds.cern.ch/search?f=author&p=Plouin%2C%20J.&ln=en">Plouin, J.</a> (Saclay) ; <a href="https://cds.cern.ch/search?f=author&p=Bambade%2C%20P.&ln=en">Bambade, P.</a> (Orsay, LAL) ; <a href="https://cds.cern.ch/search?f=author&p=Chaikovska%2C%20I.&ln=en">Chaikovska, I.</a> (Orsay, LAL) ; <a href="https://cds.cern.ch/search?f=author&p=Chehab%2C%20R.&ln=en">Chehab, R.</a> (Orsay, LAL) ; <a href="https://cds.cern.ch/search?f=author&p=Delerue%2C%20N.&ln=en">Delerue, N.</a> (Orsay, LAL) ; <a href="https://cds.cern.ch/search?f=author&p=Davier%2C%20M.&ln=en">Davier, M.</a> (Orsay, LAL) ; <a href="https://cds.cern.ch/search?f=author&p=Faus-Golfe%2C%20A.&ln=en">Faus-Golfe, A.</a> (Orsay, LAL) ; 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<a href="https://cds.cern.ch/search?f=author&p=Bernhard%2C%20A.&ln=en">Bernhard, A.</a> (KIT, Karlsruhe, IPE) ; <a href="https://cds.cern.ch/search?f=author&p=Br%C3%BCndermann%2C%20E.&ln=en">Bründermann, E.</a> (KIT, Karlsruhe, IPE) ; <a href="https://cds.cern.ch/search?f=author&p=Casalbuoni%2C%20S.&ln=en">Casalbuoni, S.</a> (KIT, Karlsruhe, IPE) ; <a href="https://cds.cern.ch/search?f=author&p=Hillenbrand%2C%20S.&ln=en">Hillenbrand, S.</a> (KIT, Karlsruhe, IPE) ; <a href="https://cds.cern.ch/search?f=author&p=Gethmann%2C%20J.&ln=en">Gethmann, J.</a> (KIT, Karlsruhe, IPE) ; <a href="https://cds.cern.ch/search?f=author&p=Grau%2C%20A.&ln=en">Grau, A.</a> (KIT, Karlsruhe, IPE) ; <a href="https://cds.cern.ch/search?f=author&p=Huttel%2C%20E.&ln=en">Huttel, E.</a> (KIT, Karlsruhe, IPE) ; <a href="https://cds.cern.ch/search?f=author&p=M%C3%BCller%2C%20A.-S.&ln=en">Müller, A.-S.</a> (KIT, Karlsruhe, IPE) ; <a href="https://cds.cern.ch/search?f=author&p=Peiffer%2C%20P.&ln=en">Peiffer, P.</a> (KIT, Karlsruhe, IPE) ; <a href="https://cds.cern.ch/search?f=author&p=Peri%C4%87%2C%20I.&ln=en">Perić, I.</a> (KIT, Karlsruhe, IPE) ; <a href="https://cds.cern.ch/search?f=author&p=Saez%20de%20Jauregui%2C%20D.&ln=en">Saez de Jauregui, D.</a> (KIT, Karlsruhe, IPE) ; <a href="https://cds.cern.ch/search?f=author&p=Emberger%2C%20L.&ln=en">Emberger, L.</a> (Munich, Max Planck Inst.) ; <a href="https://cds.cern.ch/search?f=author&p=Graf%2C%20C.&ln=en">Graf, C.</a> (Munich, Max Planck Inst.) ; <a href="https://cds.cern.ch/search?f=author&p=Simon%2C%20F.&ln=en">Simon, F.</a> (Munich, Max Planck Inst.) ; <a href="https://cds.cern.ch/search?f=author&p=Szalay%2C%20M.&ln=en">Szalay, M.</a> (Munich, Max Planck Inst.) ; <a href="https://cds.cern.ch/search?f=author&p=van%20der%20Kolk%2C%20N.&ln=en">van der Kolk, N.</a> (Munich, Max Planck Inst.) ; <a href="https://cds.cern.ch/search?f=author&p=Brass%2C%20S.&ln=en">Brass, S.</a> (Siegen U.) ; <a href="https://cds.cern.ch/search?f=author&p=Kilian%2C%20W.&ln=en">Kilian, W.</a> (Siegen U.) ; <a href="https://cds.cern.ch/search?f=author&p=Alexopoulos%2C%20T.&ln=en">Alexopoulos, T.</a> (Natl. Tech. U., Athens) ; <a href="https://cds.cern.ch/search?f=author&p=Apostolopoulos%2C%20T.&ln=en">Apostolopoulos, T.</a> (Natl. Tech. U., Athens) ; <a href="https://cds.cern.ch/search?f=author&p=Gazis%2C%20E.N.&ln=en">Gazis, E.N.</a> (Natl. Tech. U., Athens) ; <a href="https://cds.cern.ch/search?f=author&p=Gazis%2C%20N.&ln=en">Gazis, N.</a> (Natl. Tech. U., Athens) ; <a href="https://cds.cern.ch/search?f=author&p=Kostopoulos%2C%20V.&ln=en">Kostopoulos, V.</a> (Natl. Tech. U., Athens) ; <a href="https://cds.cern.ch/search?f=author&p=Kourkoulis%2C%20S.&ln=en">Kourkoulis, S.</a> (Natl. Tech. U., Athens) ; <a href="https://cds.cern.ch/search?f=author&p=Heilig%2C%20B.&ln=en">Heilig, B.</a> (Eotvos U.) ; <a href="https://cds.cern.ch/search?f=author&p=Lichtenberger%2C%20J.&ln=en">Lichtenberger, J.</a> (Eotvos U.) ; <a href="https://cds.cern.ch/search?f=author&p=Shrivastava%2C%20P.&ln=en">Shrivastava, P.</a> (CAT, INDUS) ; <a href="https://cds.cern.ch/search?f=author&p=Dayyani%2C%20M.K.&ln=en">Dayyani, M.K.</a> (IPM, Tehran) ; <a href="https://cds.cern.ch/search?f=author&p=Ghasem%2C%20H.&ln=en">Ghasem, H.</a> (IPM, Tehran) ; <a href="https://cds.cern.ch/search?f=author&p=Hajari%2C%20S.S.&ln=en">Hajari, S.S.</a> (IPM, Tehran) ; <a href="https://cds.cern.ch/search?f=author&p=Shaker%2C%20H.&ln=en">Shaker, H.</a> (IPM, Tehran) ; <a href="https://cds.cern.ch/search?f=author&p=Ashkenazy%2C%20Y.&ln=en">Ashkenazy, Y.</a> (Hebrew U.) ; <a href="https://cds.cern.ch/search?f=author&p=Popov%2C%20I.&ln=en">Popov, I.</a> (Hebrew U.) ; <a href="https://cds.cern.ch/search?f=author&p=Engelberg%2C%20E.&ln=en">Engelberg, E.</a> (Hebrew U.) ; <a href="https://cds.cern.ch/search?f=author&p=Yashar%2C%20A.&ln=en">Yashar, A.</a> (Hebrew U.) ; <a href="https://cds.cern.ch/search?f=author&p=Abramowicz%2C%20H.&ln=en">Abramowicz, H.</a> (Tel Aviv U.) ; <a href="https://cds.cern.ch/search?f=author&p=Benhammou%2C%20Y.&ln=en">Benhammou, Y.</a> (Tel Aviv U.) ; <a href="https://cds.cern.ch/search?f=author&p=Borysov%2C%20O.&ln=en">Borysov, O.</a> (Tel Aviv U.) ; <a href="https://cds.cern.ch/search?f=author&p=Borysova%2C%20M.&ln=en">Borysova, M.</a> (Tel Aviv U.) ; <a href="https://cds.cern.ch/search?f=author&p=Levy%2C%20A.&ln=en">Levy, A.</a> (Tel Aviv U.) ; <a href="https://cds.cern.ch/search?f=author&p=Levy%2C%20I.&ln=en">Levy, I.</a> (Tel Aviv U.) ; <a href="https://cds.cern.ch/search?f=author&p=Alesini%2C%20D.&ln=en">Alesini, D.</a> (Frascati) ; <a href="https://cds.cern.ch/search?f=author&p=Bellaveglia%2C%20M.&ln=en">Bellaveglia, M.</a> (Frascati) ; <a href="https://cds.cern.ch/search?f=author&p=Buonomo%2C%20B.&ln=en">Buonomo, B.</a> (Frascati) ; <a href="https://cds.cern.ch/search?f=author&p=Cardelli%2C%20A.&ln=en">Cardelli, A.</a> (Frascati) ; <a href="https://cds.cern.ch/search?f=author&p=Diomede%2C%20M.&ln=en">Diomede, M.</a> (Frascati) ; <a href="https://cds.cern.ch/search?f=author&p=Ferrario%2C%20M.&ln=en">Ferrario, M.</a> (Frascati) ; <a href="https://cds.cern.ch/search?f=author&p=Gallo%2C%20A.&ln=en">Gallo, A.</a> (Frascati) ; <a href="https://cds.cern.ch/search?f=author&p=Ghigo%2C%20A.&ln=en">Ghigo, A.</a> (Frascati) ; <a href="https://cds.cern.ch/search?f=author&p=Giribono%2C%20A.&ln=en">Giribono, A.</a> (Frascati) ; <a href="https://cds.cern.ch/search?f=author&p=Piersanti%2C%20L.&ln=en">Piersanti, L.</a> (Frascati) ; <a href="https://cds.cern.ch/search?f=author&p=Stella%2C%20A.&ln=en">Stella, A.</a> (Frascati) ; <a href="https://cds.cern.ch/search?f=author&p=Vaccarezza%2C%20C.&ln=en">Vaccarezza, C.</a> (Frascati) ; <a href="https://cds.cern.ch/search?f=author&p=de%20Blas%2C%20J.&ln=en">de Blas, J.</a> (INFN, Padua ; Trento U.) ; <a href="https://cds.cern.ch/search?f=author&p=Franceschini%2C%20R.&ln=en">Franceschini, R.</a> (INFN, Rome3 ; Rome III U.) ; <a href="https://cds.cern.ch/search?f=author&p=D%27Auria%2C%20G.&ln=en">D'Auria, G.</a> (Sincrotrone Trieste) ; <a href="https://cds.cern.ch/search?f=author&p=Di%20Mitri%2C%20S.&ln=en">Di Mitri, S.</a> (Sincrotrone Trieste) ; <a href="https://cds.cern.ch/search?f=author&p=Abe%2C%20T.&ln=en">Abe, T.</a> (KEK, Tsukuba) ; <a href="https://cds.cern.ch/search?f=author&p=Aryshev%2C%20A.&ln=en">Aryshev, A.</a> (KEK, Tsukuba) ; <a href="https://cds.cern.ch/search?f=author&p=Fukuda%2C%20M.&ln=en">Fukuda, M.</a> (KEK, Tsukuba) ; <a href="https://cds.cern.ch/search?f=author&p=Furukawa%2C%20K.&ln=en">Furukawa, K.</a> (KEK, Tsukuba) ; <a href="https://cds.cern.ch/search?f=author&p=Hayano%2C%20H.&ln=en">Hayano, H.</a> (KEK, Tsukuba) ; <a href="https://cds.cern.ch/search?f=author&p=Higashi%2C%20Y.&ln=en">Higashi, Y.</a> (KEK, Tsukuba) ; <a href="https://cds.cern.ch/search?f=author&p=Higo%2C%20T.&ln=en">Higo, T.</a> (KEK, Tsukuba) ; <a href="https://cds.cern.ch/search?f=author&p=Kubo%2C%20K.&ln=en">Kubo, K.</a> (KEK, Tsukuba) ; <a href="https://cds.cern.ch/search?f=author&p=Kuroda%2C%20S.&ln=en">Kuroda, S.</a> (KEK, Tsukuba) ; <a href="https://cds.cern.ch/search?f=author&p=Matsumoto%2C%20S.&ln=en">Matsumoto, S.</a> (KEK, Tsukuba) ; <a href="https://cds.cern.ch/search?f=author&p=Michizono%2C%20S.&ln=en">Michizono, S.</a> (KEK, Tsukuba) ; <a href="https://cds.cern.ch/search?f=author&p=Naito%2C%20T.&ln=en">Naito, T.</a> (KEK, Tsukuba) ; <a href="https://cds.cern.ch/search?f=author&p=Okugi%2C%20T.&ln=en">Okugi, T.</a> (KEK, Tsukuba) ; <a href="https://cds.cern.ch/search?f=author&p=Shidara%2C%20T.&ln=en">Shidara, T.</a> (KEK, Tsukuba) ; <a href="https://cds.cern.ch/search?f=author&p=Tauchi%2C%20T.&ln=en">Tauchi, T.</a> (KEK, Tsukuba) ; <a href="https://cds.cern.ch/search?f=author&p=Terunuma%2C%20N.&ln=en">Terunuma, N.</a> (KEK, Tsukuba) ; <a href="https://cds.cern.ch/search?f=author&p=Urakawa%2C%20J.&ln=en">Urakawa, J.</a> (KEK, Tsukuba) ; <a href="https://cds.cern.ch/search?f=author&p=Yamamoto%2C%20A.&ln=en">Yamamoto, A.</a> (KEK, Tsukuba) ; <a href="https://cds.cern.ch/search?f=author&p=Raboanary%2C%20R.&ln=en">Raboanary, R.</a> (iHEP-MAD) ; <a href="https://cds.cern.ch/search?f=author&p=Luiten%2C%20O.J.&ln=en">Luiten, O.J.</a> (Eindhoven, Tech. U.) ; <a href="https://cds.cern.ch/search?f=author&p=Stragier%2C%20X.F.D.&ln=en">Stragier, X.F.D.</a> (Eindhoven, Tech. U.) ; <a href="https://cds.cern.ch/search?f=author&p=Hart%2C%20R.&ln=en">Hart, R.</a> (Nikhef, Amsterdam) ; <a href="https://cds.cern.ch/search?f=author&p=van%20der%20Graaf%2C%20H.&ln=en">van der Graaf, H.</a> (Nikhef, Amsterdam) ; <a href="https://cds.cern.ch/search?f=author&p=Eigen%2C%20G.&ln=en">Eigen, G.</a> (Bergen U.) ; <a href="https://cds.cern.ch/search?f=author&p=Adli%2C%20E.&ln=en">Adli, E.</a> (Oslo U.) ; <a href="https://cds.cern.ch/search?f=author&p=Lindstr%C3%B8m%2C%20C.A.&ln=en">Lindstrøm, C.A.</a> (Oslo U.) ; <a href="https://cds.cern.ch/search?f=author&p=Lillest%C3%B8l%2C%20R.&ln=en">Lillestøl, R.</a> (Oslo U.) ; <a href="https://cds.cern.ch/search?f=author&p=Malina%2C%20L.&ln=en">Malina, L.</a> (Oslo U.) ; <a href="https://cds.cern.ch/search?f=author&p=Pfingstner%2C%20J.&ln=en">Pfingstner, J.</a> (Oslo U.) ; <a href="https://cds.cern.ch/search?f=author&p=Sjobak%2C%20K.N.&ln=en">Sjobak, K.N.</a> (Oslo U.) ; <a href="https://cds.cern.ch/search?f=author&p=Ahmad%2C%20A.&ln=en">Ahmad, A.</a> (NCP, Islamabad) ; <a href="https://cds.cern.ch/search?f=author&p=Hoorani%2C%20H.&ln=en">Hoorani, H.</a> (NCP, Islamabad) ; <a href="https://cds.cern.ch/search?f=author&p=Khan%2C%20W.A.&ln=en">Khan, W.A.</a> (NCP, Islamabad) ; <a href="https://cds.cern.ch/search?f=author&p=Bugiel%2C%20S.&ln=en">Bugiel, S.</a> (AGH-UST, Cracow) ; <a href="https://cds.cern.ch/search?f=author&p=Bugiel%2C%20R.&ln=en">Bugiel, R.</a> (AGH-UST, Cracow) ; <a href="https://cds.cern.ch/search?f=author&p=Firlej%2C%20M.&ln=en">Firlej, M.</a> (AGH-UST, Cracow) ; <a href="https://cds.cern.ch/search?f=author&p=Fiutowski%2C%20T.A.&ln=en">Fiutowski, T.A.</a> (AGH-UST, Cracow) ; <a href="https://cds.cern.ch/search?f=author&p=Idzik%2C%20M.&ln=en">Idzik, M.</a> (AGH-UST, Cracow) ; <a href="https://cds.cern.ch/search?f=author&p=Moro%C5%84%2C%20J.&ln=en">Moroń, J.</a> (AGH-UST, Cracow) ; <a href="https://cds.cern.ch/search?f=author&p=%C5%9Awientek%2C%20K.P.&ln=en">Świentek, K.P.</a> (AGH-UST, Cracow) ; <a href="https://cds.cern.ch/search?f=author&p=Br%C3%BCckman%20de%20Renstrom%2C%20P.&ln=en">Brückman de Renstrom, P.</a> (Cracow, INP) ; <a href="https://cds.cern.ch/search?f=author&p=Krupa%2C%20B.&ln=en">Krupa, B.</a> (Cracow, INP) ; <a href="https://cds.cern.ch/search?f=author&p=Kucharczyk%2C%20M.&ln=en">Kucharczyk, M.</a> (Cracow, INP) ; <a href="https://cds.cern.ch/search?f=author&p=Lesiak%2C%20T.&ln=en">Lesiak, T.</a> (Cracow, INP) ; <a href="https://cds.cern.ch/search?f=author&p=Pawlik%2C%20B.&ln=en">Pawlik, B.</a> (Cracow, INP) ; <a href="https://cds.cern.ch/search?f=author&p=Sopicki%2C%20P.&ln=en">Sopicki, P.</a> (Cracow, INP) ; <a href="https://cds.cern.ch/search?f=author&p=Turbiarz%2C%20B.&ln=en">Turbiarz, B.</a> (Cracow, INP) ; <a href="https://cds.cern.ch/search?f=author&p=Wojto%C5%84%2C%20T.&ln=en">Wojtoń, T.</a> (Cracow, INP) ; <a href="https://cds.cern.ch/search?f=author&p=Zawiejski%2C%20L.K.&ln=en">Zawiejski, L.K.</a> (Cracow, INP) ; <a href="https://cds.cern.ch/search?f=author&p=Kalinowski%2C%20J.&ln=en">Kalinowski, J.</a> (Warsaw U.) ; <a href="https://cds.cern.ch/search?f=author&p=Nowak%2C%20K.&ln=en">Nowak, K.</a> (Warsaw U.) ; <a href="https://cds.cern.ch/search?f=author&p=%C5%BBarnecki%2C%20A.F.&ln=en">Żarnecki, A.F.</a> (Warsaw U.) ; <a href="https://cds.cern.ch/search?f=author&p=Firu%2C%20E.&ln=en">Firu, E.</a> (Bucharest, Inst. Space Science) ; <a href="https://cds.cern.ch/search?f=author&p=Ghenescu%2C%20V.&ln=en">Ghenescu, V.</a> (Bucharest, Inst. Space Science) ; <a href="https://cds.cern.ch/search?f=author&p=Neagu%2C%20A.T.&ln=en">Neagu, A.T.</a> (Bucharest, Inst. Space Science) ; <a href="https://cds.cern.ch/search?f=author&p=Preda%2C%20T.&ln=en">Preda, T.</a> (Bucharest, Inst. Space Science) ; <a href="https://cds.cern.ch/search?f=author&p=Zgura%2C%20I.S.&ln=en">Zgura, I.S.</a> (Bucharest, Inst. Space Science) ; <a href="https://cds.cern.ch/search?f=author&p=Aloev%2C%20A.&ln=en">Aloev, A.</a> (Dubna, JINR) ; <a href="https://cds.cern.ch/search?f=author&p=Azaryan%2C%20N.&ln=en">Azaryan, N.</a> (Dubna, JINR) ; <a href="https://cds.cern.ch/search?f=author&p=Boyko%2C%20I.&ln=en">Boyko, I.</a> (Dubna, JINR) ; <a href="https://cds.cern.ch/search?f=author&p=Budagov%2C%20J.&ln=en">Budagov, J.</a> (Dubna, JINR) ; <a href="https://cds.cern.ch/search?f=author&p=Chizhov%2C%20M.&ln=en">Chizhov, M.</a> (Dubna, JINR) ; <a href="https://cds.cern.ch/search?f=author&p=Filippova%2C%20M.&ln=en">Filippova, M.</a> (Dubna, JINR) ; <a href="https://cds.cern.ch/search?f=author&p=Glagolev%2C%20V.&ln=en">Glagolev, V.</a> (Dubna, JINR) ; <a href="https://cds.cern.ch/search?f=author&p=Gongadze%2C%20A.&ln=en">Gongadze, A.</a> (Dubna, JINR) ; <a href="https://cds.cern.ch/search?f=author&p=Grigoryan%2C%20S.&ln=en">Grigoryan, S.</a> (Dubna, JINR) ; <a href="https://cds.cern.ch/search?f=author&p=Gudkov%2C%20D.&ln=en">Gudkov, D.</a> (Dubna, JINR) ; <a href="https://cds.cern.ch/search?f=author&p=Karjavine%2C%20V.&ln=en">Karjavine, V.</a> (Dubna, JINR) ; <a href="https://cds.cern.ch/search?f=author&p=Lyablin%2C%20M.&ln=en">Lyablin, M.</a> (Dubna, JINR) ; <a href="https://cds.cern.ch/search?f=author&p=Nefedov%2C%20Yu.&ln=en">Nefedov, Yu.</a> (Dubna, JINR) ; <a href="https://cds.cern.ch/search?f=author&p=Olyunina%2C%20A.&ln=en">Olyunina, A.</a> (Dubna, JINR) ; <a href="https://cds.cern.ch/search?f=author&p=Rymbekova%2C%20A.&ln=en">Rymbekova, A.</a> (Dubna, JINR) ; <a href="https://cds.cern.ch/search?f=author&p=Samochkine%2C%20A.&ln=en">Samochkine, A.</a> (Dubna, JINR) ; <a href="https://cds.cern.ch/search?f=author&p=Sapronov%2C%20A.&ln=en">Sapronov, A.</a> (Dubna, JINR) ; <a href="https://cds.cern.ch/search?f=author&p=Shelkov%2C%20G.&ln=en">Shelkov, G.</a> (Dubna, JINR) ; <a href="https://cds.cern.ch/search?f=author&p=Shirkov%2C%20G.&ln=en">Shirkov, G.</a> (Dubna, JINR) ; <a href="https://cds.cern.ch/search?f=author&p=Soldatov%2C%20V.&ln=en">Soldatov, V.</a> (Dubna, JINR) ; <a href="https://cds.cern.ch/search?f=author&p=Solodko%2C%20E.&ln=en">Solodko, E.</a> (Dubna, JINR) ; <a href="https://cds.cern.ch/search?f=author&p=Trubnikov%2C%20G.&ln=en">Trubnikov, G.</a> (Dubna, JINR) ; <a href="https://cds.cern.ch/search?f=author&p=Tyapkin%2C%20I.&ln=en">Tyapkin, I.</a> (Dubna, JINR) ; <a href="https://cds.cern.ch/search?f=author&p=Uzhinsky%2C%20V.&ln=en">Uzhinsky, V.</a> (Dubna, JINR) ; <a href="https://cds.cern.ch/search?f=author&p=Vorozhtov%2C%20A.&ln=en">Vorozhtov, A.</a> (Dubna, JINR) ; <a href="https://cds.cern.ch/search?f=author&p=Zhemchugov%2C%20A.&ln=en">Zhemchugov, A.</a> (Dubna, JINR) ; <a href="https://cds.cern.ch/search?f=author&p=Levichev%2C%20E.&ln=en">Levichev, E.</a> (Novosibirsk, IYF) ; <a href="https://cds.cern.ch/search?f=author&p=Mezentsev%2C%20N.&ln=en">Mezentsev, N.</a> (Novosibirsk, IYF) ; <a href="https://cds.cern.ch/search?f=author&p=Piminov%2C%20P.&ln=en">Piminov, P.</a> (Novosibirsk, IYF) ; <a href="https://cds.cern.ch/search?f=author&p=Shatilov%2C%20D.&ln=en">Shatilov, D.</a> (Novosibirsk, IYF) ; <a href="https://cds.cern.ch/search?f=author&p=Vobly%2C%20P.&ln=en">Vobly, P.</a> (Novosibirsk, IYF) ; <a href="https://cds.cern.ch/search?f=author&p=Zolotarev%2C%20K.&ln=en">Zolotarev, K.</a> (Novosibirsk, IYF) ; <a href="https://cds.cern.ch/search?f=author&p=Bo%C5%BEovi%C4%87Jelisav%C4%8Di%C4%87%2C%20I.&ln=en">BožovićJelisavčić, I.</a> (VINCA Inst. Nucl. Sci., Belgrade) ; <a href="https://cds.cern.ch/search?f=author&p=Ka%C4%8Darevi%C4%87%2C%20G.&ln=en">Kačarević, G.</a> (VINCA Inst. Nucl. Sci., Belgrade) ; <a href="https://cds.cern.ch/search?f=author&p=Milutinovi%C4%87Dumbelovi%C4%87%2C%20G.&ln=en">MilutinovićDumbelović, G.</a> (VINCA Inst. Nucl. Sci., Belgrade) ; <a href="https://cds.cern.ch/search?f=author&p=Pandurovi%C4%87%2C%20M.&ln=en">Pandurović, M.</a> (VINCA Inst. Nucl. Sci., Belgrade) ; <a href="https://cds.cern.ch/search?f=author&p=Radulovi%C4%87%2C%20M.&ln=en">Radulović, M.</a> (VINCA Inst. Nucl. Sci., Belgrade) ; <a href="https://cds.cern.ch/search?f=author&p=Stevanovi%C4%87%2C%20J.&ln=en">Stevanović, J.</a> (VINCA Inst. Nucl. Sci., Belgrade) ; <a href="https://cds.cern.ch/search?f=author&p=Vukasinovi%C4%87%2C%20N.&ln=en">Vukasinović, N.</a> (VINCA Inst. Nucl. Sci., Belgrade) ; <a href="https://cds.cern.ch/search?f=author&p=Lee%2C%20D.-H.&ln=en">Lee, D.-H.</a> (Myong Ji U.) ; <a href="https://cds.cern.ch/search?f=author&p=Ayala%2C%20N.&ln=en">Ayala, N.</a> (ICE, Barcelona) ; <a href="https://cds.cern.ch/search?f=author&p=Benedetti%2C%20G.&ln=en">Benedetti, G.</a> (ICE, Barcelona) ; <a href="https://cds.cern.ch/search?f=author&p=Guenzel%2C%20T.&ln=en">Guenzel, T.</a> (ICE, Barcelona) ; <a href="https://cds.cern.ch/search?f=author&p=Iriso%2C%20U.&ln=en">Iriso, U.</a> (ICE, Barcelona) ; <a href="https://cds.cern.ch/search?f=author&p=Marti%2C%20Z.&ln=en">Marti, Z.</a> (ICE, Barcelona) ; <a href="https://cds.cern.ch/search?f=author&p=Perez%2C%20F.&ln=en">Perez, F.</a> (ICE, Barcelona) ; <a href="https://cds.cern.ch/search?f=author&p=Pont%2C%20M.&ln=en">Pont, M.</a> (ICE, Barcelona) ; <a href="https://cds.cern.ch/search?f=author&p=Trenado%2C%20J.&ln=en">Trenado, J.</a> (Barcelona U.) ; <a href="https://cds.cern.ch/search?f=author&p=Ruiz-Jimeno%2C%20A.&ln=en">Ruiz-Jimeno, A.</a> (Cantabria Inst. of Phys.) ; <a href="https://cds.cern.ch/search?f=author&p=Vila%2C%20I.&ln=en">Vila, I.</a> (Cantabria Inst. of Phys.) ; <a href="https://cds.cern.ch/search?f=author&p=Calero%2C%20J.&ln=en">Calero, J.</a> (Madrid, CIEMAT) ; <a href="https://cds.cern.ch/search?f=author&p=Dominguez%2C%20M.&ln=en">Dominguez, M.</a> (Madrid, CIEMAT) ; <a href="https://cds.cern.ch/search?f=author&p=Garcia-Tabares%2C%20L.&ln=en">Garcia-Tabares, L.</a> (Madrid, CIEMAT) ; <a href="https://cds.cern.ch/search?f=author&p=Gavela%2C%20D.&ln=en">Gavela, D.</a> (Madrid, CIEMAT) ; <a href="https://cds.cern.ch/search?f=author&p=Lopez%2C%20D.&ln=en">Lopez, D.</a> (Madrid, CIEMAT) ; <a href="https://cds.cern.ch/search?f=author&p=Toral%2C%20F.&ln=en">Toral, F.</a> (Madrid, CIEMAT) ; <a href="https://cds.cern.ch/search?f=author&p=Blanch%20Gutierrez%2C%20C.&ln=en">Blanch Gutierrez, C.</a> (Valencia U., IFIC) ; <a href="https://cds.cern.ch/search?f=author&p=Boronat%2C%20M.&ln=en">Boronat, M.</a> (Valencia U., IFIC) ; <a href="https://cds.cern.ch/search?f=author&p=Esperante%2C%20D.&ln=en">Esperante, D.</a> (Valencia U., IFIC) ; <a href="https://cds.cern.ch/search?f=author&p=Fullana%2C%20E.&ln=en">Fullana, E.</a> (Valencia U., IFIC) ; <a href="https://cds.cern.ch/search?f=author&p=Fuster%2C%20J.&ln=en">Fuster, J.</a> (Valencia U., IFIC) ; <a href="https://cds.cern.ch/search?f=author&p=Garc%C3%ADa%2C%20I.&ln=en">García, I.</a> (Valencia U., IFIC) ; <a href="https://cds.cern.ch/search?f=author&p=Gimeno%2C%20B.&ln=en">Gimeno, B.</a> (Valencia U., IFIC) ; <a href="https://cds.cern.ch/search?f=author&p=Gomis%20Lopez%2C%20P.&ln=en">Gomis Lopez, P.</a> (Valencia U., IFIC) ; <a href="https://cds.cern.ch/search?f=author&p=Gonz%C3%A1lez%2C%20D.&ln=en">González, D.</a> (Valencia U., IFIC) ; <a href="https://cds.cern.ch/search?f=author&p=Perell%C3%B3%2C%20M.&ln=en">Perelló, M.</a> (Valencia U., IFIC) ; <a href="https://cds.cern.ch/search?f=author&p=Ros%2C%20E.&ln=en">Ros, E.</a> (Valencia U., IFIC) ; <a href="https://cds.cern.ch/search?f=author&p=Villarejo%2C%20M.A.&ln=en">Villarejo, M.A.</a> (Valencia U., IFIC) ; <a href="https://cds.cern.ch/search?f=author&p=Vnuchenko%2C%20A.&ln=en">Vnuchenko, A.</a> (Valencia U., IFIC) ; <a href="https://cds.cern.ch/search?f=author&p=Vos%2C%20M.&ln=en">Vos, M.</a> (Valencia U., IFIC) ; <a href="https://cds.cern.ch/search?f=author&p=Borgmann%2C%20Ch.&ln=en">Borgmann, Ch.</a> (Uppsala U.) ; <a href="https://cds.cern.ch/search?f=author&p=Brenner%2C%20R.&ln=en">Brenner, R.</a> (Uppsala U.) ; <a href="https://cds.cern.ch/search?f=author&p=Ekel%C3%B6f%2C%20T.&ln=en">Ekelöf, T.</a> (Uppsala U.) ; <a href="https://cds.cern.ch/search?f=author&p=Jacewicz%2C%20M.&ln=en">Jacewicz, M.</a> (Uppsala U.) ; <a href="https://cds.cern.ch/search?f=author&p=Olveg%C3%A5rd%2C%20M.&ln=en">Olvegård, M.</a> (Uppsala U.) ; <a href="https://cds.cern.ch/search?f=author&p=Ruber%2C%20R.&ln=en">Ruber, R.</a> (Uppsala U.) ; <a href="https://cds.cern.ch/search?f=author&p=Ziemann%2C%20V.&ln=en">Ziemann, V.</a> (Uppsala U.) ; <a href="https://cds.cern.ch/search?f=author&p=Aguglia%2C%20D.&ln=en">Aguglia, D.</a> (CERN) ; <a href="https://cds.cern.ch/search?f=author&p=Alabau%20Gonzalvo%2C%20J.&ln=en">Alabau Gonzalvo, J.</a> (CERN) ; <a href="https://cds.cern.ch/search?f=author&p=Alcaide%20Leon%2C%20M.&ln=en">Alcaide Leon, M.</a> (CERN) ; <a href="https://cds.cern.ch/search?f=author&p=Alipour%20Tehrani%2C%20N.&ln=en">Alipour Tehrani, N.</a> (CERN) ; <a href="https://cds.cern.ch/search?f=author&p=Anastasopoulos%2C%20M.&ln=en">Anastasopoulos, M.</a> (CERN) ; <a href="https://cds.cern.ch/search?f=author&p=Andersson%2C%20A.&ln=en">Andersson, A.</a> (CERN) ; <a href="https://cds.cern.ch/search?f=author&p=Andrianala%2C%20F.&ln=en">Andrianala, F.</a> (CERN) ; <a href="https://cds.cern.ch/search?f=author&p=Antoniou%2C%20F.&ln=en">Antoniou, F.</a> (CERN) ; <a href="https://cds.cern.ch/search?f=author&p=Apyan%2C%20A.&ln=en">Apyan, A.</a> (CERN) ; <a href="https://cds.cern.ch/search?f=author&p=Arominski%2C%20D.&ln=en">Arominski, D.</a> (CERN) ; <a href="https://cds.cern.ch/search?f=author&p=Artoos%2C%20K.&ln=en">Artoos, K.</a> (CERN) ; <a href="https://cds.cern.ch/search?f=author&p=Assly%2C%20S.&ln=en">Assly, S.</a> (CERN) ; <a href="https://cds.cern.ch/search?f=author&p=Atieh%2C%20S.&ln=en">Atieh, S.</a> (CERN) ; <a href="https://cds.cern.ch/search?f=author&p=Baccigalupi%2C%20C.&ln=en">Baccigalupi, C.</a> (CERN) ; <a href="https://cds.cern.ch/search?f=author&p=Ballabriga%20Sune%2C%20R.&ln=en">Ballabriga Sune, R.</a> (CERN) ; <a href="https://cds.cern.ch/search?f=author&p=Banon%20Caballero%2C%20D.&ln=en">Banon Caballero, D.</a> (CERN) ; <a href="https://cds.cern.ch/search?f=author&p=Barnes%2C%20M.J.&ln=en">Barnes, M.J.</a> (CERN) ; <a href="https://cds.cern.ch/search?f=author&p=Barranco%20Garcia%2C%20J.&ln=en">Barranco Garcia, J.</a> (CERN) ; <a href="https://cds.cern.ch/search?f=author&p=Bartalesi%2C%20A.&ln=en">Bartalesi, A.</a> (CERN) ; <a href="https://cds.cern.ch/search?f=author&p=Bauche%2C%20J.&ln=en">Bauche, J.</a> (CERN) ; <a href="https://cds.cern.ch/search?f=author&p=Bayar%2C%20C.&ln=en">Bayar, C.</a> (CERN) ; <a href="https://cds.cern.ch/search?f=author&p=Belver-Aguilar%2C%20C.&ln=en">Belver-Aguilar, C.</a> (CERN) ; <a href="https://cds.cern.ch/search?f=author&p=Benot%20Morell%2C%20A.&ln=en">Benot Morell, A.</a> (CERN) ; <a href="https://cds.cern.ch/search?f=author&p=Bernardini%2C%20M.&ln=en">Bernardini, M.</a> (CERN) ; <a href="https://cds.cern.ch/search?f=author&p=Bett%2C%20D.R.&ln=en">Bett, D.R.</a> (CERN) ; <a href="https://cds.cern.ch/search?f=author&p=Bettoni%2C%20S.&ln=en">Bettoni, S.</a> (CERN) ; <a href="https://cds.cern.ch/search?f=author&p=Bettencourt%2C%20M.&ln=en">Bettencourt, M.</a> (CERN) ; <a href="https://cds.cern.ch/search?f=author&p=Bielawski%2C%20B.&ln=en">Bielawski, B.</a> (CERN) ; <a href="https://cds.cern.ch/search?f=author&p=Blanco%20Garcia%2C%20O.&ln=en">Blanco Garcia, O.</a> (CERN) ; <a href="https://cds.cern.ch/search?f=author&p=Blaskovic%20Kraljevic%2C%20N.&ln=en">Blaskovic Kraljevic, N.</a> (CERN) ; <a href="https://cds.cern.ch/search?f=author&p=Bolzon%2C%20B.&ln=en">Bolzon, B.</a> (CERN) ; <a href="https://cds.cern.ch/search?f=author&p=Bonnin%2C%20X.A.&ln=en">Bonnin, X.A.</a> (CERN) ; 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<a href="https://cds.cern.ch/search?f=author&p=Neilson%2C%20J.&ln=en">Neilson, J.</a> (SLAC) ; <a href="https://cds.cern.ch/search?f=author&p=Nosochkov%2C%20Y.&ln=en">Nosochkov, Y.</a> (SLAC) ; <a href="https://cds.cern.ch/search?f=author&p=Oriunno%2C%20M.&ln=en">Oriunno, M.</a> (SLAC) ; <a href="https://cds.cern.ch/search?f=author&p=Phinney%2C%20N.&ln=en">Phinney, N.</a> (SLAC) ; <a href="https://cds.cern.ch/search?f=author&p=Rizzo%2C%20T.&ln=en">Rizzo, T.</a> (SLAC) ; <a href="https://cds.cern.ch/search?f=author&p=Tantawi%2C%20S.&ln=en">Tantawi, S.</a> (SLAC) ; <a href="https://cds.cern.ch/search?f=author&p=Wang%2C%20J.&ln=en">Wang, J.</a> (SLAC) ; <a href="https://cds.cern.ch/search?f=author&p=Weatherford%2C%20B.&ln=en">Weatherford, B.</a> (SLAC) ; <a href="https://cds.cern.ch/search?f=author&p=White%2C%20G.&ln=en">White, G.</a> (SLAC) ; <a href="https://cds.cern.ch/search?f=author&p=Woodley%2C%20M.&ln=en">Woodley, M.</a> (SLAC)</p> <span id="extension"></span> <small><i><a id="link" href="#" onclick="toggle_authors_visibility()" style="color:rgb(204,0,0);"></a></i></small><script type="text/javascript">set_up()</script></td></tr> <tr><td class="formatRecordLabel"> Collaboration </td><td style="padding-left:5px;">CLICdp Collaboration ; CLIC Collaboration</td></tr> <tr><td class="formatRecordLabel"> Publication </td><td style="padding-left:5px;">2018-12-14 - 112.</td></tr> <tr><td class="formatRecordLabel"> Series </td><td style="padding-left:5px;">(<a href="/search?f=490__a&p=CERN%20Yellow%20Reports%3A%20Monographs">CERN Yellow Reports: Monographs</a> ; 2/2018)</td></tr> <tr><td class="formatRecordLabel"> In: </td><td style="padding-left:5px;"><a href="http://dx.doi.org/10.23731/CYRM-2018-002">10.23731/CYRM-2018-002</a></td></tr> <tr><td class="formatRecordLabel"> Subject code </td><td style="padding-left:5px;"><a href="/search?f=080__a&p=621.384">621.384</a></td></tr> <tr><td class="formatRecordLabel"> Subject category </td><td style="padding-left:5px;">physics.acc-ph ; Accelerators and Storage Rings</td></tr> <tr><td class="formatRecordLabel"> Accelerator/Facility, Experiment </td><td style="padding-left:5px;"><a href="https://cds.cern.ch/search?p=CLICdp&f=693__e">CLICdp</a></td></tr> <tr><td class="formatRecordLabel"> Abstract </td><td style="padding-left:5px;">The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^−$ collider under development at CERN. Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25–30 years.</td></tr> <tr><td class="formatRecordLabel"> ISBN </td><td style="padding-left:5px;">9789290835066 (print version, paperback)<br/>9789290835073 (electronic version)<br/></td></tr> <tr><td class="formatRecordLabel"> DOI </td><td style="padding-left:5px;">Publication: <a href="http://dx.doi.org/10.23731/CYRM-2018-002" title="DOI" target="_blank">10.23731/CYRM-2018-002</a> <tr><td class="formatRecordLabel"> Copyright/License </td><td style="padding-left:5px;">publication: © 2018-2025 CERN (License: <a href="http://creativecommons.org/licenses/by/4.0/">CC-BY-4.0</a>)<br/>preprint: (License: <a href="http://creativecommons.org/licenses/by/4.0/">CC-BY-4.0</a>)</td></tr> </table> <br/>Corresponding record in: <a href="http://inspirehep.net/record/1709232">Inspire</a> <div style="box-sizing: inherit;position: relative;min-height: 1em;margin: 1em 10px;background: #f8f8f9;padding: 1em 1.5em;line-height: 1.4285em;transition: opacity .1s ease,color .1s ease,background .1s ease,box-shadow .1s ease,-webkit-box-shadow .1s ease;border-radius: .28571429rem;font-size: 1.1em;background-color: #f8ffff;color: #276f86;box-shadow: 0 0 0 1px #a9d5de inset,0 0 0 0 transparent;"> <i class="fa fa-info"></i><span style="padding-left: 9px;"> To loan this literature, see Library holdings in the <a style="font-weight: bold; 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Following the CLIC conceptual design published in 2012, this report provides an overview of the CLIC project, its current status, and future developments. It presents the CLIC physics potential and reports on design, technology, and implementation aspects of the accelerator and the detector. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV, respectively, for a site length ranging from 11 km to 50 km. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12 GHz accelerating structures are powered via a high-current drive beam. For the first stage, an alternative with X-band klystron powering is also considered. CLIC accelerator optimisation, technical developments and system tests have resulted in significant progress in recent years. Moreover, this has led to an increased energy efficiency (power around 170 MW) for the 380 GeV stage, together with a reduced cost estimate at the level of 6 billion CHF. The detector concept, which matches the physics performance requirements and the CLIC experimental conditions, has been refined using improved software tools for simulation and reconstruction. Significant progress has been made on detector technology developments for the tracking and calorimetry systems. A wide range of CLIC physics studies has been conducted, both through full detector simulations with overlay of beam-induced backgrounds, and through parametric studies, together providing a broad overview of the CLIC physics potential. Each of the three energy stages adds cornerstones of the full CLIC physics programme, such as Higgs width and couplings, top-quark properties, Higgs self-coupling, direct searches, and many precision electroweak measurements. The interpretation of the combined results gives crucial and accurate insight into new physics, largely complementary to LHC and HL-LHC. The construction of the first CLIC energy stage could start by 2026. First beams would be available by 2035, marking the beginning of a broad CLIC physics programme spanning 25\u201330 years." }); // ]]> </script>  </div> </div> <div style="clear:both;margin-bottom: 0;"></div> </div> <div class="bottom-left"></div><div class="bottom-right"></div> </div> </div></div> <footer id="footer" class="pagefooter clearfix">  <div class="pagefooterstripeleft"> CERN Document Server :: <a class="footer" href="https://cds.cern.ch/?ln=en">Search</a> :: <a class="footer" href="https://cds.cern.ch/submit?ln=en">Submit</a> :: <a class="footer" href="https://cds.cern.ch/youraccount/display?ln=en">Personalize</a> :: <a class="footer" href="https://cds.cern.ch/help/?ln=en">Help</a> :: <a class="footer" href="https://cern.service-now.com/service-portal?id=privacy_policy&se=CDS-Service" target="_blank">Privacy Notice</a> :: <a class="footer" href="https://repository.cern/content-policy" target="_blank">Content Policy</a> :: <a class="footer" href="https://repository.cern/terms" target="_blank">Terms and Conditions</a> <br /> Powered by <a class="footer" href="http://invenio-software.org/">Invenio</a> <br /> Maintained by <a class="footer" href="https://cern.service-now.com/service-portal?id=service_element&name=CDS-Service">CDS Service</a> - Need help? 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