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href="https://www.academia.edu/22534531/Semiclassical_Transport_Models_for_Semiconductor_Spintronics"><img alt="Research paper thumbnail of Semiclassical Transport Models for Semiconductor Spintronics" class="work-thumbnail" src="https://attachments.academia-assets.com/43148409/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/22534531/Semiclassical_Transport_Models_for_Semiconductor_Spintronics">Semiclassical Transport Models for Semiconductor Spintronics</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">We will summarize and consider several examples of applications of semiclassi- cal approaches use...</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">We will summarize and consider several examples of applications of semiclassi- cal approaches used in semiconductor spintronic device modeling. These include drift-diffusion models, kinetic transport equations and Monte Carlo simulation schemes.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="f1d1965511294760e300bfaa793675c5" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":43148409,"asset_id":22534531,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/43148409/download_file?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="22534531"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="22534531"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 22534531; 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$(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="22534529"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/22534529/Spin_polarized_transport_modeling"><img alt="Research paper thumbnail of Spin-polarized transport modeling" 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" rel="nofollow" href="https://www.academia.edu/22534529/Spin_polarized_transport_modeling">Spin-polarized transport modeling</a></div><div class="wp-workCard_item wp-workCard--coauthors"><span>by </span><span><a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/VladimirPrivman">Vladimir Privman</a> and <a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/SemionSaikin">Semion Saikin</a></span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">The emerging field of semiconductor spintronics promises to utilize spin degree of freedom in ele...</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">The emerging field of semiconductor spintronics promises to utilize spin degree of freedom in electronic device operation. In order to understand advantages and limitations of proposed spintronic devices, realistic models for spin-polarized transport in device structures are needed. We study spin-polarized electron transport properties in semiconductor non-magnetic heterostructures where electron spin dynamics is controlled by a spin-orbit interaction. Two complementary</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="22534529"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="22534529"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 22534529; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=22534529]").text(description); $(".js-view-count[data-work-id=22534529]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 22534529; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='22534529']"); 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></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-a9bf3a2bc8c89fa2a77156577594264ee8a0f214d74241bc0fcd3f69f8d107ac.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" } } $('.js-work-strip[data-work-id=22534529]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":22534529,"title":"Spin-polarized transport modeling","internal_url":"https://www.academia.edu/22534529/Spin_polarized_transport_modeling","owner_id":44056208,"coauthors_can_edit":true,"owner":{"id":44056208,"first_name":"Semion","middle_initials":null,"last_name":"Saikin","page_name":"SemionSaikin","domain_name":"independent","created_at":"2016-02-27T17:30:43.004-08:00","display_name":"Semion Saikin","url":"https://independent.academia.edu/SemionSaikin"},"attachments":[]}, 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="22534525"><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/22534525/Spin_polarized_transport_in_semiconductor_nanostructures"><img alt="Research paper thumbnail of Spin-polarized transport in semiconductor nanostructures" class="work-thumbnail" src="https://attachments.academia-assets.com/43148422/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/22534525/Spin_polarized_transport_in_semiconductor_nanostructures">Spin-polarized transport in semiconductor nanostructures</a></div><div class="wp-workCard_item wp-workCard--coauthors"><span>by </span><span><a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/VladimirPrivman">Vladimir Privman</a> and <a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/SemionSaikin">Semion Saikin</a></span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">We study spin polarization patterns in semiconductor nanostructures produced by stationary inject...</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">We study spin polarization patterns in semiconductor nanostructures produced by stationary injected spin-polarized electrons using the Monte Carlo device simulation scheme. Spatial transport affects the spin polarization by means of a spin-orbit interaction. Effects of the applied electric field along the transport direction, temperature, non-parabolicity of conduction band and anisotropy of the spin-orbit interaction are considered. We compare the simulated</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="45ba76b8a43dfd47dcbc336982d411c4" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":43148422,"asset_id":22534525,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/43148422/download_file?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="22534525"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="22534525"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 22534525; 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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="22534523"><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/22534523/Monte_Carlo_Modeling_of_Spin_FETs_Controlled_by_Spin_Orbit_Interaction"><img alt="Research paper thumbnail of Monte Carlo Modeling of Spin FETs Controlled by Spin-Orbit Interaction" class="work-thumbnail" src="https://attachments.academia-assets.com/43148428/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/22534523/Monte_Carlo_Modeling_of_Spin_FETs_Controlled_by_Spin_Orbit_Interaction">Monte Carlo Modeling of Spin FETs Controlled by Spin-Orbit Interaction</a></div><div class="wp-workCard_item wp-workCard--coauthors"><span>by </span><span><a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/VladimirPrivman">Vladimir Privman</a> and <a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/SemionSaikin">Semion Saikin</a></span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">A method for Monte Carlo simulation of 2D spin-polarized electron transport in III-V semiconducto...</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">A method for Monte Carlo simulation of 2D spin-polarized electron transport in III-V semiconductor heterojunction FETs is presented. In the simulation, the dynamics of the electrons in coordinate and momentum space is treated semiclassically. The density matrix description of the spin is incorporated in the Monte Carlo method to account for the spin polarization dynamics. The spin-orbit interaction in the</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="63948f826bc766ba28c8111361e36be5" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":43148428,"asset_id":22534523,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/43148428/download_file?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="22534523"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="22534523"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 22534523; 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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="22534522"><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/22534522/Probing_biological_light_harvesting_phenomena_by_optical_cavities"><img alt="Research paper thumbnail of Probing biological light-harvesting phenomena by optical cavities" class="work-thumbnail" src="https://attachments.academia-assets.com/43148372/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/22534522/Probing_biological_light_harvesting_phenomena_by_optical_cavities">Probing biological light-harvesting phenomena by optical cavities</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">We propose a driven optical cavity quantum electrodynamics (QED) set up aimed at directly probing...</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">We propose a driven optical cavity quantum electrodynamics (QED) set up aimed at directly probing energy transport dynamics in photosynthetic biomolecules. We show that detailed information concerning energy transfer paths and delocalization of exciton states can be inferred (and exciton energies estimated) from the statistical properties of the emitted photons. This approach provides us with a novel spectroscopic tool for</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="f8bf19799477bd031bea452876f6858c" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":43148372,"asset_id":22534522,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/43148372/download_file?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="22534522"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="22534522"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 22534522; 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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="22534521"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/22534521/Simulation_of_spin_polarized_transport_in_submicrometer_device_structures"><img alt="Research paper thumbnail of Simulation of spin-polarized transport in submicrometer device structures" 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" rel="nofollow" href="https://www.academia.edu/22534521/Simulation_of_spin_polarized_transport_in_submicrometer_device_structures">Simulation of spin-polarized transport in submicrometer device structures</a></div><div class="wp-workCard_item wp-workCard--coauthors"><span>by </span><span><a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/VladimirPrivman">Vladimir Privman</a> and <a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/SemionSaikin">Semion Saikin</a></span></div><div class="wp-workCard_item"><span>2003 Third IEEE Conference on Nanotechnology, 2003. IEEE-NANO 2003.</span><span>, 2003</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">The Monte Carlo approach is utilized to study spin-polarized electron transport in spintronic dev...</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">The Monte Carlo approach is utilized to study spin-polarized electron transport in spintronic device structures. Evolution of the electron spin polarization vector is controlled by the spin-orbit interaction. Spin polarization properties, including the spin-dephasing length and orientation of the polarization vector, are investigated, for the applied voltage from 0.05 V to 0.25 V, and for temperatures ranging from 77 K</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="22534521"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="22534521"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 22534521; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); 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dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=22534521]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":22534521,"title":"Simulation of spin-polarized transport in submicrometer device structures","internal_url":"https://www.academia.edu/22534521/Simulation_of_spin_polarized_transport_in_submicrometer_device_structures","owner_id":44056208,"coauthors_can_edit":true,"owner":{"id":44056208,"first_name":"Semion","middle_initials":null,"last_name":"Saikin","page_name":"SemionSaikin","domain_name":"independent","created_at":"2016-02-27T17:30:43.004-08:00","display_name":"Semion Saikin","url":"https://independent.academia.edu/SemionSaikin"},"attachments":[]}, 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="22534520"><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/22534520/Monte_Carlo_Simulation_of_Spin_Polarized_Transport"><img alt="Research paper thumbnail of Monte Carlo Simulation of Spin-Polarized Transport" class="work-thumbnail" src="https://attachments.academia-assets.com/43148425/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/22534520/Monte_Carlo_Simulation_of_Spin_Polarized_Transport">Monte Carlo Simulation of Spin-Polarized Transport</a></div><div class="wp-workCard_item wp-workCard--coauthors"><span>by </span><span><a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/VladimirPrivman">Vladimir Privman</a> and <a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/SemionSaikin">Semion Saikin</a></span></div><div class="wp-workCard_item"><span>Lecture Notes in Computer Science</span><span>, 2003</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Monte Carlo simulations are performed to study the in-plane transport of spin-polarized electrons...</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">Monte Carlo simulations are performed to study the in-plane transport of spin-polarized electrons in III-V semiconductor quantum wells. The density matrix description of the spin polarization is incorporated in the simulation algorithm. The spin-orbit interaction terms generate coherent evolution of the electron spin polarization and also cause dephasing. The spatial motion of the electrons is treated semiclassically. Three different scattering mechanisms-optical phonons, acoustic phonons and ionized impurities-are considered. The electric field is calculated self-consistently from the charge distribution. The Monte Carlo scheme is described, and simulation results are reported for temperatures in the range 77-300 K.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="ff722c121e7077304c8d2c38036e3671" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":43148425,"asset_id":22534520,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/43148425/download_file?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="22534520"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="22534520"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 22534520; 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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="22534519"><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/22534519/Fast_Delocalization_Leads_To_Robust_Long_Range_Excitonic_Transfer_in_a_Large_Quantum_Chlorosome_Model"><img alt="Research paper thumbnail of Fast Delocalization Leads To Robust Long-Range Excitonic Transfer in a Large Quantum Chlorosome Model" class="work-thumbnail" src="https://attachments.academia-assets.com/43148426/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/22534519/Fast_Delocalization_Leads_To_Robust_Long_Range_Excitonic_Transfer_in_a_Large_Quantum_Chlorosome_Model">Fast Delocalization Leads To Robust Long-Range Excitonic Transfer in a Large Quantum Chlorosome Model</a></div><div class="wp-workCard_item"><span>Nano Letters</span><span>, 2015</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Chlorosomes are efficient light-harvesting antennas containing up to hundreds of thousands of bac...</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">Chlorosomes are efficient light-harvesting antennas containing up to hundreds of thousands of bacteriochlorophyll molecules. With massively parallel computer hardware, we use a nonperturbative stochastic Schrodinger equation, while including an atomistically derived spectral density, to study excitonic energy transfer in a realistically sized chlorosome model. We find that fast short-range delocalization leads to robust long-range transfer due to the antennae's concentric-roll structure. Additionally, we discover anomalous behavior arising from different initial conditions, and outline general considerations for simulating excitonic systems on the nanometer to micrometer scale.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="a51b8cfc4b401904f333cbfaf957136c" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":43148426,"asset_id":22534519,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/43148426/download_file?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="22534519"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="22534519"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 22534519; 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</script> <div class="js-work-strip profile--work_container" data-work-id="15177655"><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/15177655/Quantum_chemistry_calculations_for_arbitrarily_complex_electrostatic_environments"><img alt="Research paper thumbnail of Quantum chemistry calculations for arbitrarily complex electrostatic environments" class="work-thumbnail" src="https://attachments.academia-assets.com/43494892/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/15177655/Quantum_chemistry_calculations_for_arbitrarily_complex_electrostatic_environments">Quantum chemistry calculations for arbitrarily complex electrostatic environments</a></div><div class="wp-workCard_item wp-workCard--coauthors"><span>by </span><span><a class="" data-click-track="profile-work-strip-authors" href="https://uci.academia.edu/DmitrijRappoport">Dmitrij Rappoport</a> and <a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/SemionSaikin">Semion Saikin</a></span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Modeling of electronic structure of molecules in electrostatic environments is of considerable re...</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">Modeling of electronic structure of molecules in electrostatic environments is of considerable relevance for surface-enhanced spectroscopy and molecular electronics. We have developed and implemented a novel approach to the molecular electronic structure in arbitrary electrostatic environments that is compatible with standard quantum chemical methods and can be applied to mediumsized and large molecules. The scheme denoted CheESE (chemistry in electrostatic environments) is based on the description of molecular electronic structure subject to a boundary condition on the system/environment interface. Thus, it is particularly suited to study molecules on metallic surfaces. The proposed model is capable of describing both electrostatic effects near nanostructured metallic surfaces and image-charge effects. We present an implementation of the CheESE model as a library module and show example applications to neutral and negatively charged molecules.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="0247c8c2a520d3ca63c23702d3fc5553" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":43494892,"asset_id":15177655,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/43494892/download_file?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="15177655"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="15177655"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 15177655; 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This transport is easily deteriorated by traps in the disordered energy landscape.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="70c2e906797ed5784c5637f59582a4ef" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":43148420,"asset_id":22534517,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/43148420/download_file?s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="22534517"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="22534517"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 22534517; 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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="22534516"><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/22534516/Chromatic_acclimation_and_population_dynamics_of_green_sulfur_bacteria_grown_with_spectrally_tailored_light"><img alt="Research paper thumbnail of Chromatic acclimation and population dynamics of green sulfur bacteria grown with spectrally tailored light" class="work-thumbnail" src="https://attachments.academia-assets.com/43148414/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/22534516/Chromatic_acclimation_and_population_dynamics_of_green_sulfur_bacteria_grown_with_spectrally_tailored_light">Chromatic acclimation and population dynamics of green sulfur bacteria grown with spectrally tailored light</a></div><div class="wp-workCard_item"><span>Scientific Reports</span><span>, 2014</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Living organisms have to adjust to their surrounding in order to survive in stressful conditions....</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">Living organisms have to adjust to their surrounding in order to survive in stressful conditions. We study this mechanism in one of most primitive creatures -photosynthetic green sulfur bacteria. These bacteria absorb photons very efficiently using the chlorosome antenna complexes and perform photosynthesis in extreme low-light environments. How the chlorosomes in green sulfur bacteria are acclimated to the stressful light conditions, for instance, if the spectrum of light is not optimal for absorption, is unknown. Studying Chlorobaculum tepidum cultures with far-red to near-infrared light-emitting diodes, we found that these bacteria react to changes in energy flow by regulating the amount of light-absorbing pigments and the size of the chlorosomes. Surprisingly, our results indicate that the bacteria can survive in near-infrared lights capturing low-frequency photons by the intermediate units of the light-harvesting complex. The latter strategy may be used by the species recently found near hydrothermal vents in the Pacific Ocean.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="7a1f338a8fa2bf7a53d462ce42d2ac7c" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":43148414,"asset_id":22534516,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/43148414/download_file?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="22534516"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="22534516"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 22534516; 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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="15177647"><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/15177647/State_by_State_Investigation_of_Destructive_Interference_in_Resonance_Raman_Spectra_of_Neutral_Tyrosine_and_the_Tyrosinate_Anion_with_the_Simplified_Sum_over_States_Approach"><img alt="Research paper thumbnail of State-by-State Investigation of Destructive Interference in Resonance Raman Spectra of Neutral Tyrosine and the Tyrosinate Anion with the Simplified Sum-over-States Approach" class="work-thumbnail" src="https://attachments.academia-assets.com/43494889/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/15177647/State_by_State_Investigation_of_Destructive_Interference_in_Resonance_Raman_Spectra_of_Neutral_Tyrosine_and_the_Tyrosinate_Anion_with_the_Simplified_Sum_over_States_Approach">State-by-State Investigation of Destructive Interference in Resonance Raman Spectra of Neutral Tyrosine and the Tyrosinate Anion with the Simplified Sum-over-States Approach</a></div><div class="wp-workCard_item wp-workCard--coauthors"><span>by </span><span><a class="" data-click-track="profile-work-strip-authors" href="https://uci.academia.edu/DmitrijRappoport">Dmitrij Rappoport</a> and <a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/SemionSaikin">Semion Saikin</a></span></div><div class="wp-workCard_item"><span>The Journal of Physical Chemistry A</span><span>, 2014</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">UV resonance Raman scattering is uniquely sensitive to the molecular electronic structure as well...</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">UV resonance Raman scattering is uniquely sensitive to the molecular electronic structure as well as intermolecular interactions. To better understand the relationship between electronic structure and resonance Raman cross section, we carried out combined experimental and theoretical studies of neutral tyrosine and the tyrosinate anion. We studied the Raman cross sections of four vibrational modes as a function of excitation wavelength, and we analyzed them in terms of the contributions of the individual electronic states as well as of the Albrecht A and B terms. Our model, which is based on time-dependent density functional theory (TDDFT), reproduced the experimental resonance Raman spectra and Raman excitation profiles for both studied molecules with good agreement. We found that for the studied modes, the contributions of Albrecht's B terms in the Raman cross sections were important across the frequency range spanning the L a,b and B a,b electronic excitations in tyrosine and the tyrosinate anion. Furthermore, we demonstrated that interference with high-energy states had a significant impact and could not be neglected even when in resonance with a lower-energy state. The symmetry of the vibrational modes served as an indicator of the dominance of the A or B mechanisms. Excitation profiles calculated with a damping constant estimated from line widths of the electronic absorption bands had the best consistency with experimental results.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="fccfba6fb8989b10f6b8b6d1c64293b6" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":43494889,"asset_id":15177647,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/43494889/download_file?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="15177647"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="15177647"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 15177647; 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dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "fccfba6fb8989b10f6b8b6d1c64293b6" } } $('.js-work-strip[data-work-id=15177647]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":15177647,"title":"State-by-State Investigation of Destructive Interference in Resonance Raman Spectra of Neutral Tyrosine and the Tyrosinate Anion with the Simplified Sum-over-States Approach","internal_url":"https://www.academia.edu/15177647/State_by_State_Investigation_of_Destructive_Interference_in_Resonance_Raman_Spectra_of_Neutral_Tyrosine_and_the_Tyrosinate_Anion_with_the_Simplified_Sum_over_States_Approach","owner_id":34230121,"coauthors_can_edit":true,"owner":{"id":34230121,"first_name":"Dmitrij","middle_initials":null,"last_name":"Rappoport","page_name":"DmitrijRappoport","domain_name":"uci","created_at":"2015-08-25T13:25:03.239-07:00","display_name":"Dmitrij Rappoport","url":"https://uci.academia.edu/DmitrijRappoport"},"attachments":[{"id":43494889,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/43494889/thumbnails/1.jpg","file_name":"A_State-by-state_Investigation_of_Destru20160308-29480-1c6ux5m.pdf","download_url":"https://www.academia.edu/attachments/43494889/download_file","bulk_download_file_name":"State_by_State_Investigation_of_Destruct.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/43494889/A_State-by-state_Investigation_of_Destru20160308-29480-1c6ux5m-libre.pdf?1457429396=\u0026response-content-disposition=attachment%3B+filename%3DState_by_State_Investigation_of_Destruct.pdf\u0026Expires=1740957552\u0026Signature=bS~jS27OH5maqS17oc~ql2xVLEX4CP7Pugsbqd8QI~httV9tSepm4pCeWfPJI8F3kPAeCoFCQP-VR2oStMtWeLu4IOxiLhP59RWCNLk1RrgCwBQSGjyWuiWdWeNDOVycePLYlWyq5zV8D8ldNvKQzf480xNHtYr~dAgutBQJGoSe7BPa29AxyDyk5aIbBYKoU8ENYBruSCTUu0EbLTNrP6sJqY1SVZBOJGAT6RM0qDHwPAOvYuxT-LKpNJe1g-7vzeL0sy36CzPSVp81yCW-YapRpUOz6cuv5ZU1LuFB1t6~zdzNAKU2l9wyKIgU7gYtwepfltpVl7xbglsbyKniwQ__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}]}, 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="22534515"><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/22534515/Isotopic_disorder_in_Ge_single_crystals_probed_with_Ge_73_NMR"><img alt="Research paper thumbnail of Isotopic disorder in Ge single crystals probed with Ge-73 NMR" class="work-thumbnail" src="https://attachments.academia-assets.com/43148410/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/22534515/Isotopic_disorder_in_Ge_single_crystals_probed_with_Ge_73_NMR">Isotopic disorder in Ge single crystals probed with Ge-73 NMR</a></div><div class="wp-workCard_item wp-workCard--coauthors"><span>by </span><span><a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/SemionSaikin">Semion Saikin</a>, <a class="" data-click-track="profile-work-strip-authors" href="https://kpfu.academia.edu/BMalkin">B. Malkin</a>, <a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/AYakubovsky">A. Yakubovsky</a>, and <a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/SVerkhovskii">S. Verkhovskii</a></span></div><div class="wp-workCard_item"><span>Physical Review B</span><span>, 2003</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">NMR spectra of 73 Ge (nuclear spin I = 9/2) in germanium single crystals with different isotopic ...</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">NMR spectra of 73 Ge (nuclear spin I = 9/2) in germanium single crystals with different isotopic compositions have been measured at the frequency of 17.4 MHz at room temperature. Due to the small concentration (~0.1%) of the magnetic ( 73 Ge) isotope, the magnetic dipole-dipole interaction is negligible in the samples studied, and the observed specific features of the resonance lineshapes (a narrow central peak and a wide plateau) are determined mainly by the quadrupole interaction of magnetic nuclei with the random electric field gradient (EFG) induced by the isotopic disorder. The second and fourth moments of the distribution function of the EFG are calculated taking into account local lattice deformations due to mass defects in the close neighborhood of the magnetic nuclei, as well as charge density redistributions and lattice strains induced by distant impurity isotopes. The simulated lineshapes, represented by a superposition of Gaussians corresponding to individual transitions between nuclear Zeeman sublevels, agree reasonably well with the measured spectra. 76.60.K, 76.60 Gv, 76.60.Es</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="f56e2e7dab113c952c2d8251b6282a4f" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":43148410,"asset_id":22534515,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/43148410/download_file?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="22534515"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="22534515"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 22534515; 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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="22534514"><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/22534514/Quantum_Nonlinear_Optics_with_Polar_J_Aggregates_in_Microcavities"><img alt="Research paper thumbnail of Quantum Nonlinear Optics with Polar J-Aggregates in Microcavities" class="work-thumbnail" src="https://attachments.academia-assets.com/43148417/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/22534514/Quantum_Nonlinear_Optics_with_Polar_J_Aggregates_in_Microcavities">Quantum Nonlinear Optics with Polar J-Aggregates in Microcavities</a></div><div class="wp-workCard_item"><span>The Journal of Physical Chemistry Letters</span><span>, 2014</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">We show that an ensemble of organic dye molecules with permanent electric dipole moments embedded...</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">We show that an ensemble of organic dye molecules with permanent electric dipole moments embedded in a microcavity can lead to strong optical nonlinearities at the single photon level. The strong long-range electrostatic interaction between chromophores due to their permanent dipoles introduces the desired nonlinearity of the light-matter coupling in the microcavity. We obtain the absorption spectra of a weak probe field under the influence of strong exciton-photon coupling with the cavity field. Using realistic parameters, we demonstrate that a single cavity photon can significantly modify the absorptive and dispersive response of the medium to a probe photon at a different frequency. Finally, we show that the system is in the regime of cavity-induced transparency with a broad transparency window for dye dimers. We illustrate our findings using pseudoisocyanine chloride (PIC) J-aggregates in currently-available optical microcavities.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="6ede18f2b9227bea03b9cfed3b75c4cc" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":43148417,"asset_id":22534514,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/43148417/download_file?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="22534514"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="22534514"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 22534514; 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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="22534513"><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/22534513/Fast_initialization_of_the_spin_state_of_an_electron_in_a_quantum_dot_in_the_voigt_configuration"><img alt="Research paper thumbnail of Fast initialization of the spin state of an electron in a quantum dot in the voigt configuration" class="work-thumbnail" src="https://attachments.academia-assets.com/43148430/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/22534513/Fast_initialization_of_the_spin_state_of_an_electron_in_a_quantum_dot_in_the_voigt_configuration">Fast initialization of the spin state of an electron in a quantum dot in the voigt configuration</a></div><div class="wp-workCard_item"><span>Physical Review Letters</span><span>, 2007</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">We consider the initialization of the spin-state of a single electron trapped in a self-assembled...</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">We consider the initialization of the spin-state of a single electron trapped in a self-assembled quantum dot via optical pumping of a trion level. We show that with a magnetic field applied perpendicular to the growth direction of the dot, a near-unity fidelity can be obtained in a time equal to a few times the inverse of the spin-conserving trion relaxation rate. This method is several orders-of-magnitude faster than with the field aligned parallel, since this configuration must rely on a slow hole spin-flip mechanism. This increase in speed does result in a limit on the maximum obtainable fidelity, but we show that for InAs dots, the error is very small.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="0d4bc507230fd369713df85f31e2a046" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":43148430,"asset_id":22534513,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/43148430/download_file?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="22534513"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="22534513"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 22534513; 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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="22534512"><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/22534512/The_nucleus_of_endothelial_cell_as_a_sensor_of_blood_flow_direction"><img alt="Research paper thumbnail of The nucleus of endothelial cell as a sensor of blood flow direction" class="work-thumbnail" src="https://attachments.academia-assets.com/43148407/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/22534512/The_nucleus_of_endothelial_cell_as_a_sensor_of_blood_flow_direction">The nucleus of endothelial cell as a sensor of blood flow direction</a></div><div class="wp-workCard_item wp-workCard--coauthors"><span>by </span><span><a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/AlexGroisman">Alex Groisman</a> and <a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/SemionSaikin">Semion Saikin</a></span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Hemodynamic shear stresses cause endothelial cells (ECs) to polarize in the plane of the flow. Pa...</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">Hemodynamic shear stresses cause endothelial cells (ECs) to polarize in the plane of the flow. Paradoxically, under strong shear flows, ECs disassemble their primary cilia, common sensors of shear, and thus must use an alternative mechanism of sensing the strength and direction of flow. In our experiments in microfluidic perfusion chambers, confluent ECs developed planar cell polarity at a rate proportional to the shear stress. The location of Golgi apparatus and microtubule organizing center was biased to the upstream side of the nucleus, i.e. the ECs polarized against the flow. These in vitro results agreed with observations in murine blood vessels, where EC polarization against the flow was stronger in high flow arteries than in veins. Once established, flow-induced polarization persisted over long time intervals without external shear. Transient destabilization of actomyosin cytoskeleton by inhibition of myosin II or depolymerization of actin promoted polarization of EC against the flow, indicating that an intact acto-myosin cytoskeleton resists flow-induced polarization. These results suggested that polarization was induced by mechanical displacement of EC nuclei downstream under the hydrodynamic drag. This hypothesis was confirmed by the observation that acute application of a large hydrodynamic force to ECs resulted in an immediate downstream displacement of nuclei and was sufficient to induce persistent polarization. Taken together, our data indicate that ECs can sense the direction and strength of blood flow through the hydrodynamic drag applied to their nuclei.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="4489e81dafaf6fae531d35c2ac82b2eb" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":43148407,"asset_id":22534512,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/43148407/download_file?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="22534512"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="22534512"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 22534512; 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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="22534511"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/22534511/System_bath_approach_to_electronic_effect_in_Surface_Enhanced_Raman_Scattering"><img alt="Research paper thumbnail of System-bath approach to electronic effect in Surface Enhanced Raman Scattering" 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" rel="nofollow" href="https://www.academia.edu/22534511/System_bath_approach_to_electronic_effect_in_Surface_Enhanced_Raman_Scattering">System-bath approach to electronic effect in Surface Enhanced Raman Scattering</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Raman scattering from molecules is greatly enhanced in proximity of a metal nanoparticle or a rou...</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">Raman scattering from molecules is greatly enhanced in proximity of a metal nanoparticle or a rough metal surface. The strong interest in this effect is driven by applications to selective detection of toxic chemicals, warfare agents, etc. The scattering enhancement has two distinct contributions. The electromagnetic effect originates in the field concentration by surface plasmons excited in the metal. The</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="22534511"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="22534511"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 22534511; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=22534511]").text(description); $(".js-view-count[data-work-id=22534511]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 22534511; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='22534511']"); 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></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-a9bf3a2bc8c89fa2a77156577594264ee8a0f214d74241bc0fcd3f69f8d107ac.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" } } $('.js-work-strip[data-work-id=22534511]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":22534511,"title":"System-bath approach to electronic effect in Surface Enhanced Raman Scattering","internal_url":"https://www.academia.edu/22534511/System_bath_approach_to_electronic_effect_in_Surface_Enhanced_Raman_Scattering","owner_id":44056208,"coauthors_can_edit":true,"owner":{"id":44056208,"first_name":"Semion","middle_initials":null,"last_name":"Saikin","page_name":"SemionSaikin","domain_name":"independent","created_at":"2016-02-27T17:30:43.004-08:00","display_name":"Semion Saikin","url":"https://independent.academia.edu/SemionSaikin"},"attachments":[]}, 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="22534510"><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/22534510/Strong_coupling_between_chlorosomes_of_photosynthetic_bacteria_and_a_confined_optical_cavity_mode"><img alt="Research paper thumbnail of Strong coupling between chlorosomes of photosynthetic bacteria and a confined optical cavity mode" class="work-thumbnail" src="https://attachments.academia-assets.com/43148408/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/22534510/Strong_coupling_between_chlorosomes_of_photosynthetic_bacteria_and_a_confined_optical_cavity_mode">Strong coupling between chlorosomes of photosynthetic bacteria and a confined optical cavity mode</a></div><div class="wp-workCard_item"><span>Nature communications</span><span>, 2014</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Strong exciton-photon coupling is the result of a reversible exchange of energy between an excite...</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">Strong exciton-photon coupling is the result of a reversible exchange of energy between an excited state and a confined optical field. This results in the formation of polariton states that have energies different from the exciton and photon. We demonstrate strong exciton-photon coupling between light-harvesting complexes and a confined optical mode within a metallic optical microcavity. The energetic anti-crossing between the exciton and photon dispersions characteristic of strong coupling is observed in reflectivity and transmission with a Rabi splitting energy on the order of 150 meV, which corresponds to about 1,000 chlorosomes coherently coupled to the cavity mode. We believe that the strong coupling regime presents an opportunity to modify the energy transfer pathways within photosynthetic organisms without modification of the molecular structure.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="57f8221de0058b0a88f54ad5a60d0163" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":43148408,"asset_id":22534510,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/43148408/download_file?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="22534510"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="22534510"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 22534510; 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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="22534509"><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/22534509/Photonics_meets_excitonics_natural_and_artificial_molecular_aggregates"><img alt="Research paper thumbnail of Photonics meets excitonics: natural and artificial molecular aggregates" class="work-thumbnail" src="https://attachments.academia-assets.com/43148429/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/22534509/Photonics_meets_excitonics_natural_and_artificial_molecular_aggregates">Photonics meets excitonics: natural and artificial molecular aggregates</a></div><div class="wp-workCard_item"><span>Nanophotonics</span><span>, 2013</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Organic molecules store the energy of absorbed light in the form of charge-neutral molecular exci...</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">Organic molecules store the energy of absorbed light in the form of charge-neutral molecular excitations -Frenkel excitons. Usually, in amorphous organic materials, excitons are viewed as quasiparticles, localized on single molecules, which diffuse randomly through the structure. However, the picture of incoherent hopping is not applicable to some classes of molecular aggregatesassemblies of molecules that have strong near field interaction between electronic excitations in the individual subunits. Molecular aggregates can be found in nature, in photosynthetic complexes of plants and bacteria, and they can also be produced artificially in various forms including quasi-one dimensional chains, two-dimensional films, tubes, etc. In these structures light is absorbed collectively by many molecules and the following dynamics of molecular excitation possesses coherent properties. This energy transfer mechanism, mediated by the coherent exciton dynamics, resembles the propagation of electromagnetic waves through a structured medium on the nanometer scale. The absorbed energy can be transferred resonantly over distances of hundreds of nanometers before exciton relaxation occurs. Furthermore, the spatial and energetic landscape of molecular aggregates can enable the funneling of the exciton energy to a small number of molecules either within or outside the aggregate. In this review we establish a bridge between the fields of photonics and excitonics by describing the present understanding of exciton dynamics in molecular aggregates. * Electronic address: <a href="mailto:saykin@fas.harvard.edu" rel="nofollow">saykin@fas.harvard.edu</a> † Electronic address: <a href="mailto:eisfeld@mpipks-dresden.mpg.de" rel="nofollow">eisfeld@mpipks-dresden.mpg.de</a> ‡ Electronic address: <a href="mailto:aspuru@chemistry.harvard.edu" rel="nofollow">aspuru@chemistry.harvard.edu</a> 1 E. Yablonovitch; Inhibited Spontaneous Emission in</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="c4acc5f5dc855aa507c0116736e22b8a" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":43148429,"asset_id":22534509,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/43148429/download_file?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="22534509"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="22534509"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 22534509; 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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="4702108" id="papers"><div class="js-work-strip profile--work_container" data-work-id="22534531"><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/22534531/Semiclassical_Transport_Models_for_Semiconductor_Spintronics"><img alt="Research paper thumbnail of Semiclassical Transport Models for Semiconductor Spintronics" class="work-thumbnail" src="https://attachments.academia-assets.com/43148409/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/22534531/Semiclassical_Transport_Models_for_Semiconductor_Spintronics">Semiclassical Transport Models for Semiconductor Spintronics</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">We will summarize and consider several examples of applications of semiclassi- cal approaches use...</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">We will summarize and consider several examples of applications of semiclassi- cal approaches used in semiconductor spintronic device modeling. These include drift-diffusion models, kinetic transport equations and Monte Carlo simulation schemes.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="f1d1965511294760e300bfaa793675c5" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":43148409,"asset_id":22534531,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/43148409/download_file?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="22534531"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="22534531"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 22534531; 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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="22534529"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/22534529/Spin_polarized_transport_modeling"><img alt="Research paper thumbnail of Spin-polarized transport modeling" 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" rel="nofollow" href="https://www.academia.edu/22534529/Spin_polarized_transport_modeling">Spin-polarized transport modeling</a></div><div class="wp-workCard_item wp-workCard--coauthors"><span>by </span><span><a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/VladimirPrivman">Vladimir Privman</a> and <a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/SemionSaikin">Semion Saikin</a></span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">The emerging field of semiconductor spintronics promises to utilize spin degree of freedom in ele...</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">The emerging field of semiconductor spintronics promises to utilize spin degree of freedom in electronic device operation. In order to understand advantages and limitations of proposed spintronic devices, realistic models for spin-polarized transport in device structures are needed. We study spin-polarized electron transport properties in semiconductor non-magnetic heterostructures where electron spin dynamics is controlled by a spin-orbit interaction. Two complementary</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="22534529"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="22534529"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 22534529; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=22534529]").text(description); $(".js-view-count[data-work-id=22534529]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 22534529; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='22534529']"); 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></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-a9bf3a2bc8c89fa2a77156577594264ee8a0f214d74241bc0fcd3f69f8d107ac.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" } } $('.js-work-strip[data-work-id=22534529]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":22534529,"title":"Spin-polarized transport modeling","internal_url":"https://www.academia.edu/22534529/Spin_polarized_transport_modeling","owner_id":44056208,"coauthors_can_edit":true,"owner":{"id":44056208,"first_name":"Semion","middle_initials":null,"last_name":"Saikin","page_name":"SemionSaikin","domain_name":"independent","created_at":"2016-02-27T17:30:43.004-08:00","display_name":"Semion Saikin","url":"https://independent.academia.edu/SemionSaikin"},"attachments":[]}, 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="22534525"><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/22534525/Spin_polarized_transport_in_semiconductor_nanostructures"><img alt="Research paper thumbnail of Spin-polarized transport in semiconductor nanostructures" class="work-thumbnail" src="https://attachments.academia-assets.com/43148422/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/22534525/Spin_polarized_transport_in_semiconductor_nanostructures">Spin-polarized transport in semiconductor nanostructures</a></div><div class="wp-workCard_item wp-workCard--coauthors"><span>by </span><span><a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/VladimirPrivman">Vladimir Privman</a> and <a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/SemionSaikin">Semion Saikin</a></span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">We study spin polarization patterns in semiconductor nanostructures produced by stationary inject...</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">We study spin polarization patterns in semiconductor nanostructures produced by stationary injected spin-polarized electrons using the Monte Carlo device simulation scheme. Spatial transport affects the spin polarization by means of a spin-orbit interaction. Effects of the applied electric field along the transport direction, temperature, non-parabolicity of conduction band and anisotropy of the spin-orbit interaction are considered. We compare the simulated</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="45ba76b8a43dfd47dcbc336982d411c4" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":43148422,"asset_id":22534525,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/43148422/download_file?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="22534525"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="22534525"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 22534525; 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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="22534523"><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/22534523/Monte_Carlo_Modeling_of_Spin_FETs_Controlled_by_Spin_Orbit_Interaction"><img alt="Research paper thumbnail of Monte Carlo Modeling of Spin FETs Controlled by Spin-Orbit Interaction" class="work-thumbnail" src="https://attachments.academia-assets.com/43148428/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/22534523/Monte_Carlo_Modeling_of_Spin_FETs_Controlled_by_Spin_Orbit_Interaction">Monte Carlo Modeling of Spin FETs Controlled by Spin-Orbit Interaction</a></div><div class="wp-workCard_item wp-workCard--coauthors"><span>by </span><span><a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/VladimirPrivman">Vladimir Privman</a> and <a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/SemionSaikin">Semion Saikin</a></span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">A method for Monte Carlo simulation of 2D spin-polarized electron transport in III-V semiconducto...</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">A method for Monte Carlo simulation of 2D spin-polarized electron transport in III-V semiconductor heterojunction FETs is presented. In the simulation, the dynamics of the electrons in coordinate and momentum space is treated semiclassically. The density matrix description of the spin is incorporated in the Monte Carlo method to account for the spin polarization dynamics. The spin-orbit interaction in the</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="63948f826bc766ba28c8111361e36be5" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":43148428,"asset_id":22534523,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/43148428/download_file?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="22534523"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="22534523"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 22534523; 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We show that detailed information concerning energy transfer paths and delocalization of exciton states can be inferred (and exciton energies estimated) from the statistical properties of the emitted photons. This approach provides us with a novel spectroscopic tool for</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="f8bf19799477bd031bea452876f6858c" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":43148372,"asset_id":22534522,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/43148372/download_file?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="22534522"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="22534522"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 22534522; 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$(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="22534521"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/22534521/Simulation_of_spin_polarized_transport_in_submicrometer_device_structures"><img alt="Research paper thumbnail of Simulation of spin-polarized transport in submicrometer device structures" 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" rel="nofollow" href="https://www.academia.edu/22534521/Simulation_of_spin_polarized_transport_in_submicrometer_device_structures">Simulation of spin-polarized transport in submicrometer device structures</a></div><div class="wp-workCard_item wp-workCard--coauthors"><span>by </span><span><a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/VladimirPrivman">Vladimir Privman</a> and <a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/SemionSaikin">Semion Saikin</a></span></div><div class="wp-workCard_item"><span>2003 Third IEEE Conference on Nanotechnology, 2003. IEEE-NANO 2003.</span><span>, 2003</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">The Monte Carlo approach is utilized to study spin-polarized electron transport in spintronic dev...</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">The Monte Carlo approach is utilized to study spin-polarized electron transport in spintronic device structures. Evolution of the electron spin polarization vector is controlled by the spin-orbit interaction. Spin polarization properties, including the spin-dephasing length and orientation of the polarization vector, are investigated, for the applied voltage from 0.05 V to 0.25 V, and for temperatures ranging from 77 K</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="22534521"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="22534521"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 22534521; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); 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dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=22534521]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":22534521,"title":"Simulation of spin-polarized transport in submicrometer device structures","internal_url":"https://www.academia.edu/22534521/Simulation_of_spin_polarized_transport_in_submicrometer_device_structures","owner_id":44056208,"coauthors_can_edit":true,"owner":{"id":44056208,"first_name":"Semion","middle_initials":null,"last_name":"Saikin","page_name":"SemionSaikin","domain_name":"independent","created_at":"2016-02-27T17:30:43.004-08:00","display_name":"Semion Saikin","url":"https://independent.academia.edu/SemionSaikin"},"attachments":[]}, 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="22534520"><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/22534520/Monte_Carlo_Simulation_of_Spin_Polarized_Transport"><img alt="Research paper thumbnail of Monte Carlo Simulation of Spin-Polarized Transport" class="work-thumbnail" src="https://attachments.academia-assets.com/43148425/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/22534520/Monte_Carlo_Simulation_of_Spin_Polarized_Transport">Monte Carlo Simulation of Spin-Polarized Transport</a></div><div class="wp-workCard_item wp-workCard--coauthors"><span>by </span><span><a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/VladimirPrivman">Vladimir Privman</a> and <a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/SemionSaikin">Semion Saikin</a></span></div><div class="wp-workCard_item"><span>Lecture Notes in Computer Science</span><span>, 2003</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Monte Carlo simulations are performed to study the in-plane transport of spin-polarized electrons...</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">Monte Carlo simulations are performed to study the in-plane transport of spin-polarized electrons in III-V semiconductor quantum wells. The density matrix description of the spin polarization is incorporated in the simulation algorithm. The spin-orbit interaction terms generate coherent evolution of the electron spin polarization and also cause dephasing. The spatial motion of the electrons is treated semiclassically. Three different scattering mechanisms-optical phonons, acoustic phonons and ionized impurities-are considered. The electric field is calculated self-consistently from the charge distribution. The Monte Carlo scheme is described, and simulation results are reported for temperatures in the range 77-300 K.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="ff722c121e7077304c8d2c38036e3671" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":43148425,"asset_id":22534520,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/43148425/download_file?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="22534520"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="22534520"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 22534520; 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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="22534519"><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/22534519/Fast_Delocalization_Leads_To_Robust_Long_Range_Excitonic_Transfer_in_a_Large_Quantum_Chlorosome_Model"><img alt="Research paper thumbnail of Fast Delocalization Leads To Robust Long-Range Excitonic Transfer in a Large Quantum Chlorosome Model" class="work-thumbnail" src="https://attachments.academia-assets.com/43148426/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/22534519/Fast_Delocalization_Leads_To_Robust_Long_Range_Excitonic_Transfer_in_a_Large_Quantum_Chlorosome_Model">Fast Delocalization Leads To Robust Long-Range Excitonic Transfer in a Large Quantum Chlorosome Model</a></div><div class="wp-workCard_item"><span>Nano Letters</span><span>, 2015</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Chlorosomes are efficient light-harvesting antennas containing up to hundreds of thousands of bac...</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">Chlorosomes are efficient light-harvesting antennas containing up to hundreds of thousands of bacteriochlorophyll molecules. With massively parallel computer hardware, we use a nonperturbative stochastic Schrodinger equation, while including an atomistically derived spectral density, to study excitonic energy transfer in a realistically sized chlorosome model. We find that fast short-range delocalization leads to robust long-range transfer due to the antennae's concentric-roll structure. Additionally, we discover anomalous behavior arising from different initial conditions, and outline general considerations for simulating excitonic systems on the nanometer to micrometer scale.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="a51b8cfc4b401904f333cbfaf957136c" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":43148426,"asset_id":22534519,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/43148426/download_file?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="22534519"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="22534519"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 22534519; 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</script> <div class="js-work-strip profile--work_container" data-work-id="15177655"><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/15177655/Quantum_chemistry_calculations_for_arbitrarily_complex_electrostatic_environments"><img alt="Research paper thumbnail of Quantum chemistry calculations for arbitrarily complex electrostatic environments" class="work-thumbnail" src="https://attachments.academia-assets.com/43494892/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/15177655/Quantum_chemistry_calculations_for_arbitrarily_complex_electrostatic_environments">Quantum chemistry calculations for arbitrarily complex electrostatic environments</a></div><div class="wp-workCard_item wp-workCard--coauthors"><span>by </span><span><a class="" data-click-track="profile-work-strip-authors" href="https://uci.academia.edu/DmitrijRappoport">Dmitrij Rappoport</a> and <a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/SemionSaikin">Semion Saikin</a></span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Modeling of electronic structure of molecules in electrostatic environments is of considerable re...</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">Modeling of electronic structure of molecules in electrostatic environments is of considerable relevance for surface-enhanced spectroscopy and molecular electronics. We have developed and implemented a novel approach to the molecular electronic structure in arbitrary electrostatic environments that is compatible with standard quantum chemical methods and can be applied to mediumsized and large molecules. The scheme denoted CheESE (chemistry in electrostatic environments) is based on the description of molecular electronic structure subject to a boundary condition on the system/environment interface. Thus, it is particularly suited to study molecules on metallic surfaces. The proposed model is capable of describing both electrostatic effects near nanostructured metallic surfaces and image-charge effects. We present an implementation of the CheESE model as a library module and show example applications to neutral and negatively charged molecules.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="0247c8c2a520d3ca63c23702d3fc5553" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":43494892,"asset_id":15177655,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/43494892/download_file?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="15177655"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="15177655"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 15177655; 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$(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="22534517"><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/22534517/Topologically_protected_excitons_in_porphyrin_thin_films"><img alt="Research paper thumbnail of Topologically protected excitons in porphyrin thin films" class="work-thumbnail" src="https://attachments.academia-assets.com/43148420/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/22534517/Topologically_protected_excitons_in_porphyrin_thin_films">Topologically protected excitons in porphyrin thin films</a></div><div class="wp-workCard_item"><span>Nature Materials</span><span>, 2014</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">The control of exciton transport in organic materials is of fundamental importance for the develo...</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">The control of exciton transport in organic materials is of fundamental importance for the development of efficient light-harvesting systems. This transport is easily deteriorated by traps in the disordered energy landscape.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="70c2e906797ed5784c5637f59582a4ef" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":43148420,"asset_id":22534517,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/43148420/download_file?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="22534517"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="22534517"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 22534517; 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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="22534516"><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/22534516/Chromatic_acclimation_and_population_dynamics_of_green_sulfur_bacteria_grown_with_spectrally_tailored_light"><img alt="Research paper thumbnail of Chromatic acclimation and population dynamics of green sulfur bacteria grown with spectrally tailored light" class="work-thumbnail" src="https://attachments.academia-assets.com/43148414/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/22534516/Chromatic_acclimation_and_population_dynamics_of_green_sulfur_bacteria_grown_with_spectrally_tailored_light">Chromatic acclimation and population dynamics of green sulfur bacteria grown with spectrally tailored light</a></div><div class="wp-workCard_item"><span>Scientific Reports</span><span>, 2014</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Living organisms have to adjust to their surrounding in order to survive in stressful conditions....</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">Living organisms have to adjust to their surrounding in order to survive in stressful conditions. We study this mechanism in one of most primitive creatures -photosynthetic green sulfur bacteria. These bacteria absorb photons very efficiently using the chlorosome antenna complexes and perform photosynthesis in extreme low-light environments. How the chlorosomes in green sulfur bacteria are acclimated to the stressful light conditions, for instance, if the spectrum of light is not optimal for absorption, is unknown. Studying Chlorobaculum tepidum cultures with far-red to near-infrared light-emitting diodes, we found that these bacteria react to changes in energy flow by regulating the amount of light-absorbing pigments and the size of the chlorosomes. Surprisingly, our results indicate that the bacteria can survive in near-infrared lights capturing low-frequency photons by the intermediate units of the light-harvesting complex. The latter strategy may be used by the species recently found near hydrothermal vents in the Pacific Ocean.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="7a1f338a8fa2bf7a53d462ce42d2ac7c" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":43148414,"asset_id":22534516,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/43148414/download_file?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="22534516"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="22534516"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 22534516; 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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="15177647"><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/15177647/State_by_State_Investigation_of_Destructive_Interference_in_Resonance_Raman_Spectra_of_Neutral_Tyrosine_and_the_Tyrosinate_Anion_with_the_Simplified_Sum_over_States_Approach"><img alt="Research paper thumbnail of State-by-State Investigation of Destructive Interference in Resonance Raman Spectra of Neutral Tyrosine and the Tyrosinate Anion with the Simplified Sum-over-States Approach" class="work-thumbnail" src="https://attachments.academia-assets.com/43494889/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/15177647/State_by_State_Investigation_of_Destructive_Interference_in_Resonance_Raman_Spectra_of_Neutral_Tyrosine_and_the_Tyrosinate_Anion_with_the_Simplified_Sum_over_States_Approach">State-by-State Investigation of Destructive Interference in Resonance Raman Spectra of Neutral Tyrosine and the Tyrosinate Anion with the Simplified Sum-over-States Approach</a></div><div class="wp-workCard_item wp-workCard--coauthors"><span>by </span><span><a class="" data-click-track="profile-work-strip-authors" href="https://uci.academia.edu/DmitrijRappoport">Dmitrij Rappoport</a> and <a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/SemionSaikin">Semion Saikin</a></span></div><div class="wp-workCard_item"><span>The Journal of Physical Chemistry A</span><span>, 2014</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">UV resonance Raman scattering is uniquely sensitive to the molecular electronic structure as well...</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">UV resonance Raman scattering is uniquely sensitive to the molecular electronic structure as well as intermolecular interactions. To better understand the relationship between electronic structure and resonance Raman cross section, we carried out combined experimental and theoretical studies of neutral tyrosine and the tyrosinate anion. We studied the Raman cross sections of four vibrational modes as a function of excitation wavelength, and we analyzed them in terms of the contributions of the individual electronic states as well as of the Albrecht A and B terms. Our model, which is based on time-dependent density functional theory (TDDFT), reproduced the experimental resonance Raman spectra and Raman excitation profiles for both studied molecules with good agreement. We found that for the studied modes, the contributions of Albrecht's B terms in the Raman cross sections were important across the frequency range spanning the L a,b and B a,b electronic excitations in tyrosine and the tyrosinate anion. Furthermore, we demonstrated that interference with high-energy states had a significant impact and could not be neglected even when in resonance with a lower-energy state. The symmetry of the vibrational modes served as an indicator of the dominance of the A or B mechanisms. Excitation profiles calculated with a damping constant estimated from line widths of the electronic absorption bands had the best consistency with experimental results.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="fccfba6fb8989b10f6b8b6d1c64293b6" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":43494889,"asset_id":15177647,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/43494889/download_file?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="15177647"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="15177647"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 15177647; 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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="22534515"><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/22534515/Isotopic_disorder_in_Ge_single_crystals_probed_with_Ge_73_NMR"><img alt="Research paper thumbnail of Isotopic disorder in Ge single crystals probed with Ge-73 NMR" class="work-thumbnail" src="https://attachments.academia-assets.com/43148410/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/22534515/Isotopic_disorder_in_Ge_single_crystals_probed_with_Ge_73_NMR">Isotopic disorder in Ge single crystals probed with Ge-73 NMR</a></div><div class="wp-workCard_item wp-workCard--coauthors"><span>by </span><span><a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/SemionSaikin">Semion Saikin</a>, <a class="" data-click-track="profile-work-strip-authors" href="https://kpfu.academia.edu/BMalkin">B. Malkin</a>, <a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/AYakubovsky">A. Yakubovsky</a>, and <a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/SVerkhovskii">S. Verkhovskii</a></span></div><div class="wp-workCard_item"><span>Physical Review B</span><span>, 2003</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">NMR spectra of 73 Ge (nuclear spin I = 9/2) in germanium single crystals with different isotopic ...</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">NMR spectra of 73 Ge (nuclear spin I = 9/2) in germanium single crystals with different isotopic compositions have been measured at the frequency of 17.4 MHz at room temperature. Due to the small concentration (~0.1%) of the magnetic ( 73 Ge) isotope, the magnetic dipole-dipole interaction is negligible in the samples studied, and the observed specific features of the resonance lineshapes (a narrow central peak and a wide plateau) are determined mainly by the quadrupole interaction of magnetic nuclei with the random electric field gradient (EFG) induced by the isotopic disorder. The second and fourth moments of the distribution function of the EFG are calculated taking into account local lattice deformations due to mass defects in the close neighborhood of the magnetic nuclei, as well as charge density redistributions and lattice strains induced by distant impurity isotopes. The simulated lineshapes, represented by a superposition of Gaussians corresponding to individual transitions between nuclear Zeeman sublevels, agree reasonably well with the measured spectra. 76.60.K, 76.60 Gv, 76.60.Es</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="f56e2e7dab113c952c2d8251b6282a4f" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":43148410,"asset_id":22534515,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/43148410/download_file?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="22534515"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="22534515"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 22534515; 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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="22534514"><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/22534514/Quantum_Nonlinear_Optics_with_Polar_J_Aggregates_in_Microcavities"><img alt="Research paper thumbnail of Quantum Nonlinear Optics with Polar J-Aggregates in Microcavities" class="work-thumbnail" src="https://attachments.academia-assets.com/43148417/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/22534514/Quantum_Nonlinear_Optics_with_Polar_J_Aggregates_in_Microcavities">Quantum Nonlinear Optics with Polar J-Aggregates in Microcavities</a></div><div class="wp-workCard_item"><span>The Journal of Physical Chemistry Letters</span><span>, 2014</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">We show that an ensemble of organic dye molecules with permanent electric dipole moments embedded...</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">We show that an ensemble of organic dye molecules with permanent electric dipole moments embedded in a microcavity can lead to strong optical nonlinearities at the single photon level. The strong long-range electrostatic interaction between chromophores due to their permanent dipoles introduces the desired nonlinearity of the light-matter coupling in the microcavity. We obtain the absorption spectra of a weak probe field under the influence of strong exciton-photon coupling with the cavity field. Using realistic parameters, we demonstrate that a single cavity photon can significantly modify the absorptive and dispersive response of the medium to a probe photon at a different frequency. Finally, we show that the system is in the regime of cavity-induced transparency with a broad transparency window for dye dimers. We illustrate our findings using pseudoisocyanine chloride (PIC) J-aggregates in currently-available optical microcavities.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="6ede18f2b9227bea03b9cfed3b75c4cc" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":43148417,"asset_id":22534514,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/43148417/download_file?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="22534514"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="22534514"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 22534514; 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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="22534513"><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/22534513/Fast_initialization_of_the_spin_state_of_an_electron_in_a_quantum_dot_in_the_voigt_configuration"><img alt="Research paper thumbnail of Fast initialization of the spin state of an electron in a quantum dot in the voigt configuration" class="work-thumbnail" src="https://attachments.academia-assets.com/43148430/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/22534513/Fast_initialization_of_the_spin_state_of_an_electron_in_a_quantum_dot_in_the_voigt_configuration">Fast initialization of the spin state of an electron in a quantum dot in the voigt configuration</a></div><div class="wp-workCard_item"><span>Physical Review Letters</span><span>, 2007</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">We consider the initialization of the spin-state of a single electron trapped in a self-assembled...</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">We consider the initialization of the spin-state of a single electron trapped in a self-assembled quantum dot via optical pumping of a trion level. We show that with a magnetic field applied perpendicular to the growth direction of the dot, a near-unity fidelity can be obtained in a time equal to a few times the inverse of the spin-conserving trion relaxation rate. This method is several orders-of-magnitude faster than with the field aligned parallel, since this configuration must rely on a slow hole spin-flip mechanism. This increase in speed does result in a limit on the maximum obtainable fidelity, but we show that for InAs dots, the error is very small.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="0d4bc507230fd369713df85f31e2a046" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":43148430,"asset_id":22534513,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/43148430/download_file?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="22534513"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="22534513"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 22534513; 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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="22534512"><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/22534512/The_nucleus_of_endothelial_cell_as_a_sensor_of_blood_flow_direction"><img alt="Research paper thumbnail of The nucleus of endothelial cell as a sensor of blood flow direction" class="work-thumbnail" src="https://attachments.academia-assets.com/43148407/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/22534512/The_nucleus_of_endothelial_cell_as_a_sensor_of_blood_flow_direction">The nucleus of endothelial cell as a sensor of blood flow direction</a></div><div class="wp-workCard_item wp-workCard--coauthors"><span>by </span><span><a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/AlexGroisman">Alex Groisman</a> and <a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/SemionSaikin">Semion Saikin</a></span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Hemodynamic shear stresses cause endothelial cells (ECs) to polarize in the plane of the flow. Pa...</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">Hemodynamic shear stresses cause endothelial cells (ECs) to polarize in the plane of the flow. Paradoxically, under strong shear flows, ECs disassemble their primary cilia, common sensors of shear, and thus must use an alternative mechanism of sensing the strength and direction of flow. In our experiments in microfluidic perfusion chambers, confluent ECs developed planar cell polarity at a rate proportional to the shear stress. The location of Golgi apparatus and microtubule organizing center was biased to the upstream side of the nucleus, i.e. the ECs polarized against the flow. These in vitro results agreed with observations in murine blood vessels, where EC polarization against the flow was stronger in high flow arteries than in veins. Once established, flow-induced polarization persisted over long time intervals without external shear. Transient destabilization of actomyosin cytoskeleton by inhibition of myosin II or depolymerization of actin promoted polarization of EC against the flow, indicating that an intact acto-myosin cytoskeleton resists flow-induced polarization. These results suggested that polarization was induced by mechanical displacement of EC nuclei downstream under the hydrodynamic drag. This hypothesis was confirmed by the observation that acute application of a large hydrodynamic force to ECs resulted in an immediate downstream displacement of nuclei and was sufficient to induce persistent polarization. Taken together, our data indicate that ECs can sense the direction and strength of blood flow through the hydrodynamic drag applied to their nuclei.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="4489e81dafaf6fae531d35c2ac82b2eb" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":43148407,"asset_id":22534512,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/43148407/download_file?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="22534512"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="22534512"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 22534512; 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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="22534511"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/22534511/System_bath_approach_to_electronic_effect_in_Surface_Enhanced_Raman_Scattering"><img alt="Research paper thumbnail of System-bath approach to electronic effect in Surface Enhanced Raman Scattering" 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" rel="nofollow" href="https://www.academia.edu/22534511/System_bath_approach_to_electronic_effect_in_Surface_Enhanced_Raman_Scattering">System-bath approach to electronic effect in Surface Enhanced Raman Scattering</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Raman scattering from molecules is greatly enhanced in proximity of a metal nanoparticle or a rou...</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">Raman scattering from molecules is greatly enhanced in proximity of a metal nanoparticle or a rough metal surface. The strong interest in this effect is driven by applications to selective detection of toxic chemicals, warfare agents, etc. The scattering enhancement has two distinct contributions. The electromagnetic effect originates in the field concentration by surface plasmons excited in the metal. The</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="22534511"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="22534511"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 22534511; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=22534511]").text(description); $(".js-view-count[data-work-id=22534511]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 22534511; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='22534511']"); 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></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-a9bf3a2bc8c89fa2a77156577594264ee8a0f214d74241bc0fcd3f69f8d107ac.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" } } $('.js-work-strip[data-work-id=22534511]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":22534511,"title":"System-bath approach to electronic effect in Surface Enhanced Raman Scattering","internal_url":"https://www.academia.edu/22534511/System_bath_approach_to_electronic_effect_in_Surface_Enhanced_Raman_Scattering","owner_id":44056208,"coauthors_can_edit":true,"owner":{"id":44056208,"first_name":"Semion","middle_initials":null,"last_name":"Saikin","page_name":"SemionSaikin","domain_name":"independent","created_at":"2016-02-27T17:30:43.004-08:00","display_name":"Semion Saikin","url":"https://independent.academia.edu/SemionSaikin"},"attachments":[]}, 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="22534510"><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/22534510/Strong_coupling_between_chlorosomes_of_photosynthetic_bacteria_and_a_confined_optical_cavity_mode"><img alt="Research paper thumbnail of Strong coupling between chlorosomes of photosynthetic bacteria and a confined optical cavity mode" class="work-thumbnail" src="https://attachments.academia-assets.com/43148408/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/22534510/Strong_coupling_between_chlorosomes_of_photosynthetic_bacteria_and_a_confined_optical_cavity_mode">Strong coupling between chlorosomes of photosynthetic bacteria and a confined optical cavity mode</a></div><div class="wp-workCard_item"><span>Nature communications</span><span>, 2014</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Strong exciton-photon coupling is the result of a reversible exchange of energy between an excite...</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">Strong exciton-photon coupling is the result of a reversible exchange of energy between an excited state and a confined optical field. This results in the formation of polariton states that have energies different from the exciton and photon. We demonstrate strong exciton-photon coupling between light-harvesting complexes and a confined optical mode within a metallic optical microcavity. The energetic anti-crossing between the exciton and photon dispersions characteristic of strong coupling is observed in reflectivity and transmission with a Rabi splitting energy on the order of 150 meV, which corresponds to about 1,000 chlorosomes coherently coupled to the cavity mode. We believe that the strong coupling regime presents an opportunity to modify the energy transfer pathways within photosynthetic organisms without modification of the molecular structure.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="57f8221de0058b0a88f54ad5a60d0163" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":43148408,"asset_id":22534510,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/43148408/download_file?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="22534510"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="22534510"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 22534510; 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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="22534509"><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/22534509/Photonics_meets_excitonics_natural_and_artificial_molecular_aggregates"><img alt="Research paper thumbnail of Photonics meets excitonics: natural and artificial molecular aggregates" class="work-thumbnail" src="https://attachments.academia-assets.com/43148429/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/22534509/Photonics_meets_excitonics_natural_and_artificial_molecular_aggregates">Photonics meets excitonics: natural and artificial molecular aggregates</a></div><div class="wp-workCard_item"><span>Nanophotonics</span><span>, 2013</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Organic molecules store the energy of absorbed light in the form of charge-neutral molecular exci...</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">Organic molecules store the energy of absorbed light in the form of charge-neutral molecular excitations -Frenkel excitons. Usually, in amorphous organic materials, excitons are viewed as quasiparticles, localized on single molecules, which diffuse randomly through the structure. However, the picture of incoherent hopping is not applicable to some classes of molecular aggregatesassemblies of molecules that have strong near field interaction between electronic excitations in the individual subunits. Molecular aggregates can be found in nature, in photosynthetic complexes of plants and bacteria, and they can also be produced artificially in various forms including quasi-one dimensional chains, two-dimensional films, tubes, etc. In these structures light is absorbed collectively by many molecules and the following dynamics of molecular excitation possesses coherent properties. This energy transfer mechanism, mediated by the coherent exciton dynamics, resembles the propagation of electromagnetic waves through a structured medium on the nanometer scale. The absorbed energy can be transferred resonantly over distances of hundreds of nanometers before exciton relaxation occurs. Furthermore, the spatial and energetic landscape of molecular aggregates can enable the funneling of the exciton energy to a small number of molecules either within or outside the aggregate. In this review we establish a bridge between the fields of photonics and excitonics by describing the present understanding of exciton dynamics in molecular aggregates. * Electronic address: <a href="mailto:saykin@fas.harvard.edu" rel="nofollow">saykin@fas.harvard.edu</a> † Electronic address: <a href="mailto:eisfeld@mpipks-dresden.mpg.de" rel="nofollow">eisfeld@mpipks-dresden.mpg.de</a> ‡ Electronic address: <a href="mailto:aspuru@chemistry.harvard.edu" rel="nofollow">aspuru@chemistry.harvard.edu</a> 1 E. Yablonovitch; Inhibited Spontaneous Emission in</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="c4acc5f5dc855aa507c0116736e22b8a" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":43148429,"asset_id":22534509,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/43148429/download_file?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="22534509"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="22534509"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 22534509; 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