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data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/26253163/Soldering_Chiralities_II_Non_Abelian_Case"><img alt="Research paper thumbnail of Soldering Chiralities II: Non-Abelian Case" class="work-thumbnail" src="https://attachments.academia-assets.com/46568576/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/26253163/Soldering_Chiralities_II_Non_Abelian_Case">Soldering Chiralities II: Non-Abelian Case</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">We study the non-abelian extension of the soldering process of two chiral WZW models of opposite ...</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 the non-abelian extension of the soldering process of two chiral WZW models of opposite chiralities, resulting in a (non-chiral) WZW model living in a 2D space-time with non trivial Riemanian curvature.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="dc2345dbdace19cd88d02d2d6fb180a2" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":46568576,"asset_id":26253163,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/46568576/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 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Systems</a></div><div class="wp-workCard_item"><span>Modern Physics Letters A</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">... Modern Physics Letters A (MPLA). Particles and Fields; Gravitation; Cosmology and Nuclear Phy...</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">... Modern Physics Letters A (MPLA). Particles and Fields; Gravitation; Cosmology and Nuclear Physics. ...</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="26253161"><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="26253161"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 26253161; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=26253161]").text(description); $(".js-view-count[data-work-id=26253161]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 26253161; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='26253161']"); 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" } } $('.js-work-strip[data-work-id=26253161]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":26253161,"title":"Symplectic Quantization of Constrained Systems","internal_url":"https://www.academia.edu/26253161/Symplectic_Quantization_of_Constrained_Systems","owner_id":4792753,"coauthors_can_edit":true,"owner":{"id":4792753,"first_name":"Clovis","middle_initials":null,"last_name":"Wotzasek","page_name":"ClovisWotzasek","domain_name":"ufrj","created_at":"2013-07-09T11:39:48.873-07:00","display_name":"Clovis Wotzasek","url":"https://ufrj.academia.edu/ClovisWotzasek"},"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="26253160"><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/26253160/Confinement_brane_symmetry_and_the_Julia_Toulouse_approach_for_defects_condensation"><img alt="Research paper thumbnail of Confinement, brane symmetry and the Julia-Toulouse approach for defects condensation" class="work-thumbnail" src="https://attachments.academia-assets.com/46568526/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/26253160/Confinement_brane_symmetry_and_the_Julia_Toulouse_approach_for_defects_condensation">Confinement, brane symmetry and the Julia-Toulouse approach for defects condensation</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">In this work the phenomenon of charge confinement is approached in various contexts. An universal...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">In this work the phenomenon of charge confinement is approached in various contexts. An universal criterium for the identification of this phenomenon is suggested: the so-called spontaneous breaking of the brane symmetry. This local symmetry has its most common incarnation in the Dirac string ambiguity present in the electromagnetic theory with monopoles. The spontaneous breaking of the brane symmetry means</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="a3bf7654549b14770dbd3863b05564d6" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":46568526,"asset_id":26253160,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/46568526/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="26253160"><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="26253160"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 26253160; 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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="26253159"><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/26253159/New_formulations_for_dual_equivalent_actions"><img alt="Research paper thumbnail of New formulations for dual equivalent actions" class="work-thumbnail" src="https://attachments.academia-assets.com/46568525/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/26253159/New_formulations_for_dual_equivalent_actions">New formulations for dual equivalent actions</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">New actions in D=2 and D=3 are proposed that are dual equivalent to known theories displaying wel...</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">New actions in D=2 and D=3 are proposed that are dual equivalent to known theories displaying well defined chirality and helicity, respectively, along with a new interpolating action that maps continuously through the original dualities. The new chiral action in D=2 is a second-order theory displaying the chiral constraint dynamically while in D=3 the helicity constraint is imposed a la</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="157231ca0c38352613d15378adf3c906" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":46568525,"asset_id":26253159,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/46568525/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="26253159"><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="26253159"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 26253159; 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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="26253158"><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/26253158/Effective_confinement_theory_from_Abelian_variables_in_SU_3_gauge_theory"><img alt="Research paper thumbnail of Effective confinement theory from Abelian variables in SU(3) gauge theory" class="work-thumbnail" src="https://attachments.academia-assets.com/46568523/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/26253158/Effective_confinement_theory_from_Abelian_variables_in_SU_3_gauge_theory">Effective confinement theory from Abelian variables in SU(3) gauge theory</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">We extend to the SU(3) gauge group a previous approach that we applied to the SU(2) gauge group i...</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 extend to the SU(3) gauge group a previous approach that we applied to the SU(2) gauge group in order to obtain an effective confinement theory for static chromoelectric probe charges due to the condensation of chromomagnetic monopoles. We use the so-called Cho decomposition of the non-Abelian connection in order to reveal the Abelian sector of the non-Abelian gauge theory</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="e3ef8d7ad1447c804a89c68ca8ca288c" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":46568523,"asset_id":26253158,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/46568523/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="26253158"><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="26253158"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 26253158; 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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="26253157"><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/26253157/Geometric_interpretation_for_the_Wess_Zumino_terms"><img alt="Research paper thumbnail of Geometric interpretation for the Wess-Zumino terms" 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/26253157/Geometric_interpretation_for_the_Wess_Zumino_terms">Geometric interpretation for the Wess-Zumino terms</a></div><div class="wp-workCard_item"><span>Physical Review D</span><span>, 1999</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">ABSTRACT We propose a geometric interpretation for the Wess-Zumino (WZ) constraint converting met...</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">ABSTRACT We propose a geometric interpretation for the Wess-Zumino (WZ) constraint converting method. This study is done in the context of nonlinearly constrained systems, formulated as gauge theories. A deep unifying concept is revealed connecting the invariant and the noninvariant models disclosing a unique relationship between the WZ gauge orbits with the nonlinear surfaces. Such structures unveil the physical and geometrical meaning of the WZ terms in turning second-class constraints into gauge generators quantities. A simple and practical mapping between gauge and nongauge theories is found, providing a new interpretation for the nonlinear constraint as the natural gauge fixing surface for the gauge theories.</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="26253157"><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="26253157"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 26253157; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=26253157]").text(description); $(".js-view-count[data-work-id=26253157]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 26253157; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='26253157']"); 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" } } $('.js-work-strip[data-work-id=26253157]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":26253157,"title":"Geometric interpretation for the Wess-Zumino terms","internal_url":"https://www.academia.edu/26253157/Geometric_interpretation_for_the_Wess_Zumino_terms","owner_id":4792753,"coauthors_can_edit":true,"owner":{"id":4792753,"first_name":"Clovis","middle_initials":null,"last_name":"Wotzasek","page_name":"ClovisWotzasek","domain_name":"ufrj","created_at":"2013-07-09T11:39:48.873-07:00","display_name":"Clovis Wotzasek","url":"https://ufrj.academia.edu/ClovisWotzasek"},"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="26253156"><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/26253156/Bose_symmetry_and_chiral_decomposition_of_2D_fermionic_determinants"><img alt="Research paper thumbnail of Bose symmetry and chiral decomposition of 2D fermionic determinants" class="work-thumbnail" src="https://attachments.academia-assets.com/46568578/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/26253156/Bose_symmetry_and_chiral_decomposition_of_2D_fermionic_determinants">Bose symmetry and chiral decomposition of 2D fermionic determinants</a></div><div class="wp-workCard_item"><span>Nuclear Physics B</span><span>, 1998</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">We show in a precise way, either in the fermionic or its bosonized version, that Bose symmetry pr...</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 in a precise way, either in the fermionic or its bosonized version, that Bose symmetry provides a systematic way to carry out the chiral decomposition of the two dimensional fermionic determinant. Interpreted properly, we show that there is no obstruction of this decomposition to gauge invariance, as is usually claimed. Finally, a new way of interpreting the Polyakov-Wiegman identity is proposed.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="b0ff5651201f3c4c6db02aa3a9546474" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":46568578,"asset_id":26253156,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/46568578/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="26253156"><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="26253156"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 26253156; 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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="26253155"><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/26253155/Remark_on_the_covariant_quantization_of_chiral_bosons"><img alt="Research paper thumbnail of Remark on the covariant quantization of chiral bosons" 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/26253155/Remark_on_the_covariant_quantization_of_chiral_bosons">Remark on the covariant quantization of chiral bosons</a></div><div class="wp-workCard_item"><span>Physical review D: Particles and fields</span><span>, Jan 15, 1991</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">... To convert this constraint into first class we add some counterterms, made of the original ch...</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">... To convert this constraint into first class we add some counterterms, made of the original chiral field Ho plus a Wess-Zumino field 8~ .. R1623 O1991 The American Physical Society Page 2. R1624 CLOVIS WOTZASEK ... Rev. D 37, 3067 (1988); S. J.Gates and W. Siegel,Phys. Lett. ...</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="26253155"><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="26253155"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 26253155; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=26253155]").text(description); $(".js-view-count[data-work-id=26253155]").attr('title', description).tooltip(); 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</script> <div class="js-work-strip profile--work_container" data-work-id="26253152"><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/26253152/Partially_embedding_of_the_quantum_mechanical_analog_of_the_nonlinear_sigma_model"><img alt="Research paper thumbnail of Partially embedding of the quantum mechanical analog of the nonlinear sigma model" class="work-thumbnail" src="https://attachments.academia-assets.com/46568575/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/26253152/Partially_embedding_of_the_quantum_mechanical_analog_of_the_nonlinear_sigma_model">Partially embedding of the quantum mechanical analog of the nonlinear sigma model</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">We consider the quantum mechanical analog of the nonlinear sigma model. There are difficulties to...</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 quantum mechanical analog of the nonlinear sigma model. There are difficulties to completely embed this theory by directly using the Batalin, Fradkin, Fradkina, and Tyutin (BFFT) formalism. We show in this paper how the BFFT method can be conveniently adapted in order to achieve a gauge theory that partially embeds the model.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="1babafcca80c910a8e3dfca9055ee3aa" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":46568575,"asset_id":26253152,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/46568575/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="26253152"><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="26253152"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 26253152; 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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="26253151"><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/26253151/Hidden_symmetry_of_a_fluid_dynamical_model"><img alt="Research paper thumbnail of Hidden symmetry of a fluid dynamical model" class="work-thumbnail" src="https://attachments.academia-assets.com/46568569/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/26253151/Hidden_symmetry_of_a_fluid_dynamical_model">Hidden symmetry of a fluid dynamical model</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">A connection between solutions of the relativistic d-brane system in (d+1) dimensions with the so...</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 connection between solutions of the relativistic d-brane system in (d+1) dimensions with the solutions of a Galileo invariant fluid in d-dimensions is by now well established. However, the physical nature of the light-cone gauge description of a relativistic membrane changes after the reduction to the fluid dynamical model since the gauge symmetry is lost. In this work we argue that the original gauge symmetry present in a relativistic d-brane system can be recovered after the reduction process to a d-dimensional fluid model. To this end we propose, without introducing Wess-Zumino fields, a gauge invariant theory of isentropic fluid dynamics and show that this symmetry corresponds to the invariance under local translation of the velocity potential in the fluid dynamics picture. We show that different but equivalent choices of the sympletic sector lead to distinct representations of the embedded gauge algebra.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="b76161f3d86360fac982509cf06b2e34" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":46568569,"asset_id":26253151,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/46568569/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="26253151"><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="26253151"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 26253151; 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dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=26253150]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":26253150,"title":"New considerations about the Maxwell鈥揚odolsky-like theory through the symplectic embedding formalism","internal_url":"https://www.academia.edu/26253150/New_considerations_about_the_Maxwell_Podolsky_like_theory_through_the_symplectic_embedding_formalism","owner_id":4792753,"coauthors_can_edit":true,"owner":{"id":4792753,"first_name":"Clovis","middle_initials":null,"last_name":"Wotzasek","page_name":"ClovisWotzasek","domain_name":"ufrj","created_at":"2013-07-09T11:39:48.873-07:00","display_name":"Clovis Wotzasek","url":"https://ufrj.academia.edu/ClovisWotzasek"},"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="26253149"><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/26253149/On_chiral_bosons_with_linear_constraint"><img alt="Research paper thumbnail of On chiral bosons with linear constraint" 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/26253149/On_chiral_bosons_with_linear_constraint">On chiral bosons with linear constraint</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">It is shown how to correctly implement the linear chiral boson constraint in the Lagrangian forma...</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">It is shown how to correctly implement the linear chiral boson constraint in the Lagrangian formalism in order to be consistent with the Hamiltonian counterpart.</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="26253149"><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="26253149"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 26253149; 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dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=26253149]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":26253149,"title":"On chiral bosons with linear constraint","internal_url":"https://www.academia.edu/26253149/On_chiral_bosons_with_linear_constraint","owner_id":4792753,"coauthors_can_edit":true,"owner":{"id":4792753,"first_name":"Clovis","middle_initials":null,"last_name":"Wotzasek","page_name":"ClovisWotzasek","domain_name":"ufrj","created_at":"2013-07-09T11:39:48.873-07:00","display_name":"Clovis Wotzasek","url":"https://ufrj.academia.edu/ClovisWotzasek"},"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="26253148"><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/26253148/Lorentz_symmetry_of_the_noncommutative_chiral_bosons"><img alt="Research paper thumbnail of Lorentz symmetry of the noncommutative chiral bosons" class="work-thumbnail" src="https://attachments.academia-assets.com/46568563/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/26253148/Lorentz_symmetry_of_the_noncommutative_chiral_bosons">Lorentz symmetry of the noncommutative chiral bosons</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">We study issues of Lorentz violation symmetry in the context of the recently proposed theory of n...</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 issues of Lorentz violation symmetry in the context of the recently proposed theory of noncommutative fields [1], using the soldering formalism. To this end a noncommutative chiralboson with a deformed algebra [2], used to study these notions in D=2, is properly generalized. We verify, also for this larger group of theories that, although the structure of the Lorentz group is preserved, the velocity of light is scaled by a function of the deformation parameter, as recently claimed. However, we found a sub-set of models where the velocity of propagation is maintained in spite of the presence of the deformed algebra. Effects of a preferred-frame of reference manifest by the presence of birefringence were also studied in the chiral boson framework leading to the scalar sector of the extended Standard Model recently proposed. 11.10.Lm, 11.15.-q and 11.30.Pb</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="5d0e7d8ac1e89c75705784e18713d620" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":46568563,"asset_id":26253148,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/46568563/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="26253148"><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="26253148"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 26253148; 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dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=26253146]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":26253146,"title":"The Wess-Zumino term for the generalized Schwinger model","internal_url":"https://www.academia.edu/26253146/The_Wess_Zumino_term_for_the_generalized_Schwinger_model","owner_id":4792753,"coauthors_can_edit":true,"owner":{"id":4792753,"first_name":"Clovis","middle_initials":null,"last_name":"Wotzasek","page_name":"ClovisWotzasek","domain_name":"ufrj","created_at":"2013-07-09T11:39:48.873-07:00","display_name":"Clovis Wotzasek","url":"https://ufrj.academia.edu/ClovisWotzasek"},"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="26253145"><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/26253145/On_the_dimensional_dependence_of_duality_groups_for_massive_p_forms"><img alt="Research paper thumbnail of On the dimensional dependence of duality groups for massive p-forms" class="work-thumbnail" src="https://attachments.academia-assets.com/46568564/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/26253145/On_the_dimensional_dependence_of_duality_groups_for_massive_p_forms">On the dimensional dependence of duality groups for massive p-forms</a></div><div class="wp-workCard_item"><span>Physics Letters B</span><span>, 2003</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">We study the soldering formalism in the context of abelian p-form theories. We develop further th...</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 the soldering formalism in the context of abelian p-form theories. We develop further the fusion process of massless antisymmetric tensors of different ranks into a massive p-form and establish its duality properties. To illustrate the formalism we consider two situations. First the soldering mass generation mechanism is compared with the Higgs and Julia-Toulouse mechanisms for mass generation due to condensation of electric and magnetic topological defects. We show that the soldering mechanism interpolates between them for even dimensional spacetimes, in this way confirming the Higgs/Julia-Toulouse duality proposed by Quevedo and Trugenberger [1] a few years ago. Next, soldering is applied to the study of duality group classification of the massive forms. We show a dichotomy controlled by the parity of the operator defining the symplectic structure of the theory and find their explicit actions.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="afac1d27e9c2d7a9d5ad67fde0d53dc0" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":46568564,"asset_id":26253145,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/46568564/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="26253145"><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="26253145"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 26253145; 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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="26253144"><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/26253144/U_1_effective_confinement_theory_from_SU_2_restricted_gauge_theory_via_the_Julia_Toulouse_approach"><img alt="Research paper thumbnail of U(1) effective confinement theory from SU(2) restricted gauge theory via the Julia-Toulouse approach" class="work-thumbnail" src="https://attachments.academia-assets.com/46568577/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/26253144/U_1_effective_confinement_theory_from_SU_2_restricted_gauge_theory_via_the_Julia_Toulouse_approach">U(1) effective confinement theory from SU(2) restricted gauge theory via the Julia-Toulouse approach</a></div><div class="wp-workCard_item"><span>Physics Letters B</span><span>, 2011</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">We derive an U (1) effective theory of color confinement by applying the so-called Julia-Toulouse...</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 derive an U (1) effective theory of color confinement by applying the so-called Julia-Toulouse Approach for defects condensation to the SU (2) restricted gauge theory defined by means of the Cho decomposition of the non-abelian connection. Cho's geometric construction naturally displays the topological degrees of freedom of the theory and can be used to put the Yang-Mills action into an abelianized form under certain conditions. On the other hand, the use of the Julia-Toulouse prescription to deal with the monopole condensation leads to an effective action describing the phase whose dynamics is dominated by the magnetic condensate. The effective theory we found describes the interaction between external electric currents displaying a short-range Yukawa interaction plus a linear confinement term that governs the long distance physics.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="baf0aae4634734d94649e01006be404d" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":46568577,"asset_id":26253144,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/46568577/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="26253144"><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="26253144"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 26253144; 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Modern Physics Letters A (MPLA). Particles and Fields; Gravitation; Cosmology and Nuclear Phy...</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">... Modern Physics Letters A (MPLA). Particles and Fields; Gravitation; Cosmology and Nuclear Physics. ...</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="26253161"><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="26253161"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 26253161; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=26253161]").text(description); $(".js-view-count[data-work-id=26253161]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 26253161; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='26253161']"); 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" } } $('.js-work-strip[data-work-id=26253161]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":26253161,"title":"Symplectic Quantization of Constrained Systems","internal_url":"https://www.academia.edu/26253161/Symplectic_Quantization_of_Constrained_Systems","owner_id":4792753,"coauthors_can_edit":true,"owner":{"id":4792753,"first_name":"Clovis","middle_initials":null,"last_name":"Wotzasek","page_name":"ClovisWotzasek","domain_name":"ufrj","created_at":"2013-07-09T11:39:48.873-07:00","display_name":"Clovis Wotzasek","url":"https://ufrj.academia.edu/ClovisWotzasek"},"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="26253160"><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/26253160/Confinement_brane_symmetry_and_the_Julia_Toulouse_approach_for_defects_condensation"><img alt="Research paper thumbnail of Confinement, brane symmetry and the Julia-Toulouse approach for defects condensation" class="work-thumbnail" src="https://attachments.academia-assets.com/46568526/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/26253160/Confinement_brane_symmetry_and_the_Julia_Toulouse_approach_for_defects_condensation">Confinement, brane symmetry and the Julia-Toulouse approach for defects condensation</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">In this work the phenomenon of charge confinement is approached in various contexts. An universal...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">In this work the phenomenon of charge confinement is approached in various contexts. An universal criterium for the identification of this phenomenon is suggested: the so-called spontaneous breaking of the brane symmetry. This local symmetry has its most common incarnation in the Dirac string ambiguity present in the electromagnetic theory with monopoles. The spontaneous breaking of the brane symmetry means</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="a3bf7654549b14770dbd3863b05564d6" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":46568526,"asset_id":26253160,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/46568526/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="26253160"><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="26253160"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 26253160; 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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="26253159"><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/26253159/New_formulations_for_dual_equivalent_actions"><img alt="Research paper thumbnail of New formulations for dual equivalent actions" class="work-thumbnail" src="https://attachments.academia-assets.com/46568525/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/26253159/New_formulations_for_dual_equivalent_actions">New formulations for dual equivalent actions</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">New actions in D=2 and D=3 are proposed that are dual equivalent to known theories displaying wel...</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">New actions in D=2 and D=3 are proposed that are dual equivalent to known theories displaying well defined chirality and helicity, respectively, along with a new interpolating action that maps continuously through the original dualities. The new chiral action in D=2 is a second-order theory displaying the chiral constraint dynamically while in D=3 the helicity constraint is imposed a la</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="157231ca0c38352613d15378adf3c906" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":46568525,"asset_id":26253159,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/46568525/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="26253159"><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="26253159"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 26253159; 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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="26253158"><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/26253158/Effective_confinement_theory_from_Abelian_variables_in_SU_3_gauge_theory"><img alt="Research paper thumbnail of Effective confinement theory from Abelian variables in SU(3) gauge theory" class="work-thumbnail" src="https://attachments.academia-assets.com/46568523/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/26253158/Effective_confinement_theory_from_Abelian_variables_in_SU_3_gauge_theory">Effective confinement theory from Abelian variables in SU(3) gauge theory</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">We extend to the SU(3) gauge group a previous approach that we applied to the SU(2) gauge group i...</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 extend to the SU(3) gauge group a previous approach that we applied to the SU(2) gauge group in order to obtain an effective confinement theory for static chromoelectric probe charges due to the condensation of chromomagnetic monopoles. We use the so-called Cho decomposition of the non-Abelian connection in order to reveal the Abelian sector of the non-Abelian gauge theory</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="e3ef8d7ad1447c804a89c68ca8ca288c" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":46568523,"asset_id":26253158,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/46568523/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="26253158"><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="26253158"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 26253158; 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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="26253157"><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/26253157/Geometric_interpretation_for_the_Wess_Zumino_terms"><img alt="Research paper thumbnail of Geometric interpretation for the Wess-Zumino terms" 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/26253157/Geometric_interpretation_for_the_Wess_Zumino_terms">Geometric interpretation for the Wess-Zumino terms</a></div><div class="wp-workCard_item"><span>Physical Review D</span><span>, 1999</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">ABSTRACT We propose a geometric interpretation for the Wess-Zumino (WZ) constraint converting met...</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">ABSTRACT We propose a geometric interpretation for the Wess-Zumino (WZ) constraint converting method. This study is done in the context of nonlinearly constrained systems, formulated as gauge theories. A deep unifying concept is revealed connecting the invariant and the noninvariant models disclosing a unique relationship between the WZ gauge orbits with the nonlinear surfaces. Such structures unveil the physical and geometrical meaning of the WZ terms in turning second-class constraints into gauge generators quantities. A simple and practical mapping between gauge and nongauge theories is found, providing a new interpretation for the nonlinear constraint as the natural gauge fixing surface for the gauge theories.</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="26253157"><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="26253157"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 26253157; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=26253157]").text(description); $(".js-view-count[data-work-id=26253157]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 26253157; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='26253157']"); 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" } } $('.js-work-strip[data-work-id=26253157]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":26253157,"title":"Geometric interpretation for the Wess-Zumino terms","internal_url":"https://www.academia.edu/26253157/Geometric_interpretation_for_the_Wess_Zumino_terms","owner_id":4792753,"coauthors_can_edit":true,"owner":{"id":4792753,"first_name":"Clovis","middle_initials":null,"last_name":"Wotzasek","page_name":"ClovisWotzasek","domain_name":"ufrj","created_at":"2013-07-09T11:39:48.873-07:00","display_name":"Clovis Wotzasek","url":"https://ufrj.academia.edu/ClovisWotzasek"},"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="26253156"><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/26253156/Bose_symmetry_and_chiral_decomposition_of_2D_fermionic_determinants"><img alt="Research paper thumbnail of Bose symmetry and chiral decomposition of 2D fermionic determinants" class="work-thumbnail" src="https://attachments.academia-assets.com/46568578/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/26253156/Bose_symmetry_and_chiral_decomposition_of_2D_fermionic_determinants">Bose symmetry and chiral decomposition of 2D fermionic determinants</a></div><div class="wp-workCard_item"><span>Nuclear Physics B</span><span>, 1998</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">We show in a precise way, either in the fermionic or its bosonized version, that Bose symmetry pr...</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 in a precise way, either in the fermionic or its bosonized version, that Bose symmetry provides a systematic way to carry out the chiral decomposition of the two dimensional fermionic determinant. Interpreted properly, we show that there is no obstruction of this decomposition to gauge invariance, as is usually claimed. Finally, a new way of interpreting the Polyakov-Wiegman identity is proposed.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="b0ff5651201f3c4c6db02aa3a9546474" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":46568578,"asset_id":26253156,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/46568578/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="26253156"><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="26253156"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 26253156; 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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="26253155"><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/26253155/Remark_on_the_covariant_quantization_of_chiral_bosons"><img alt="Research paper thumbnail of Remark on the covariant quantization of chiral bosons" 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/26253155/Remark_on_the_covariant_quantization_of_chiral_bosons">Remark on the covariant quantization of chiral bosons</a></div><div class="wp-workCard_item"><span>Physical review D: Particles and fields</span><span>, Jan 15, 1991</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">... To convert this constraint into first class we add some counterterms, made of the original ch...</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">... To convert this constraint into first class we add some counterterms, made of the original chiral field Ho plus a Wess-Zumino field 8~ .. R1623 O1991 The American Physical Society Page 2. R1624 CLOVIS WOTZASEK ... Rev. D 37, 3067 (1988); S. J.Gates and W. Siegel,Phys. Lett. ...</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="26253155"><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="26253155"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 26253155; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=26253155]").text(description); $(".js-view-count[data-work-id=26253155]").attr('title', description).tooltip(); 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</script> <div class="js-work-strip profile--work_container" data-work-id="26253152"><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/26253152/Partially_embedding_of_the_quantum_mechanical_analog_of_the_nonlinear_sigma_model"><img alt="Research paper thumbnail of Partially embedding of the quantum mechanical analog of the nonlinear sigma model" class="work-thumbnail" src="https://attachments.academia-assets.com/46568575/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/26253152/Partially_embedding_of_the_quantum_mechanical_analog_of_the_nonlinear_sigma_model">Partially embedding of the quantum mechanical analog of the nonlinear sigma model</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">We consider the quantum mechanical analog of the nonlinear sigma model. There are difficulties to...</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 quantum mechanical analog of the nonlinear sigma model. There are difficulties to completely embed this theory by directly using the Batalin, Fradkin, Fradkina, and Tyutin (BFFT) formalism. We show in this paper how the BFFT method can be conveniently adapted in order to achieve a gauge theory that partially embeds the model.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="1babafcca80c910a8e3dfca9055ee3aa" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":46568575,"asset_id":26253152,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/46568575/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="26253152"><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="26253152"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 26253152; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=26253152]").text(description); $(".js-view-count[data-work-id=26253152]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 26253152; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='26253152']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-a9bf3a2bc8c89fa2a77156577594264ee8a0f214d74241bc0fcd3f69f8d107ac.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); 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$(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="26253151"><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/26253151/Hidden_symmetry_of_a_fluid_dynamical_model"><img alt="Research paper thumbnail of Hidden symmetry of a fluid dynamical model" class="work-thumbnail" src="https://attachments.academia-assets.com/46568569/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/26253151/Hidden_symmetry_of_a_fluid_dynamical_model">Hidden symmetry of a fluid dynamical model</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">A connection between solutions of the relativistic d-brane system in (d+1) dimensions with the so...</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 connection between solutions of the relativistic d-brane system in (d+1) dimensions with the solutions of a Galileo invariant fluid in d-dimensions is by now well established. However, the physical nature of the light-cone gauge description of a relativistic membrane changes after the reduction to the fluid dynamical model since the gauge symmetry is lost. In this work we argue that the original gauge symmetry present in a relativistic d-brane system can be recovered after the reduction process to a d-dimensional fluid model. To this end we propose, without introducing Wess-Zumino fields, a gauge invariant theory of isentropic fluid dynamics and show that this symmetry corresponds to the invariance under local translation of the velocity potential in the fluid dynamics picture. We show that different but equivalent choices of the sympletic sector lead to distinct representations of the embedded gauge algebra.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="b76161f3d86360fac982509cf06b2e34" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":46568569,"asset_id":26253151,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/46568569/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="26253151"><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="26253151"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 26253151; 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dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=26253149]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":26253149,"title":"On chiral bosons with linear constraint","internal_url":"https://www.academia.edu/26253149/On_chiral_bosons_with_linear_constraint","owner_id":4792753,"coauthors_can_edit":true,"owner":{"id":4792753,"first_name":"Clovis","middle_initials":null,"last_name":"Wotzasek","page_name":"ClovisWotzasek","domain_name":"ufrj","created_at":"2013-07-09T11:39:48.873-07:00","display_name":"Clovis Wotzasek","url":"https://ufrj.academia.edu/ClovisWotzasek"},"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="26253148"><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/26253148/Lorentz_symmetry_of_the_noncommutative_chiral_bosons"><img alt="Research paper thumbnail of Lorentz symmetry of the noncommutative chiral bosons" class="work-thumbnail" src="https://attachments.academia-assets.com/46568563/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/26253148/Lorentz_symmetry_of_the_noncommutative_chiral_bosons">Lorentz symmetry of the noncommutative chiral bosons</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">We study issues of Lorentz violation symmetry in the context of the recently proposed theory of n...</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 issues of Lorentz violation symmetry in the context of the recently proposed theory of noncommutative fields [1], using the soldering formalism. To this end a noncommutative chiralboson with a deformed algebra [2], used to study these notions in D=2, is properly generalized. We verify, also for this larger group of theories that, although the structure of the Lorentz group is preserved, the velocity of light is scaled by a function of the deformation parameter, as recently claimed. However, we found a sub-set of models where the velocity of propagation is maintained in spite of the presence of the deformed algebra. Effects of a preferred-frame of reference manifest by the presence of birefringence were also studied in the chiral boson framework leading to the scalar sector of the extended Standard Model recently proposed. 11.10.Lm, 11.15.-q and 11.30.Pb</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="5d0e7d8ac1e89c75705784e18713d620" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":46568563,"asset_id":26253148,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/46568563/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="26253148"><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="26253148"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 26253148; 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window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=26253146]").text(description); $(".js-view-count[data-work-id=26253146]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 26253146; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='26253146']"); 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" } } $('.js-work-strip[data-work-id=26253146]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":26253146,"title":"The Wess-Zumino term for the generalized Schwinger model","internal_url":"https://www.academia.edu/26253146/The_Wess_Zumino_term_for_the_generalized_Schwinger_model","owner_id":4792753,"coauthors_can_edit":true,"owner":{"id":4792753,"first_name":"Clovis","middle_initials":null,"last_name":"Wotzasek","page_name":"ClovisWotzasek","domain_name":"ufrj","created_at":"2013-07-09T11:39:48.873-07:00","display_name":"Clovis Wotzasek","url":"https://ufrj.academia.edu/ClovisWotzasek"},"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="26253145"><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/26253145/On_the_dimensional_dependence_of_duality_groups_for_massive_p_forms"><img alt="Research paper thumbnail of On the dimensional dependence of duality groups for massive p-forms" class="work-thumbnail" src="https://attachments.academia-assets.com/46568564/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/26253145/On_the_dimensional_dependence_of_duality_groups_for_massive_p_forms">On the dimensional dependence of duality groups for massive p-forms</a></div><div class="wp-workCard_item"><span>Physics Letters B</span><span>, 2003</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">We study the soldering formalism in the context of abelian p-form theories. We develop further th...</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 the soldering formalism in the context of abelian p-form theories. We develop further the fusion process of massless antisymmetric tensors of different ranks into a massive p-form and establish its duality properties. To illustrate the formalism we consider two situations. First the soldering mass generation mechanism is compared with the Higgs and Julia-Toulouse mechanisms for mass generation due to condensation of electric and magnetic topological defects. We show that the soldering mechanism interpolates between them for even dimensional spacetimes, in this way confirming the Higgs/Julia-Toulouse duality proposed by Quevedo and Trugenberger [1] a few years ago. Next, soldering is applied to the study of duality group classification of the massive forms. We show a dichotomy controlled by the parity of the operator defining the symplectic structure of the theory and find their explicit actions.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="afac1d27e9c2d7a9d5ad67fde0d53dc0" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":46568564,"asset_id":26253145,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/46568564/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="26253145"><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="26253145"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 26253145; 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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="26253144"><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/26253144/U_1_effective_confinement_theory_from_SU_2_restricted_gauge_theory_via_the_Julia_Toulouse_approach"><img alt="Research paper thumbnail of U(1) effective confinement theory from SU(2) restricted gauge theory via the Julia-Toulouse approach" class="work-thumbnail" src="https://attachments.academia-assets.com/46568577/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/26253144/U_1_effective_confinement_theory_from_SU_2_restricted_gauge_theory_via_the_Julia_Toulouse_approach">U(1) effective confinement theory from SU(2) restricted gauge theory via the Julia-Toulouse approach</a></div><div class="wp-workCard_item"><span>Physics Letters B</span><span>, 2011</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">We derive an U (1) effective theory of color confinement by applying the so-called Julia-Toulouse...</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 derive an U (1) effective theory of color confinement by applying the so-called Julia-Toulouse Approach for defects condensation to the SU (2) restricted gauge theory defined by means of the Cho decomposition of the non-abelian connection. Cho's geometric construction naturally displays the topological degrees of freedom of the theory and can be used to put the Yang-Mills action into an abelianized form under certain conditions. On the other hand, the use of the Julia-Toulouse prescription to deal with the monopole condensation leads to an effective action describing the phase whose dynamics is dominated by the magnetic condensate. The effective theory we found describes the interaction between external electric currents displaying a short-range Yukawa interaction plus a linear confinement term that governs the long distance physics.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="baf0aae4634734d94649e01006be404d" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":46568577,"asset_id":26253144,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/46568577/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="26253144"><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="26253144"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 26253144; 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