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Vincenzo Pierro | Università degli Studi del Sannio - Academia.edu
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class="user-summary-container"><div class="social-profile-avatar-container"><img class="profile-avatar u-positionAbsolute" alt="Vincenzo Pierro" border="0" onerror="if (this.src != '//a.academia-assets.com/images/s200_no_pic.png') this.src = '//a.academia-assets.com/images/s200_no_pic.png';" width="200" height="200" src="https://0.academia-photos.com/32700082/101687794/90846847/s200_vincenzo.pierro.jpeg" /></div><div class="title-container"><h1 class="ds2-5-heading-sans-serif-sm">Vincenzo Pierro</h1><div class="affiliations-container fake-truncate js-profile-affiliations"><div><a class="u-tcGrayDarker" href="https://unisannio.academia.edu/">Università degli Studi del Sannio</a>, <a class="u-tcGrayDarker" href="https://unisannio.academia.edu/Departments/Department_of_Engineering/Documents">Department of Engineering</a>, <span class="u-tcGrayDarker">Faculty Member</span></div></div></div></div><div class="sidebar-cta-container"><button class="ds2-5-button hidden profile-cta-button grow 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class="u-taCenter"></div><div class="profile--tab_content_container js-tab-pane tab-pane active" id="all"><div class="profile--tab_heading_container js-section-heading" data-section="Papers" id="Papers"><h3 class="profile--tab_heading_container">Papers by Vincenzo Pierro</h3></div><div class="js-work-strip profile--work_container" data-work-id="105869624"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/105869624/Sequential_nonideal_measurements_of_quantum_oscillators_Statistical_characterization_with_and_without_environmental_coupling"><img alt="Research paper thumbnail of Sequential nonideal measurements of quantum oscillators: Statistical characterization with and without environmental coupling" class="work-thumbnail" src="https://attachments.academia-assets.com/105219238/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/105869624/Sequential_nonideal_measurements_of_quantum_oscillators_Statistical_characterization_with_and_without_environmental_coupling">Sequential nonideal measurements of quantum oscillators: Statistical characterization with and without environmental coupling</a></div><div class="wp-workCard_item"><span>Physical Review A</span><span>, 2015</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="2d6ddf4e8b972a690412a536fd5c66f6" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":105219238,"asset_id":105869624,"asset_type":"Work","button_location":"profile"}" 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})(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "2d6ddf4e8b972a690412a536fd5c66f6" } } $('.js-work-strip[data-work-id=105869624]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":105869624,"title":"Sequential nonideal measurements of quantum oscillators: Statistical characterization with and without environmental coupling","translated_title":"","metadata":{"publisher":"American Physical Society (APS)","grobid_abstract":"A one-dimensional quantum oscillator is monitored by taking repeated position measurements. As a first contribution, it is shown that, under a quantum nondemolition measurement scheme applied to a system initially at the ground state: i) the observed sequence of measurements (quantum tracks) corresponding to a single experiment converges to a limit point, and that ii) the limit point is random over the ensemble of the experiments, being distributed as a zero-mean Gaussian random variable with a variance at most equal to the ground state variance. As a second contribution, the richer scenario where the oscillator is coupled with a frozen (i.e., at the ground state) ensemble of independent quantum oscillators. A sharply different behavior emerges: under the same measurement scheme, here we observe that the measurement sequences are essentially divergent. Such a rigorous statistical analysis of the sequential measurement process might be useful for characterizing the main quantities that are currently used for inference, manipulation and monitoring of many quantum systems. Several interesting properties of the quantum tracks evolution, as well as of the associated (quantum) threshold crossing times are discussed, and the dependence upon the main system parameters (e.g., the choice of the measurement sampling time, the degree of interaction with the environment, the measurement device accuracy) are elucidated. At a more fundamental level, it is seen that, as an application of basic Quantum Mechanics principles, a sharp difference exists between the intrinsic randomness unavoidably present in any quantum system, and the extrinsic randomness arising from the environmental coupling, i.e., the randomness induced by an external source of disturbance.","publication_date":{"day":null,"month":null,"year":2015,"errors":{}},"publication_name":"Physical Review A","grobid_abstract_attachment_id":105219238},"translated_abstract":null,"internal_url":"https://www.academia.edu/105869624/Sequential_nonideal_measurements_of_quantum_oscillators_Statistical_characterization_with_and_without_environmental_coupling","translated_internal_url":"","created_at":"2023-08-22T23:31:10.850-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":32700082,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[{"id":105219238,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/105219238/thumbnails/1.jpg","file_name":"1511.03849v1.pdf","download_url":"https://www.academia.edu/attachments/105219238/download_file?st=MTczMjgwMjYzMCw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Sequential_nonideal_measurements_of_quan.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/105219238/1511.03849v1-libre.pdf?1692772556=\u0026response-content-disposition=attachment%3B+filename%3DSequential_nonideal_measurements_of_quan.pdf\u0026Expires=1732777820\u0026Signature=IlOtcVTUiLo0umfsg59fIovFmsYgs9YizOLTbtr7y8r3R-Yh~50WrS4Qaf7ZqFwgWUGK5Pv4gDPic6qQiHaM9AZMLK6uN3ldON8Gr9iYyV511R6P9U-Wq9RAFn79f1YlqYm6lkSmCRQjn8uw8iCiuRqQlhUOMKH9SoAd-tRrkve7peKjaI-39Pjt9SLBpBEKWeAYZ-3pPV5I7u1jluu3E~1FaHj0k10e0MBfpH5x5Arp8FgwMJ5H1EsI4R4xzh2cKUpY7RzUGblFjunpwQ14nGeEqauu7qJbHhaKpKI1nq7d1TAHCQNPuc56jvGrVnnTJyvV6N0x8NKhnvhMheXQSg__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"Sequential_nonideal_measurements_of_quantum_oscillators_Statistical_characterization_with_and_without_environmental_coupling","translated_slug":"","page_count":18,"language":"en","content_type":"Work","owner":{"id":32700082,"first_name":"Vincenzo","middle_initials":null,"last_name":"Pierro","page_name":"VincenzoPierro","domain_name":"unisannio","created_at":"2015-07-01T06:11:32.248-07:00","display_name":"Vincenzo Pierro","url":"https://unisannio.academia.edu/VincenzoPierro"},"attachments":[{"id":105219238,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/105219238/thumbnails/1.jpg","file_name":"1511.03849v1.pdf","download_url":"https://www.academia.edu/attachments/105219238/download_file?st=MTczMjgwMjYzMCw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Sequential_nonideal_measurements_of_quan.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/105219238/1511.03849v1-libre.pdf?1692772556=\u0026response-content-disposition=attachment%3B+filename%3DSequential_nonideal_measurements_of_quan.pdf\u0026Expires=1732777820\u0026Signature=IlOtcVTUiLo0umfsg59fIovFmsYgs9YizOLTbtr7y8r3R-Yh~50WrS4Qaf7ZqFwgWUGK5Pv4gDPic6qQiHaM9AZMLK6uN3ldON8Gr9iYyV511R6P9U-Wq9RAFn79f1YlqYm6lkSmCRQjn8uw8iCiuRqQlhUOMKH9SoAd-tRrkve7peKjaI-39Pjt9SLBpBEKWeAYZ-3pPV5I7u1jluu3E~1FaHj0k10e0MBfpH5x5Arp8FgwMJ5H1EsI4R4xzh2cKUpY7RzUGblFjunpwQ14nGeEqauu7qJbHhaKpKI1nq7d1TAHCQNPuc56jvGrVnnTJyvV6N0x8NKhnvhMheXQSg__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":498,"name":"Physics","url":"https://www.academia.edu/Documents/in/Physics"},{"id":16460,"name":"Statistical Physics","url":"https://www.academia.edu/Documents/in/Statistical_Physics"},{"id":69262,"name":"Quantum","url":"https://www.academia.edu/Documents/in/Quantum"},{"id":80414,"name":"Mathematical Sciences","url":"https://www.academia.edu/Documents/in/Mathematical_Sciences"},{"id":118582,"name":"Physical sciences","url":"https://www.academia.edu/Documents/in/Physical_sciences"},{"id":129087,"name":"Randomness","url":"https://www.academia.edu/Documents/in/Randomness"},{"id":260118,"name":"CHEMICAL SCIENCES","url":"https://www.academia.edu/Documents/in/CHEMICAL_SCIENCES"},{"id":1007970,"name":"Quantum Process","url":"https://www.academia.edu/Documents/in/Quantum_Process"}],"urls":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="98516826"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/98516826/Meta_Heuristics_Optimization_of_Mirrors_for_Gravitational_Wave_Detectors_Cryogenic_Case"><img alt="Research paper thumbnail of Meta-Heuristics Optimization of Mirrors for Gravitational Wave Detectors: Cryogenic Case" class="work-thumbnail" src="https://attachments.academia-assets.com/99845460/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/98516826/Meta_Heuristics_Optimization_of_Mirrors_for_Gravitational_Wave_Detectors_Cryogenic_Case">Meta-Heuristics Optimization of Mirrors for Gravitational Wave Detectors: Cryogenic Case</a></div><div class="wp-workCard_item"><span>Applied Sciences</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">In this paper, we explore the behavior of several optimization methods for reducing coating Brown...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">In this paper, we explore the behavior of several optimization methods for reducing coating Brownian noise in the mirrors of gravitational wave detectors. We will refer to cryogenic operating temperatures, where the low refractive index material has mechanical losses higher than those of the high refractive index material. This situation is the exact opposite of that which occurs at room temperature, which is already widely known. The optimal design of the dielectric mirror (without a priori assumptions on thicknesses) can be obtained through the combined multi-objective optimization of transmittance and thermal noise. In the following, we apply several multi-objective meta-heuristics to compute the Pareto front related to the optimization problem of dielectric mirror thicknesses made of two materials (binary coatings). This approach gives us more certainty about the structure of the final result. We find strong evidence that all meta-heuristics converge to the same solution. The fi...</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="13433e24dd5734985ee5c8d060013a01" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":99845460,"asset_id":98516826,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/99845460/download_file?st=MTczMjgwMjYzMCw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="98516826"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="98516826"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 98516826; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=98516826]").text(description); $(".js-view-count[data-work-id=98516826]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 98516826; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='98516826']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 98516826, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "13433e24dd5734985ee5c8d060013a01" } } $('.js-work-strip[data-work-id=98516826]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":98516826,"title":"Meta-Heuristics Optimization of Mirrors for Gravitational Wave Detectors: Cryogenic Case","translated_title":"","metadata":{"abstract":"In this paper, we explore the behavior of several optimization methods for reducing coating Brownian noise in the mirrors of gravitational wave detectors. We will refer to cryogenic operating temperatures, where the low refractive index material has mechanical losses higher than those of the high refractive index material. This situation is the exact opposite of that which occurs at room temperature, which is already widely known. The optimal design of the dielectric mirror (without a priori assumptions on thicknesses) can be obtained through the combined multi-objective optimization of transmittance and thermal noise. In the following, we apply several multi-objective meta-heuristics to compute the Pareto front related to the optimization problem of dielectric mirror thicknesses made of two materials (binary coatings). This approach gives us more certainty about the structure of the final result. We find strong evidence that all meta-heuristics converge to the same solution. The fi...","publisher":"MDPI AG","publication_name":"Applied Sciences"},"translated_abstract":"In this paper, we explore the behavior of several optimization methods for reducing coating Brownian noise in the mirrors of gravitational wave detectors. We will refer to cryogenic operating temperatures, where the low refractive index material has mechanical losses higher than those of the high refractive index material. This situation is the exact opposite of that which occurs at room temperature, which is already widely known. The optimal design of the dielectric mirror (without a priori assumptions on thicknesses) can be obtained through the combined multi-objective optimization of transmittance and thermal noise. In the following, we apply several multi-objective meta-heuristics to compute the Pareto front related to the optimization problem of dielectric mirror thicknesses made of two materials (binary coatings). This approach gives us more certainty about the structure of the final result. We find strong evidence that all meta-heuristics converge to the same solution. 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We carry out the searches in the LIGO data from the first six months of the third Advanced LIGO and Virgo observing run using the Weave semi-coherent method, which sums matched-filter detection-statistic values over many time segments spanning the observation period. No gravitational wave signal is detected in the search band of 20-976 Hz for assumed source ages greater than 300 years for Cas A and greater than 700 years for Vela Jr. Estimates from simulated continuous wave signals indicate we achieve the most sensitive results to date across the explored parameter space volume, probing to strain magnitudes as low as ∼6.3 × 10 −26 for Cas A and ∼5.6 × 10 −26 for Vela Jr. at frequencies near 166 Hz at 95% efficiency.","publication_name":"Physical Review 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href="https://www.academia.edu/98516823/Identification_and_mitigation_of_narrow_spectral_artifacts_that_degrade_searches_for_persistent_gravitational_waves_in_the_first_two_observing_runs_of_Advanced_LIGO"><img alt="Research paper thumbnail of Identification and mitigation of narrow spectral artifacts that degrade searches for persistent gravitational waves in the first two observing runs of Advanced LIGO" class="work-thumbnail" src="https://attachments.academia-assets.com/99845464/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/98516823/Identification_and_mitigation_of_narrow_spectral_artifacts_that_degrade_searches_for_persistent_gravitational_waves_in_the_first_two_observing_runs_of_Advanced_LIGO">Identification and mitigation of narrow spectral artifacts that degrade searches for persistent gravitational waves in the first two observing runs of Advanced LIGO</a></div><div class="wp-workCard_item"><span>Physical Review D</span><span>, 2018</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="e2ce3770306a56537013ebec7c6dfc98" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":99845464,"asset_id":98516823,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/99845464/download_file?st=MTczMjgwMjYzMCw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="98516823"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i 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$(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="91767452"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/91767452/Negative_differential_resistance_in_Josephson_junctions_coupled_to_a_cavity"><img alt="Research paper thumbnail of Negative differential resistance in Josephson junctions coupled to a cavity" class="work-thumbnail" src="https://attachments.academia-assets.com/94960623/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/91767452/Negative_differential_resistance_in_Josephson_junctions_coupled_to_a_cavity">Negative differential resistance in Josephson junctions coupled to a cavity</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Regions with negative differential resistance can arise in the IV curve of Josephson junctions an...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Regions with negative differential resistance can arise in the IV curve of Josephson junctions and this phenomenon plays an essential role for applications, in particular for THz radiation emission. For the measurement of high frequency radiation from Josephson junctions, a cavity-either internal or externalis often used. A cavity may also induce a negative differential resistance region at the lower side of the resonance frequency. We investigate the dynamics of Josephson junctions with a negative differential resistance in the quasi particle tunnel current, i.e. in the McCumber curve. We find that very complicated and unexpected interactions take place. This may be useful for the interpretation of experimental measurements of THz radiation from intrinsic Josephson junctions.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="9c76f0f2ce3472d14803e0db65e26b19" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":94960623,"asset_id":91767452,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/94960623/download_file?st=MTczMjgwMjYzMCw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="91767452"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="91767452"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 91767452; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=91767452]").text(description); $(".js-view-count[data-work-id=91767452]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 91767452; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='91767452']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 91767452, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "9c76f0f2ce3472d14803e0db65e26b19" } } $('.js-work-strip[data-work-id=91767452]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":91767452,"title":"Negative differential resistance in Josephson junctions coupled to a cavity","translated_title":"","metadata":{"doi":"10.1016/j.physc.2014.02.025","abstract":"Regions with negative differential resistance can arise in the IV curve of Josephson junctions and this phenomenon plays an essential role for applications, in particular for THz radiation emission. 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$(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="88357389"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/88357389/Bimodal_Approach_for_Noise_Figures_of_Merit_Evaluation_in_Quantum_Limited_Josephson_Traveling_Wave_Parametric_Amplifiers"><img alt="Research paper thumbnail of Bimodal Approach for Noise Figures of Merit Evaluation in Quantum-Limited Josephson Traveling Wave Parametric Amplifiers" class="work-thumbnail" src="https://attachments.academia-assets.com/92345177/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/88357389/Bimodal_Approach_for_Noise_Figures_of_Merit_Evaluation_in_Quantum_Limited_Josephson_Traveling_Wave_Parametric_Amplifiers">Bimodal Approach for Noise Figures of Merit Evaluation in Quantum-Limited Josephson Traveling Wave Parametric Amplifiers</a></div><div class="wp-workCard_item"><span>IEEE Transactions on Applied Superconductivity</span><span>, 2022</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="955f5b73e0d48629e0731f3d3d60ce59" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":92345177,"asset_id":88357389,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/92345177/download_file?st=MTczMjgwMjYzMCw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="88357389"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="88357389"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 88357389; 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Exploiting a theoretical bimodal description of a linear phase-preserving amplifier, in this contribution we analyze some of the intrinsic properties of a model architecture (i.e., an rf-SQUID based Josephson Traveling Wave Parametric Amplifier) in terms of amplification and noise generation for key case study input states (Fock and coherent). 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class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/88357385/Development_of_Quantum_Limited_Superconducting_Amplifiers_for_Advanced_Detection">Development of Quantum Limited Superconducting Amplifiers for Advanced Detection</a></div><div class="wp-workCard_item"><span>IEEE Transactions on Applied Superconductivity</span><span>, 2022</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Ultralow-noise microwave amplification and detection play a central role in different application...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Ultralow-noise microwave amplification and detection play a central role in different applications, going from fundamental physics experiments to the deployment of quantum technologies. In many applications the necessity of reading multiple detectors, or cavities or qubits, calls for large bandwidth amplifiers with the lowest possible noise. Current technologies are based on High Electron Mobility Transistors and Josephson Parametric Amplifiers. Both have limitations, the former in terms of the minimum noise, the latter in terms of bandwidth. Superconducting Traveling Wave Parametric Amplifiers (TWPAs) have the potential of offering quantum limited noise and large bandwidth. These amplifiers are based on the parametric amplification of microwaves traveling along a transmission line with embedded nonlinear elements. We are developing superconducting TWPAs based both on Josephson junction arrays (Traveling Wave Josephson Parametric Amplifiers) and on nonlinear kinetic inductance (Dispersion Engineered Traveling Wave Kinetic Inductance Amplifiers). Our goal is to achieve large bandwidth (in the 5 to 10 GHz range), large gain (more than 20 dB), large saturation power (more than −50 dBm), and near quantum limited noise (noise temperature less than 600 mK). Current achievements in the design and development of the high performance TWPAs are here reported and discussed, together with current limitations and possible future developments.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="88357385"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="88357385"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 88357385; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=88357385]").text(description); $(".js-view-count[data-work-id=88357385]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 88357385; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='88357385']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 88357385, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=88357385]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":88357385,"title":"Development of Quantum Limited Superconducting Amplifiers for Advanced Detection","translated_title":"","metadata":{"abstract":"Ultralow-noise microwave amplification and detection play a central role in different applications, going from fundamental physics experiments to the deployment of quantum technologies. In many applications the necessity of reading multiple detectors, or cavities or qubits, calls for large bandwidth amplifiers with the lowest possible noise. Current technologies are based on High Electron Mobility Transistors and Josephson Parametric Amplifiers. Both have limitations, the former in terms of the minimum noise, the latter in terms of bandwidth. Superconducting Traveling Wave Parametric Amplifiers (TWPAs) have the potential of offering quantum limited noise and large bandwidth. These amplifiers are based on the parametric amplification of microwaves traveling along a transmission line with embedded nonlinear elements. We are developing superconducting TWPAs based both on Josephson junction arrays (Traveling Wave Josephson Parametric Amplifiers) and on nonlinear kinetic inductance (Dispersion Engineered Traveling Wave Kinetic Inductance Amplifiers). Our goal is to achieve large bandwidth (in the 5 to 10 GHz range), large gain (more than 20 dB), large saturation power (more than −50 dBm), and near quantum limited noise (noise temperature less than 600 mK). Current achievements in the design and development of the high performance TWPAs are here reported and discussed, together with current limitations and possible future developments.","publisher":"Institute of Electrical and Electronics Engineers (IEEE)","publication_date":{"day":null,"month":null,"year":2022,"errors":{}},"publication_name":"IEEE Transactions on Applied Superconductivity"},"translated_abstract":"Ultralow-noise microwave amplification and detection play a central role in different applications, going from fundamental physics experiments to the deployment of quantum technologies. In many applications the necessity of reading multiple detectors, or cavities or qubits, calls for large bandwidth amplifiers with the lowest possible noise. 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Based on some recently published analytic approximations (valid in the infinite-test-mass limit) for the Brownian and thermoelastic mirror noises in the presence of arbitrary-shaped beams, this paper addresses certain preliminary issues related to the optimal beam-shaping problem. In particular, with specific reference to the Laser Interferometer Gravitational-wave Observatory (LIGO) experiment, absolute and realistic lower-bounds for the various thermal noise constituents are obtained and compared with the current status (Gaussian beams) and trends (&amp;quot;mesa&amp;quot; beams), indicating fairly ample margins for further reduction. In this framework, the effective dimension of the related optimization problem, and its relationship to the critical design parameters are identified, physical-feasibility and model-consistency issues are considered, and possible additional requirements and/or prior information exploitable to drive the subsequent optimization process are highlighted.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="88357375"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="88357375"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 88357375; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=88357375]").text(description); $(".js-view-count[data-work-id=88357375]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 88357375; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='88357375']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 88357375, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=88357375]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":88357375,"title":"Perspectives on B eam -Shaping O ptim ization for Therm al-N oise R eduction in A dvanced G ravitational-W ave Interferom etric D etectors: B ounds,Proles,and C riticalParam eters","translated_title":"","metadata":{"abstract":"ABSTRACT Suitable shaping (in particular, flattening and broadening) of the laser beam has recently been proposed as an effective device to reduce internal (mirror) thermal noise in advanced gravitational wave interferometric detectors. 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}); </script> <div class="js-work-strip profile--work_container" data-work-id="88357363"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/88357363/Josephson_based_Threshold_Detector_for_L%C3%A9vy_Distributed_Current_Fluctuations"><img alt="Research paper thumbnail of Josephson-based Threshold Detector for Lévy-Distributed Current Fluctuations" class="work-thumbnail" src="https://attachments.academia-assets.com/92345233/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/88357363/Josephson_based_Threshold_Detector_for_L%C3%A9vy_Distributed_Current_Fluctuations">Josephson-based Threshold Detector for Lévy-Distributed Current Fluctuations</a></div><div class="wp-workCard_item"><span>Physical Review Applied</span><span>, 2019</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="09ba81cf64af1e833a114cf35072b28c" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":92345233,"asset_id":88357363,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/92345233/download_file?st=MTczMjgwMjYzMCw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="88357363"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span 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The Lévy noise current added to a linearly ramped bias current results in clear changes in the distribution of switching currents out of the zero-voltage state of the junction. We observe that the analysis of the cumulative distribution function of the switching currents supplies information on both the characteristics shape parameter α of the Lévy statistics and the intensity of the fluctuations. Moreover, we discuss a theoretical model which allows to extract characteristic features of the Lévy fluctuations from a measured distribution of switching currents. 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In this context, we investigate the probability distribution of the Josephson junctions switching current taking into account the effect of the bias sweeping rate and introducing a simple nonideal quantum measurements scheme. The measurements are modelled as repeated voltage samplings at discrete time intervals, that is with repeated projections of the time dependent quantum solutions on the static or the running states, to retrieve the probability distribution of the switching currents. The distribution appears to be immune of the quantum Zeno effect, and it is close to, but distinguishable from, the Wentzel-Kramers-Brillouin approximation. For energy barriers comparable to the quantum fundamental energy state and in the fast bias current ramp rate the difference is neat, and remains sizeable in the asymptotic slow rate limit. This behaviour is a consequence of the quantum character of the system that confirms the presence of a backreaction of quantum measurements on the outcome of mesoscopic Josephson junctions.","publication_date":{"day":null,"month":null,"year":2016,"errors":{}},"publication_name":"Physical Review A","grobid_abstract_attachment_id":92345226},"translated_abstract":null,"internal_url":"https://www.academia.edu/88357358/Nonideal_quantum_measurement_effects_on_the_switching_current_distribution_of_Josephson_junctions","translated_internal_url":"","created_at":"2022-10-12T11:16:30.759-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":32700082,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[{"id":92345226,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/92345226/thumbnails/1.jpg","file_name":"1607.pdf","download_url":"https://www.academia.edu/attachments/92345226/download_file?st=MTczMjgwMjYzMCw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Nonideal_quantum_measurement_effects_on.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/92345226/1607-libre.pdf?1665606488=\u0026response-content-disposition=attachment%3B+filename%3DNonideal_quantum_measurement_effects_on.pdf\u0026Expires=1732777821\u0026Signature=E78M6PZ0ehm0mR-AV80geFIBPHuzdpAKovjJEuzAsvhq7A2e9w-cLW0wFVVfr78~iWJWkjz5vpRlIKf6H-LPu9Ci-R2CgjYe8Lza1QH7I5EoU39AlyZSrsgwK8xDnACLeWUDtoXvkND60O4CjbvTQvcMxqxz3yx5t5xpFwB4jzphoHm6J9Yw-BvWlQgjAn0etjN~bXX-gpQsuB~FwX4Vg2k8UB-FcynCmKzKaygT~dRmUdw5mBCcSR3P9Bxl50-jxJHsU5eaDxkeSuOynLtQ4j7KLFtxiK2SZhLhyAO49e7pATPd~NrGped8RNiOGEkh2yvK2~xReai9azkqWtbHkA__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"Nonideal_quantum_measurement_effects_on_the_switching_current_distribution_of_Josephson_junctions","translated_slug":"","page_count":9,"language":"en","content_type":"Work","owner":{"id":32700082,"first_name":"Vincenzo","middle_initials":null,"last_name":"Pierro","page_name":"VincenzoPierro","domain_name":"unisannio","created_at":"2015-07-01T06:11:32.248-07:00","display_name":"Vincenzo Pierro","url":"https://unisannio.academia.edu/VincenzoPierro"},"attachments":[{"id":92345226,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/92345226/thumbnails/1.jpg","file_name":"1607.pdf","download_url":"https://www.academia.edu/attachments/92345226/download_file?st=MTczMjgwMjYzMCw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Nonideal_quantum_measurement_effects_on.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/92345226/1607-libre.pdf?1665606488=\u0026response-content-disposition=attachment%3B+filename%3DNonideal_quantum_measurement_effects_on.pdf\u0026Expires=1732777821\u0026Signature=E78M6PZ0ehm0mR-AV80geFIBPHuzdpAKovjJEuzAsvhq7A2e9w-cLW0wFVVfr78~iWJWkjz5vpRlIKf6H-LPu9Ci-R2CgjYe8Lza1QH7I5EoU39AlyZSrsgwK8xDnACLeWUDtoXvkND60O4CjbvTQvcMxqxz3yx5t5xpFwB4jzphoHm6J9Yw-BvWlQgjAn0etjN~bXX-gpQsuB~FwX4Vg2k8UB-FcynCmKzKaygT~dRmUdw5mBCcSR3P9Bxl50-jxJHsU5eaDxkeSuOynLtQ4j7KLFtxiK2SZhLhyAO49e7pATPd~NrGped8RNiOGEkh2yvK2~xReai9azkqWtbHkA__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":498,"name":"Physics","url":"https://www.academia.edu/Documents/in/Physics"},{"id":518,"name":"Quantum Physics","url":"https://www.academia.edu/Documents/in/Quantum_Physics"}],"urls":[{"id":24705161,"url":"http://link.aps.org/article/10.1103/PhysRevA.94.042116"}]}, dispatcherData: dispatcherData }); 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$(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> </div><div class="profile--tab_content_container js-tab-pane tab-pane" data-section-id="3130336" id="papers"><div class="js-work-strip profile--work_container" data-work-id="105869624"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/105869624/Sequential_nonideal_measurements_of_quantum_oscillators_Statistical_characterization_with_and_without_environmental_coupling"><img alt="Research paper thumbnail of Sequential nonideal measurements of quantum oscillators: Statistical characterization with and without environmental coupling" class="work-thumbnail" src="https://attachments.academia-assets.com/105219238/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/105869624/Sequential_nonideal_measurements_of_quantum_oscillators_Statistical_characterization_with_and_without_environmental_coupling">Sequential nonideal measurements of quantum oscillators: Statistical characterization with and without environmental coupling</a></div><div class="wp-workCard_item"><span>Physical Review A</span><span>, 2015</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="2d6ddf4e8b972a690412a536fd5c66f6" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":105219238,"asset_id":105869624,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/105219238/download_file?st=MTczMjgwMjYzMCw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="105869624"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="105869624"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 105869624; 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As a first contribution, it is shown that, under a quantum nondemolition measurement scheme applied to a system initially at the ground state: i) the observed sequence of measurements (quantum tracks) corresponding to a single experiment converges to a limit point, and that ii) the limit point is random over the ensemble of the experiments, being distributed as a zero-mean Gaussian random variable with a variance at most equal to the ground state variance. As a second contribution, the richer scenario where the oscillator is coupled with a frozen (i.e., at the ground state) ensemble of independent quantum oscillators. A sharply different behavior emerges: under the same measurement scheme, here we observe that the measurement sequences are essentially divergent. Such a rigorous statistical analysis of the sequential measurement process might be useful for characterizing the main quantities that are currently used for inference, manipulation and monitoring of many quantum systems. Several interesting properties of the quantum tracks evolution, as well as of the associated (quantum) threshold crossing times are discussed, and the dependence upon the main system parameters (e.g., the choice of the measurement sampling time, the degree of interaction with the environment, the measurement device accuracy) are elucidated. At a more fundamental level, it is seen that, as an application of basic Quantum Mechanics principles, a sharp difference exists between the intrinsic randomness unavoidably present in any quantum system, and the extrinsic randomness arising from the environmental coupling, i.e., the randomness induced by an external source of disturbance.","publication_date":{"day":null,"month":null,"year":2015,"errors":{}},"publication_name":"Physical Review A","grobid_abstract_attachment_id":105219238},"translated_abstract":null,"internal_url":"https://www.academia.edu/105869624/Sequential_nonideal_measurements_of_quantum_oscillators_Statistical_characterization_with_and_without_environmental_coupling","translated_internal_url":"","created_at":"2023-08-22T23:31:10.850-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":32700082,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[{"id":105219238,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/105219238/thumbnails/1.jpg","file_name":"1511.03849v1.pdf","download_url":"https://www.academia.edu/attachments/105219238/download_file?st=MTczMjgwMjYzMCw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Sequential_nonideal_measurements_of_quan.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/105219238/1511.03849v1-libre.pdf?1692772556=\u0026response-content-disposition=attachment%3B+filename%3DSequential_nonideal_measurements_of_quan.pdf\u0026Expires=1732777820\u0026Signature=IlOtcVTUiLo0umfsg59fIovFmsYgs9YizOLTbtr7y8r3R-Yh~50WrS4Qaf7ZqFwgWUGK5Pv4gDPic6qQiHaM9AZMLK6uN3ldON8Gr9iYyV511R6P9U-Wq9RAFn79f1YlqYm6lkSmCRQjn8uw8iCiuRqQlhUOMKH9SoAd-tRrkve7peKjaI-39Pjt9SLBpBEKWeAYZ-3pPV5I7u1jluu3E~1FaHj0k10e0MBfpH5x5Arp8FgwMJ5H1EsI4R4xzh2cKUpY7RzUGblFjunpwQ14nGeEqauu7qJbHhaKpKI1nq7d1TAHCQNPuc56jvGrVnnTJyvV6N0x8NKhnvhMheXQSg__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"Sequential_nonideal_measurements_of_quantum_oscillators_Statistical_characterization_with_and_without_environmental_coupling","translated_slug":"","page_count":18,"language":"en","content_type":"Work","owner":{"id":32700082,"first_name":"Vincenzo","middle_initials":null,"last_name":"Pierro","page_name":"VincenzoPierro","domain_name":"unisannio","created_at":"2015-07-01T06:11:32.248-07:00","display_name":"Vincenzo Pierro","url":"https://unisannio.academia.edu/VincenzoPierro"},"attachments":[{"id":105219238,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/105219238/thumbnails/1.jpg","file_name":"1511.03849v1.pdf","download_url":"https://www.academia.edu/attachments/105219238/download_file?st=MTczMjgwMjYzMCw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Sequential_nonideal_measurements_of_quan.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/105219238/1511.03849v1-libre.pdf?1692772556=\u0026response-content-disposition=attachment%3B+filename%3DSequential_nonideal_measurements_of_quan.pdf\u0026Expires=1732777820\u0026Signature=IlOtcVTUiLo0umfsg59fIovFmsYgs9YizOLTbtr7y8r3R-Yh~50WrS4Qaf7ZqFwgWUGK5Pv4gDPic6qQiHaM9AZMLK6uN3ldON8Gr9iYyV511R6P9U-Wq9RAFn79f1YlqYm6lkSmCRQjn8uw8iCiuRqQlhUOMKH9SoAd-tRrkve7peKjaI-39Pjt9SLBpBEKWeAYZ-3pPV5I7u1jluu3E~1FaHj0k10e0MBfpH5x5Arp8FgwMJ5H1EsI4R4xzh2cKUpY7RzUGblFjunpwQ14nGeEqauu7qJbHhaKpKI1nq7d1TAHCQNPuc56jvGrVnnTJyvV6N0x8NKhnvhMheXQSg__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":498,"name":"Physics","url":"https://www.academia.edu/Documents/in/Physics"},{"id":16460,"name":"Statistical Physics","url":"https://www.academia.edu/Documents/in/Statistical_Physics"},{"id":69262,"name":"Quantum","url":"https://www.academia.edu/Documents/in/Quantum"},{"id":80414,"name":"Mathematical Sciences","url":"https://www.academia.edu/Documents/in/Mathematical_Sciences"},{"id":118582,"name":"Physical sciences","url":"https://www.academia.edu/Documents/in/Physical_sciences"},{"id":129087,"name":"Randomness","url":"https://www.academia.edu/Documents/in/Randomness"},{"id":260118,"name":"CHEMICAL SCIENCES","url":"https://www.academia.edu/Documents/in/CHEMICAL_SCIENCES"},{"id":1007970,"name":"Quantum Process","url":"https://www.academia.edu/Documents/in/Quantum_Process"}],"urls":[]}, dispatcherData: dispatcherData }); 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We will refer to cryogenic operating temperatures, where the low refractive index material has mechanical losses higher than those of the high refractive index material. This situation is the exact opposite of that which occurs at room temperature, which is already widely known. The optimal design of the dielectric mirror (without a priori assumptions on thicknesses) can be obtained through the combined multi-objective optimization of transmittance and thermal noise. In the following, we apply several multi-objective meta-heuristics to compute the Pareto front related to the optimization problem of dielectric mirror thicknesses made of two materials (binary coatings). This approach gives us more certainty about the structure of the final result. We find strong evidence that all meta-heuristics converge to the same solution. 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We will refer to cryogenic operating temperatures, where the low refractive index material has mechanical losses higher than those of the high refractive index material. This situation is the exact opposite of that which occurs at room temperature, which is already widely known. The optimal design of the dielectric mirror (without a priori assumptions on thicknesses) can be obtained through the combined multi-objective optimization of transmittance and thermal noise. In the following, we apply several multi-objective meta-heuristics to compute the Pareto front related to the optimization problem of dielectric mirror thicknesses made of two materials (binary coatings). This approach gives us more certainty about the structure of the final result. We find strong evidence that all meta-heuristics converge to the same solution. The fi...","publisher":"MDPI AG","publication_name":"Applied Sciences"},"translated_abstract":"In this paper, we explore the behavior of several optimization methods for reducing coating Brownian noise in the mirrors of gravitational wave detectors. We will refer to cryogenic operating temperatures, where the low refractive index material has mechanical losses higher than those of the high refractive index material. This situation is the exact opposite of that which occurs at room temperature, which is already widely known. The optimal design of the dielectric mirror (without a priori assumptions on thicknesses) can be obtained through the combined multi-objective optimization of transmittance and thermal noise. In the following, we apply several multi-objective meta-heuristics to compute the Pareto front related to the optimization problem of dielectric mirror thicknesses made of two materials (binary coatings). This approach gives us more certainty about the structure of the final result. We find strong evidence that all meta-heuristics converge to the same solution. 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We carry out the searches in the LIGO data from the first six months of the third Advanced LIGO and Virgo observing run using the Weave semi-coherent method, which sums matched-filter detection-statistic values over many time segments spanning the observation period. No gravitational wave signal is detected in the search band of 20-976 Hz for assumed source ages greater than 300 years for Cas A and greater than 700 years for Vela Jr. Estimates from simulated continuous wave signals indicate we achieve the most sensitive results to date across the explored parameter space volume, probing to strain magnitudes as low as ∼6.3 × 10 −26 for Cas A and ∼5.6 × 10 −26 for Vela Jr. at frequencies near 166 Hz at 95% efficiency.","publication_name":"Physical Review 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href="https://www.academia.edu/98516823/Identification_and_mitigation_of_narrow_spectral_artifacts_that_degrade_searches_for_persistent_gravitational_waves_in_the_first_two_observing_runs_of_Advanced_LIGO"><img alt="Research paper thumbnail of Identification and mitigation of narrow spectral artifacts that degrade searches for persistent gravitational waves in the first two observing runs of Advanced LIGO" class="work-thumbnail" src="https://attachments.academia-assets.com/99845464/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/98516823/Identification_and_mitigation_of_narrow_spectral_artifacts_that_degrade_searches_for_persistent_gravitational_waves_in_the_first_two_observing_runs_of_Advanced_LIGO">Identification and mitigation of narrow spectral artifacts that degrade searches for persistent gravitational waves in the first two observing runs of Advanced LIGO</a></div><div class="wp-workCard_item"><span>Physical Review D</span><span>, 2018</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="e2ce3770306a56537013ebec7c6dfc98" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":99845464,"asset_id":98516823,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/99845464/download_file?st=MTczMjgwMjYzMCw4LjIyMi4yMDguMTQ2&st=MTczMjgwMjYzMCw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="98516823"><a 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$(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="91767452"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/91767452/Negative_differential_resistance_in_Josephson_junctions_coupled_to_a_cavity"><img alt="Research paper thumbnail of Negative differential resistance in Josephson junctions coupled to a cavity" class="work-thumbnail" src="https://attachments.academia-assets.com/94960623/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/91767452/Negative_differential_resistance_in_Josephson_junctions_coupled_to_a_cavity">Negative differential resistance in Josephson junctions coupled to a cavity</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Regions with negative differential resistance can arise in the IV curve of Josephson junctions an...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Regions with negative differential resistance can arise in the IV curve of Josephson junctions and this phenomenon plays an essential role for applications, in particular for THz radiation emission. For the measurement of high frequency radiation from Josephson junctions, a cavity-either internal or externalis often used. A cavity may also induce a negative differential resistance region at the lower side of the resonance frequency. We investigate the dynamics of Josephson junctions with a negative differential resistance in the quasi particle tunnel current, i.e. in the McCumber curve. We find that very complicated and unexpected interactions take place. This may be useful for the interpretation of experimental measurements of THz radiation from intrinsic Josephson junctions.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="9c76f0f2ce3472d14803e0db65e26b19" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":94960623,"asset_id":91767452,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/94960623/download_file?st=MTczMjgwMjYzMCw4LjIyMi4yMDguMTQ2&s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="91767452"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="91767452"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 91767452; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=91767452]").text(description); $(".js-view-count[data-work-id=91767452]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 91767452; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='91767452']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 91767452, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "9c76f0f2ce3472d14803e0db65e26b19" } } $('.js-work-strip[data-work-id=91767452]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":91767452,"title":"Negative differential resistance in Josephson junctions coupled to a cavity","translated_title":"","metadata":{"doi":"10.1016/j.physc.2014.02.025","abstract":"Regions with negative differential resistance can arise in the IV curve of Josephson junctions and this phenomenon plays an essential role for applications, in particular for THz radiation emission. For the measurement of high frequency radiation from Josephson junctions, a cavity-either internal or externalis often used. A cavity may also induce a negative differential resistance region at the lower side of the resonance frequency. We investigate the dynamics of Josephson junctions with a negative differential resistance in the quasi particle tunnel current, i.e. in the McCumber curve. We find that very complicated and unexpected interactions take place. This may be useful for the interpretation of experimental measurements of THz radiation from intrinsic Josephson junctions."},"translated_abstract":"Regions with negative differential resistance can arise in the IV curve of Josephson junctions and this phenomenon plays an essential role for applications, in particular for THz radiation emission. For the measurement of high frequency radiation from Josephson junctions, a cavity-either internal or externalis often used. A cavity may also induce a negative differential resistance region at the lower side of the resonance frequency. We investigate the dynamics of Josephson junctions with a negative differential resistance in the quasi particle tunnel current, i.e. in the McCumber curve. We find that very complicated and unexpected interactions take place. This may be useful for the interpretation of experimental measurements of THz radiation from intrinsic Josephson junctions.","internal_url":"https://www.academia.edu/91767452/Negative_differential_resistance_in_Josephson_junctions_coupled_to_a_cavity","translated_internal_url":"","created_at":"2022-11-28T03:04:32.756-08:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":32700082,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[{"id":39125386,"work_id":91767452,"tagging_user_id":32700082,"tagged_user_id":38757552,"co_author_invite_id":null,"email":"m***n@mat.dtu.dk","display_order":1,"name":"Mads Sørensen","title":"Negative differential resistance in Josephson junctions coupled to a cavity"},{"id":39125387,"work_id":91767452,"tagging_user_id":32700082,"tagged_user_id":38825248,"co_author_invite_id":null,"email":"n***n@mat.dtu.dk","display_order":2,"name":"Niels Pedersen","title":"Negative differential resistance in Josephson junctions coupled to a cavity"},{"id":39125388,"work_id":91767452,"tagging_user_id":32700082,"tagged_user_id":32627756,"co_author_invite_id":null,"email":"f***a@unisannio.it","affiliation":"Università degli Studi del Sannio","display_order":3,"name":"G. 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We demonstrate that the loss of information that occurs retaining only the sequence of escapes , rather than the full trajectory, can be very mild and can lead to an effective method to reveal the noise intensity or the presence of a coherent signal.","publication_date":{"day":null,"month":null,"year":2013,"errors":{}},"publication_name":"EPL (Europhysics Letters)","grobid_abstract_attachment_id":92348626},"translated_abstract":null,"internal_url":"https://www.academia.edu/88361862/Escape_time_characterization_of_pendular_Fabry_Perot","translated_internal_url":"","created_at":"2022-10-12T12:59:02.332-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":32700082,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[{"id":92348626,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/92348626/thumbnails/1.jpg","file_name":"1301.2653v1.pdf","download_url":"https://www.academia.edu/attachments/92348626/download_file?st=MTczMjgwMjYzMCw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Escape_time_characterization_of_pendular.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/92348626/1301.2653v1-libre.pdf?1665606402=\u0026response-content-disposition=attachment%3B+filename%3DEscape_time_characterization_of_pendular.pdf\u0026Expires=1732777820\u0026Signature=Glq0Pu-i~rDEb4qqjluHYp~FkRYlkLYSVLtirz1iP2aSZJig8hQ3TDV4sFMHj8-R95BffcaX4MpXFpOtbnddtroD6E0cHwcmn7NZaNRCOrsEZ9KBFV~7zx98tONmSthv7SeiSWKAsBW3EYmZnA9Agxomh9WmRdcP2kiu~rg5iyBSqZtp3-EPcvc6Sl1rhY9hL7FajTE1kDdAIm313AHj1AUhhFz8caCXnE-45~tjnTxmIpDVJVMqk6vFFMSgElfRmahzMP--zikHOTDKzwnQGzuqypgqleYTDfElhNf9p6~zxFL3Ld35L8faifMx11FoBvaSFwF-oUQOWOGMubn3xQ__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"Escape_time_characterization_of_pendular_Fabry_Perot","translated_slug":"","page_count":16,"language":"en","content_type":"Work","owner":{"id":32700082,"first_name":"Vincenzo","middle_initials":null,"last_name":"Pierro","page_name":"VincenzoPierro","domain_name":"unisannio","created_at":"2015-07-01T06:11:32.248-07:00","display_name":"Vincenzo Pierro","url":"https://unisannio.academia.edu/VincenzoPierro"},"attachments":[{"id":92348626,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/92348626/thumbnails/1.jpg","file_name":"1301.2653v1.pdf","download_url":"https://www.academia.edu/attachments/92348626/download_file?st=MTczMjgwMjYzMCw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Escape_time_characterization_of_pendular.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/92348626/1301.2653v1-libre.pdf?1665606402=\u0026response-content-disposition=attachment%3B+filename%3DEscape_time_characterization_of_pendular.pdf\u0026Expires=1732777820\u0026Signature=Glq0Pu-i~rDEb4qqjluHYp~FkRYlkLYSVLtirz1iP2aSZJig8hQ3TDV4sFMHj8-R95BffcaX4MpXFpOtbnddtroD6E0cHwcmn7NZaNRCOrsEZ9KBFV~7zx98tONmSthv7SeiSWKAsBW3EYmZnA9Agxomh9WmRdcP2kiu~rg5iyBSqZtp3-EPcvc6Sl1rhY9hL7FajTE1kDdAIm313AHj1AUhhFz8caCXnE-45~tjnTxmIpDVJVMqk6vFFMSgElfRmahzMP--zikHOTDKzwnQGzuqypgqleYTDfElhNf9p6~zxFL3Ld35L8faifMx11FoBvaSFwF-oUQOWOGMubn3xQ__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":498,"name":"Physics","url":"https://www.academia.edu/Documents/in/Physics"},{"id":80414,"name":"Mathematical Sciences","url":"https://www.academia.edu/Documents/in/Mathematical_Sciences"},{"id":118582,"name":"Physical sciences","url":"https://www.academia.edu/Documents/in/Physical_sciences"},{"id":148392,"name":"EPL","url":"https://www.academia.edu/Documents/in/EPL"}],"urls":[{"id":24707388,"url":"https://iopscience.iop.org/article/10.1209/0295-5075/101/20005/pdf"}]}, dispatcherData: dispatcherData }); 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Engineering","url":"https://www.academia.edu/Documents/in/Materials_Engineering"},{"id":498,"name":"Physics","url":"https://www.academia.edu/Documents/in/Physics"},{"id":505,"name":"Condensed Matter Physics","url":"https://www.academia.edu/Documents/in/Condensed_Matter_Physics"},{"id":343764,"name":"Squid","url":"https://www.academia.edu/Documents/in/Squid"},{"id":877641,"name":"Amplifier","url":"https://www.academia.edu/Documents/in/Amplifier"},{"id":901940,"name":"Parametric Statistics","url":"https://www.academia.edu/Documents/in/Parametric_Statistics"},{"id":1237788,"name":"Electrical And Electronic Engineering","url":"https://www.academia.edu/Documents/in/Electrical_And_Electronic_Engineering"},{"id":1308377,"name":"Figure of Merit","url":"https://www.academia.edu/Documents/in/Figure_of_Merit"},{"id":2493561,"name":"Quantum Noise","url":"https://www.academia.edu/Documents/in/Quantum_Noise"}],"urls":[{"id":24705179,"url":"http://xplorestaging.ieee.org/ielx7/77/9646455/09705608.pdf?arnumber=9705608"}]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="88357385"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/88357385/Development_of_Quantum_Limited_Superconducting_Amplifiers_for_Advanced_Detection"><img alt="Research paper thumbnail of Development of Quantum Limited Superconducting Amplifiers for Advanced Detection" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/88357385/Development_of_Quantum_Limited_Superconducting_Amplifiers_for_Advanced_Detection">Development of Quantum Limited Superconducting Amplifiers for Advanced Detection</a></div><div class="wp-workCard_item"><span>IEEE Transactions on Applied Superconductivity</span><span>, 2022</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Ultralow-noise microwave amplification and detection play a central role in different application...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Ultralow-noise microwave amplification and detection play a central role in different applications, going from fundamental physics experiments to the deployment of quantum technologies. In many applications the necessity of reading multiple detectors, or cavities or qubits, calls for large bandwidth amplifiers with the lowest possible noise. Current technologies are based on High Electron Mobility Transistors and Josephson Parametric Amplifiers. Both have limitations, the former in terms of the minimum noise, the latter in terms of bandwidth. Superconducting Traveling Wave Parametric Amplifiers (TWPAs) have the potential of offering quantum limited noise and large bandwidth. These amplifiers are based on the parametric amplification of microwaves traveling along a transmission line with embedded nonlinear elements. We are developing superconducting TWPAs based both on Josephson junction arrays (Traveling Wave Josephson Parametric Amplifiers) and on nonlinear kinetic inductance (Dispersion Engineered Traveling Wave Kinetic Inductance Amplifiers). Our goal is to achieve large bandwidth (in the 5 to 10 GHz range), large gain (more than 20 dB), large saturation power (more than −50 dBm), and near quantum limited noise (noise temperature less than 600 mK). Current achievements in the design and development of the high performance TWPAs are here reported and discussed, together with current limitations and possible future developments.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="88357385"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="88357385"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 88357385; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=88357385]").text(description); $(".js-view-count[data-work-id=88357385]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 88357385; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='88357385']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 88357385, container: "", }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=88357385]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":88357385,"title":"Development of Quantum Limited Superconducting Amplifiers for Advanced Detection","translated_title":"","metadata":{"abstract":"Ultralow-noise microwave amplification and detection play a central role in different applications, going from fundamental physics experiments to the deployment of quantum technologies. In many applications the necessity of reading multiple detectors, or cavities or qubits, calls for large bandwidth amplifiers with the lowest possible noise. Current technologies are based on High Electron Mobility Transistors and Josephson Parametric Amplifiers. Both have limitations, the former in terms of the minimum noise, the latter in terms of bandwidth. Superconducting Traveling Wave Parametric Amplifiers (TWPAs) have the potential of offering quantum limited noise and large bandwidth. These amplifiers are based on the parametric amplification of microwaves traveling along a transmission line with embedded nonlinear elements. We are developing superconducting TWPAs based both on Josephson junction arrays (Traveling Wave Josephson Parametric Amplifiers) and on nonlinear kinetic inductance (Dispersion Engineered Traveling Wave Kinetic Inductance Amplifiers). 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Based on some recently published analytic approximations (valid in the infinite-test-mass limit) for the Brownian and thermoelastic mirror noises in the presence of arbitrary-shaped beams, this paper addresses certain preliminary issues related to the optimal beam-shaping problem. In particular, with specific reference to the Laser Interferometer Gravitational-wave Observatory (LIGO) experiment, absolute and realistic lower-bounds for the various thermal noise constituents are obtained and compared with the current status (Gaussian beams) and trends (&amp;quot;mesa&amp;quot; beams), indicating fairly ample margins for further reduction. 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In particular, with specific reference to the Laser Interferometer Gravitational-wave Observatory (LIGO) experiment, absolute and realistic lower-bounds for the various thermal noise constituents are obtained and compared with the current status (Gaussian beams) and trends (\u0026amp;quot;mesa\u0026amp;quot; beams), indicating fairly ample margins for further reduction. 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highlighted.","internal_url":"https://www.academia.edu/88357375/Perspectives_on_B_eam_Shaping_O_ptim_ization_for_Therm_al_N_oise_R_eduction_in_A_dvanced_G_ravitational_W_ave_Interferom_etric_D_etectors_B_ounds_Proles_and_C_riticalParam_eters","translated_internal_url":"","created_at":"2022-10-12T11:16:36.233-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":32700082,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[],"slug":"Perspectives_on_B_eam_Shaping_O_ptim_ization_for_Therm_al_N_oise_R_eduction_in_A_dvanced_G_ravitational_W_ave_Interferom_etric_D_etectors_B_ounds_Proles_and_C_riticalParam_eters","translated_slug":"","page_count":null,"language":"en","content_type":"Work","owner":{"id":32700082,"first_name":"Vincenzo","middle_initials":null,"last_name":"Pierro","page_name":"VincenzoPierro","domain_name":"unisannio","created_at":"2015-07-01T06:11:32.248-07:00","display_name":"Vincenzo 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The Lévy noise current added to a linearly ramped bias current results in clear changes in the distribution of switching currents out of the zero-voltage state of the junction. We observe that the analysis of the cumulative distribution function of the switching currents supplies information on both the characteristics shape parameter α of the Lévy statistics and the intensity of the fluctuations. Moreover, we discuss a theoretical model which allows to extract characteristic features of the Lévy fluctuations from a measured distribution of switching currents. 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dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "25c1bcb2c118860907c03a7e44924e80" } } $('.js-work-strip[data-work-id=88357358]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":88357358,"title":"Nonideal quantum measurement effects on the switching-current distribution of Josephson junctions","translated_title":"","metadata":{"publisher":"American Physical Society (APS)","grobid_abstract":"The quantum character of Josephson junctions is ordinarily revealed through the analysis of the switching currents, i.e. the current at which a finite voltage appears: A sharp rise of the voltage signals the passage (tunnel) from a trapped state (the zero voltage solution) to a running state (the finite voltage solution). In this context, we investigate the probability distribution of the Josephson junctions switching current taking into account the effect of the bias sweeping rate and introducing a simple nonideal quantum measurements scheme. The measurements are modelled as repeated voltage samplings at discrete time intervals, that is with repeated projections of the time dependent quantum solutions on the static or the running states, to retrieve the probability distribution of the switching currents. The distribution appears to be immune of the quantum Zeno effect, and it is close to, but distinguishable from, the Wentzel-Kramers-Brillouin approximation. For energy barriers comparable to the quantum fundamental energy state and in the fast bias current ramp rate the difference is neat, and remains sizeable in the asymptotic slow rate limit. This behaviour is a consequence of the quantum character of the system that confirms the presence of a backreaction of quantum measurements on the outcome of mesoscopic Josephson junctions.","publication_date":{"day":null,"month":null,"year":2016,"errors":{}},"publication_name":"Physical Review A","grobid_abstract_attachment_id":92345226},"translated_abstract":null,"internal_url":"https://www.academia.edu/88357358/Nonideal_quantum_measurement_effects_on_the_switching_current_distribution_of_Josephson_junctions","translated_internal_url":"","created_at":"2022-10-12T11:16:30.759-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":32700082,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[{"id":92345226,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/92345226/thumbnails/1.jpg","file_name":"1607.pdf","download_url":"https://www.academia.edu/attachments/92345226/download_file?st=MTczMjgwMjYzMCw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Nonideal_quantum_measurement_effects_on.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/92345226/1607-libre.pdf?1665606488=\u0026response-content-disposition=attachment%3B+filename%3DNonideal_quantum_measurement_effects_on.pdf\u0026Expires=1732777821\u0026Signature=E78M6PZ0ehm0mR-AV80geFIBPHuzdpAKovjJEuzAsvhq7A2e9w-cLW0wFVVfr78~iWJWkjz5vpRlIKf6H-LPu9Ci-R2CgjYe8Lza1QH7I5EoU39AlyZSrsgwK8xDnACLeWUDtoXvkND60O4CjbvTQvcMxqxz3yx5t5xpFwB4jzphoHm6J9Yw-BvWlQgjAn0etjN~bXX-gpQsuB~FwX4Vg2k8UB-FcynCmKzKaygT~dRmUdw5mBCcSR3P9Bxl50-jxJHsU5eaDxkeSuOynLtQ4j7KLFtxiK2SZhLhyAO49e7pATPd~NrGped8RNiOGEkh2yvK2~xReai9azkqWtbHkA__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"Nonideal_quantum_measurement_effects_on_the_switching_current_distribution_of_Josephson_junctions","translated_slug":"","page_count":9,"language":"en","content_type":"Work","owner":{"id":32700082,"first_name":"Vincenzo","middle_initials":null,"last_name":"Pierro","page_name":"VincenzoPierro","domain_name":"unisannio","created_at":"2015-07-01T06:11:32.248-07:00","display_name":"Vincenzo Pierro","url":"https://unisannio.academia.edu/VincenzoPierro"},"attachments":[{"id":92345226,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/92345226/thumbnails/1.jpg","file_name":"1607.pdf","download_url":"https://www.academia.edu/attachments/92345226/download_file?st=MTczMjgwMjYzMCw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Nonideal_quantum_measurement_effects_on.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/92345226/1607-libre.pdf?1665606488=\u0026response-content-disposition=attachment%3B+filename%3DNonideal_quantum_measurement_effects_on.pdf\u0026Expires=1732777821\u0026Signature=E78M6PZ0ehm0mR-AV80geFIBPHuzdpAKovjJEuzAsvhq7A2e9w-cLW0wFVVfr78~iWJWkjz5vpRlIKf6H-LPu9Ci-R2CgjYe8Lza1QH7I5EoU39AlyZSrsgwK8xDnACLeWUDtoXvkND60O4CjbvTQvcMxqxz3yx5t5xpFwB4jzphoHm6J9Yw-BvWlQgjAn0etjN~bXX-gpQsuB~FwX4Vg2k8UB-FcynCmKzKaygT~dRmUdw5mBCcSR3P9Bxl50-jxJHsU5eaDxkeSuOynLtQ4j7KLFtxiK2SZhLhyAO49e7pATPd~NrGped8RNiOGEkh2yvK2~xReai9azkqWtbHkA__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":498,"name":"Physics","url":"https://www.academia.edu/Documents/in/Physics"},{"id":518,"name":"Quantum Physics","url":"https://www.academia.edu/Documents/in/Quantum_Physics"}],"urls":[{"id":24705161,"url":"http://link.aps.org/article/10.1103/PhysRevA.94.042116"}]}, dispatcherData: dispatcherData }); 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