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navbar-expand-md breadcrumb-bar pb-3 order-2 order-md-2"> <div class="container-fluid container-fluid-max-xl"> <div class="portlet-boundary portlet-boundary_com_liferay_site_navigation_breadcrumb_web_portlet_SiteNavigationBreadcrumbPortlet_ portlet-static portlet-static-end portlet-barebone portlet-breadcrumb " id="p_p_id_com_liferay_site_navigation_breadcrumb_web_portlet_SiteNavigationBreadcrumbPortlet_"> <span id="p_com_liferay_site_navigation_breadcrumb_web_portlet_SiteNavigationBreadcrumbPortlet"></span> <section class="portlet" id="portlet_com_liferay_site_navigation_breadcrumb_web_portlet_SiteNavigationBreadcrumbPortlet"> <div class="portlet-content"> <div class=" portlet-content-container"> <div class="portlet-body"> <nav aria-label="Breadcrumb" id="_com_liferay_site_navigation_breadcrumb_web_portlet_SiteNavigationBreadcrumbPortlet_breadcrumbs-defaultScreen"> <ol class="breadcrumb"> <li class="breadcrumb-item"> <a class="breadcrumb-link" > <span class="breadcrumb-text-truncate">Experimentos de neutrinos</span> </a> </li> <li class="breadcrumb-item"> <a class="breadcrumb-link" href="https://neutrinos.portales.ciemat.es/en/projects" > <span class="breadcrumb-text-truncate">Projects</span> </a> </li> <li class="breadcrumb-item"> <span class="active breadcrumb-text-truncate">Double Chooz</span> </li> </ol> </nav> </div> </div> </div> </section> </div> </div> </div> </header> <section class="container flex-fill" id="content"> <h2 class="sr-only" role="heading" aria-level="1">Double Chooz - Experimentos de neutrinos</h2> <style type="text/css"> .master-layout-fragment .portlet-header { display: none; } </style> <div class="columns-1-2-1" id="main-content" role="main"> <div class="portlet-layout row"> <div class="col-md-12 portlet-column portlet-column-only" id="column-1"> <div class="portlet-dropzone portlet-column-content portlet-column-content-only" id="layout-column_column-1"> <div class="portlet-boundary 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data-analytics-asset-title="Double Chooz" data-analytics-asset-type="web-content"> <style> ol > li { font-size: 13px !important; line-height: 21px; font-weight: 400; margin-bottom:7px; color: #777!important; text-align: justify!important; } </style> <script> $(function() { $("#accordion2096062").accordion({ autoHeight: false, navigation: true, heightStyle: "content" }); }); </script> <div class="ev-content-container"> <h1> <span>Double Chooz Experiment</span> </h1> <div class="hr hr-short hr-center avia-builder-el-10 el_after_av_textblock el_before_av_textblock"> <span class="hr-inner"> <span class="hr-inner-style"></span> </span> </div> <p> <p dir="ltr" style="text-align: justify;"><span id="docs-internal-guid-4cf4cfef-7fff-6495-30cf-7d14c41d5885">The </span>Double Chooz (DC) experiment was located at the Chooz nuclear power plant in France and took data between 2011 and 2018, and the data analysis is still going on. The DC far detector (FD) was placed at 1050 m away from the cores, close to the maximal oscillation distance. A second, almost identical detector, called near detector (ND) was installed 400 m away from the reactor cores. This multi-detector setup allowed to drastically reduce the systematic errors mainly associated with the neutrino flux and provide a precise value of the neutrino mixing angle θ13. </p> <p dir="ltr" style="text-align: center;"> </p> <p dir="ltr" style="text-align: center;"><span id="docs-internal-guid-4cf4cfef-7fff-6495-30cf-7d14c41d5885"><img height="421" src="https://lh4.googleusercontent.com/Jvxp66g3_MhEH851oVTAOUvYHP7po7CD-Qa8LVNCdSrpkilLzECyCicmGwMhWl8su7BOggyFyXD9989BKpbUIv2nAQI41bm2uL5BKAceEo2gICaTCKWQUjgq8oPk7hE7aqROnsmyE6MWeDEyyg" style="height:auto;vertical-align:middle;border:0px;margin-top:0px;" width="602" /></span></p> <p dir="ltr" style="text-align: justify;"><span id="docs-internal-guid-4cf4cfef-7fff-6495-30cf-7d14c41d5885">The CIEMAT neutrino experimental physics group has been an active member of the Double Chooz collaboration since 2006. The CIEMAT group contributed extensively in the hardware and construction of the detector as well as in the physics data analysis.</span></p> <p dir="ltr" style="text-align: center;"><span id="docs-internal-guid-4cf4cfef-7fff-6495-30cf-7d14c41d5885"><img height="401" src="https://lh3.googleusercontent.com/UGSYl3SuGKqqkXsmGPcH96ItAcGs7UufncCc3iyIbDL9wM0tdj5IRsL3G0kBMA0u6szh5kSTqsHMjrkLrGyiq_qReB64qkJdgEuT_T51Q5vreFQQK2Wer5-XGdgQAHeWZBe_J8mcWTEREV83Xg" style="height:auto;vertical-align:middle;border:0px;margin-top:0px;" width="602" /></span></p> <p dir="ltr" style="text-align: justify;"><span id="docs-internal-guid-4cf4cfef-7fff-6495-30cf-7d14c41d5885">The main contributions and responsibilities of our group in the Double Chooz detectors were:</span></p> <ul style="list-style-type:disc;"> <li role="presentation"><span id="docs-internal-guid-4cf4cfef-7fff-6495-30cf-7d14c41d5885">Design, manufacture, assembly and installation of the 800 mechanical supports for the 10" photomultipliers (PMTs) of the near and far detectors</span></li> <li role="presentation"><span id="docs-internal-guid-4cf4cfef-7fff-6495-30cf-7d14c41d5885">Design, manufacture and assembly of the 800 magnetic shields for the PMTs</span></li> <li role="presentation"><span id="docs-internal-guid-4cf4cfef-7fff-6495-30cf-7d14c41d5885">Design, manufacture and installation of 800 HV splitters and high voltage cables</span></li> <li role="presentation"><span id="docs-internal-guid-4cf4cfef-7fff-6495-30cf-7d14c41d5885">Installation of the PMTs inside the tanks of the far and near detectors</span></li> <li role="presentation"><span id="docs-internal-guid-4cf4cfef-7fff-6495-30cf-7d14c41d5885">Study of the emission of light from the base of the PMTs</span></li> </ul> <p dir="ltr" style="text-align: justify;"><span id="docs-internal-guid-4cf4cfef-7fff-6495-30cf-7d14c41d5885">The CIEMAT neutrino group contributed very significantly to the data analysis of the two detectors. We were responsible for the measurement of the remaining background due to accidental coincidences in the detector. For the analysis channel that includes the neutron captures on H, this background is the most important one in the FD and is the main background below 2 MeV for both detectors, where the oscillation is maximum. The CIEMAT group was in charge of the determination of the neutron detection efficiency for both detectors, which is the dominant systematic uncertainty in the detection of electron antineutrinos through the inverse β-decay reaction in DC, limiting the precision of the measurement of the neutrino mixing angle θ13. A second independent measurement of θ</span>13 was performed by DC using a different analysis technique led by the CIEMAT group: the reactor rate modulation (RRM) analysis. The rate of neutrino candidates is measured during periods of different reactor power ranging from zero power to full power. This analysis allowed the measurement of θ13 without an a priori knowledge of the background.</p> <p dir="ltr"><span id="docs-internal-guid-4cf4cfef-7fff-6495-30cf-7d14c41d5885">Publications with significant contributions from the CIEMAT group:</span></p> <ul style="list-style-type:disc;"> <li role="presentation"><span id="docs-internal-guid-4cf4cfef-7fff-6495-30cf-7d14c41d5885"><a href="https://arxiv.org/abs/2201.13285">The Double Chooz antineutrino detectors, Double Chooz Collaboration</a></span>, (H. De Kerret et al.), <span style="color: rgb(119, 119, 119);">EPJC 82 (2022) 804.</span></li> <li role="presentation"><span id="docs-internal-guid-4cf4cfef-7fff-6495-30cf-7d14c41d5885"><a href="https://link.springer.com/article/10.1007/JHEP01(2021)190">Reactor Rate Modulation oscillation analysis with two detectors in Double Chooz</a></span>, Double Chooz Collaboration (Abrahao, T. et al.), JHEP 01 (2021) 190.</li> <li role="presentation"><span id="docs-internal-guid-4cf4cfef-7fff-6495-30cf-7d14c41d5885"><a href="https://www.nature.com/articles/s41567-020-0831-y">Double Chooz theta13 measurement via total neutron capture detection</a></span>, Double Chooz Collaboration (H. Kerret et al.) Nature Physics 16 (2020) 558.</li> <li role="presentation"><span id="docs-internal-guid-4cf4cfef-7fff-6495-30cf-7d14c41d5885"><a href="http://iopscience.iop.org/article/10.1088/1748-0221/11/08/P08001">Characterization of the spontaneous light emission of the PMTs used in the Double Chooz experiment</a></span>, Double Chooz Collaboration (Y. Abe et al.), JINST 11 (2016) P08001</li> <li role="presentation"><span id="docs-internal-guid-4cf4cfef-7fff-6495-30cf-7d14c41d5885"><a href="https://link.springer.com/article/10.1007%2FJHEP01%282016%29163">Measurement of theta13 in Double Chooz using neutron captures on hydrogen with novel background rejection techniques</a></span>, Double Chooz Collaboration (Y. Abe et al.), JHEP 1601 (2016) 163</li> <li role="presentation"><span id="docs-internal-guid-4cf4cfef-7fff-6495-30cf-7d14c41d5885"><a href="https://www.sciencedirect.com/science/article/pii/S0370269314002858?via%3Dihub">Background independent measurement of theta13 in Double Chooz</a></span>, Double Chooz Collaboration (Y. Abe et al.), Phys. Lett. B 735 (2014) 51-56.</li> <li role="presentation"><span id="docs-internal-guid-4cf4cfef-7fff-6495-30cf-7d14c41d5885"><a href="https://link.springer.com/article/10.1007%2FJHEP10%282014%29086">Improved measurements of the neutrino mixing angle theta13 with the Double Chooz detector</a></span>, Double Chooz Collaboration (Y. Abe et al.), JHEP 10 (2014) 086.</li> <li role="presentation"><span id="docs-internal-guid-4cf4cfef-7fff-6495-30cf-7d14c41d5885"><a href="https://journals.aps.org/prd/abstract/10.1103/PhysRevD.86.052008">Reactor electron antineutrino disappearance in the Double Chooz experiment</a></span>, Double Chooz Collaboration (Y. Abe et al.), Phys.Rev.D 86 (2012) 052008</li> <li role="presentation"><span id="docs-internal-guid-4cf4cfef-7fff-6495-30cf-7d14c41d5885"><a href="https://journals.aps.org/prl/abstract/10.1103/PhysRevLett.108.131801">Indication of Reactor \bar{\nu}_e Disappearance in the Double Chooz Experiment</a></span>, Double Chooz Collaboration (Y. Abe et al.), Phys.Rev.Lett. 108 (2012) 131801</li> <li role="presentation"><span id="docs-internal-guid-4cf4cfef-7fff-6495-30cf-7d14c41d5885"><a href="https://www.sciencedirect.com/science/article/pii/S016890021001199X?via%3Dihub">Characterization of large area photomutipliers under low magnetic fields: Design and performances of the magnetic shielding for the Double Chooz neutrino experiment</a></span>, E. Calvo, M. Cerrada, C. Fernández-Bedoya, I. Gil-Botella, C. Palomares, I. Rodríguez, F. Toral, A. 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