Loading…

Chiral-spin symmetry emergence in baryons and eigenmodes of the Dirac operator

Truncating the low-lying modes of the lattice Dirac operator results in an emergence of the chiral-spin symmetry \(SU(2)_{CS}\) and its flavor extension \(SU(2N_F)\) in hadrons. These are symmetries of the quark - chromo-electric interaction and include chiral symmetries as subgroups. Hence the quar...

Full description

Saved in:
Bibliographic Details
Published in:arXiv.org 2019-05
Main Authors: Catillo, Marco, Leonid Ya Glozman, Lang, Christian B
Format: Article
Language:English
Subjects:
Online Access:Get full text
Tags: Add Tag
No Tags, Be the first to tag this record!
cited_by
cites
container_end_page
container_issue
container_start_page
container_title arXiv.org
container_volume
creator Catillo, Marco
Leonid Ya Glozman
Lang, Christian B
description Truncating the low-lying modes of the lattice Dirac operator results in an emergence of the chiral-spin symmetry \(SU(2)_{CS}\) and its flavor extension \(SU(2N_F)\) in hadrons. These are symmetries of the quark - chromo-electric interaction and include chiral symmetries as subgroups. Hence the quark - chromo-magnetic interaction, which breaks both symmetries, is located at least predominantly in the near - zero modes. Using as a tool the expansion of propagators into eigenmodes of the Dirac operator we here analytically study effects of a gap in the eigenmode spectrum on baryon correlators. We find that both \(U(1)_A\) and \(SU(2)_L \times SU(2)_R\) emerge automatically if there is a gap around zero. Emergence of larger \(SU(2)_{CS}\) and \(SU(4)\) symmetries requires in addition a microscopical dynamical input about the higher-lying modes and their symmetry structure.
doi_str_mv 10.48550/arxiv.1904.01969
format article
fullrecord <record><control><sourceid>proquest</sourceid><recordid>TN_cdi_proquest_journals_2226271640</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>2226271640</sourcerecordid><originalsourceid>FETCH-LOGICAL-a520-4fdc185f58ee7586ec56cd3f05fbcc4a0a0c936061586cde2991c3f62420ef643</originalsourceid><addsrcrecordid>eNotjctqwzAUREWh0JDmA7oTdG336upha1ncJ4R2k31Q5KvGIbZcySnN39fQrAbOcGYYuxNQqlpreHDpt_sphQVVgrDGXrEFSimKWiHesFXOBwBAU6HWcsE-mn2X3LHIYzfwfO57mtKZU0_piwZPfKY7l85xyNwNLaduxn1sKfMY-LQn_jTrnseRkptiumXXwR0zrS65ZJuX503zVqw_X9-bx3XhNEKhQutFrYOuiSpdG_La-FYG0GHnvXLgwFtpwIi59C2htcLLYFAhUDBKLtn9_-yY4veJ8rQ9xFMa5sctIhqshFEg_wCYEVAZ</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>2226271640</pqid></control><display><type>article</type><title>Chiral-spin symmetry emergence in baryons and eigenmodes of the Dirac operator</title><source>Publicly Available Content Database</source><creator>Catillo, Marco ; Leonid Ya Glozman ; Lang, Christian B</creator><creatorcontrib>Catillo, Marco ; Leonid Ya Glozman ; Lang, Christian B</creatorcontrib><description>Truncating the low-lying modes of the lattice Dirac operator results in an emergence of the chiral-spin symmetry \(SU(2)_{CS}\) and its flavor extension \(SU(2N_F)\) in hadrons. These are symmetries of the quark - chromo-electric interaction and include chiral symmetries as subgroups. Hence the quark - chromo-magnetic interaction, which breaks both symmetries, is located at least predominantly in the near - zero modes. Using as a tool the expansion of propagators into eigenmodes of the Dirac operator we here analytically study effects of a gap in the eigenmode spectrum on baryon correlators. We find that both \(U(1)_A\) and \(SU(2)_L \times SU(2)_R\) emerge automatically if there is a gap around zero. Emergence of larger \(SU(2)_{CS}\) and \(SU(4)\) symmetries requires in addition a microscopical dynamical input about the higher-lying modes and their symmetry structure.</description><identifier>EISSN: 2331-8422</identifier><identifier>DOI: 10.48550/arxiv.1904.01969</identifier><language>eng</language><publisher>Ithaca: Cornell University Library, arXiv.org</publisher><subject>Baryons ; Correlators ; Emergence ; Flavor (particle physics) ; Hadrons ; Lattice vibration ; Quarks ; Subgroups ; Symmetry</subject><ispartof>arXiv.org, 2019-05</ispartof><rights>2019. This work is published under http://arxiv.org/licenses/nonexclusive-distrib/1.0/ (the “License”). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://www.proquest.com/docview/2226271640?pq-origsite=primo$$EHTML$$P50$$Gproquest$$Hfree_for_read</linktohtml><link.rule.ids>776,780,25731,27902,36989,44566</link.rule.ids></links><search><creatorcontrib>Catillo, Marco</creatorcontrib><creatorcontrib>Leonid Ya Glozman</creatorcontrib><creatorcontrib>Lang, Christian B</creatorcontrib><title>Chiral-spin symmetry emergence in baryons and eigenmodes of the Dirac operator</title><title>arXiv.org</title><description>Truncating the low-lying modes of the lattice Dirac operator results in an emergence of the chiral-spin symmetry \(SU(2)_{CS}\) and its flavor extension \(SU(2N_F)\) in hadrons. These are symmetries of the quark - chromo-electric interaction and include chiral symmetries as subgroups. Hence the quark - chromo-magnetic interaction, which breaks both symmetries, is located at least predominantly in the near - zero modes. Using as a tool the expansion of propagators into eigenmodes of the Dirac operator we here analytically study effects of a gap in the eigenmode spectrum on baryon correlators. We find that both \(U(1)_A\) and \(SU(2)_L \times SU(2)_R\) emerge automatically if there is a gap around zero. Emergence of larger \(SU(2)_{CS}\) and \(SU(4)\) symmetries requires in addition a microscopical dynamical input about the higher-lying modes and their symmetry structure.</description><subject>Baryons</subject><subject>Correlators</subject><subject>Emergence</subject><subject>Flavor (particle physics)</subject><subject>Hadrons</subject><subject>Lattice vibration</subject><subject>Quarks</subject><subject>Subgroups</subject><subject>Symmetry</subject><issn>2331-8422</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2019</creationdate><recordtype>article</recordtype><sourceid>PIMPY</sourceid><recordid>eNotjctqwzAUREWh0JDmA7oTdG336upha1ncJ4R2k31Q5KvGIbZcySnN39fQrAbOcGYYuxNQqlpreHDpt_sphQVVgrDGXrEFSimKWiHesFXOBwBAU6HWcsE-mn2X3LHIYzfwfO57mtKZU0_piwZPfKY7l85xyNwNLaduxn1sKfMY-LQn_jTrnseRkptiumXXwR0zrS65ZJuX503zVqw_X9-bx3XhNEKhQutFrYOuiSpdG_La-FYG0GHnvXLgwFtpwIi59C2htcLLYFAhUDBKLtn9_-yY4veJ8rQ9xFMa5sctIhqshFEg_wCYEVAZ</recordid><startdate>20190515</startdate><enddate>20190515</enddate><creator>Catillo, Marco</creator><creator>Leonid Ya Glozman</creator><creator>Lang, Christian B</creator><general>Cornell University Library, arXiv.org</general><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>L6V</scope><scope>M7S</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>PTHSS</scope></search><sort><creationdate>20190515</creationdate><title>Chiral-spin symmetry emergence in baryons and eigenmodes of the Dirac operator</title><author>Catillo, Marco ; Leonid Ya Glozman ; Lang, Christian B</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a520-4fdc185f58ee7586ec56cd3f05fbcc4a0a0c936061586cde2991c3f62420ef643</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2019</creationdate><topic>Baryons</topic><topic>Correlators</topic><topic>Emergence</topic><topic>Flavor (particle physics)</topic><topic>Hadrons</topic><topic>Lattice vibration</topic><topic>Quarks</topic><topic>Subgroups</topic><topic>Symmetry</topic><toplevel>online_resources</toplevel><creatorcontrib>Catillo, Marco</creatorcontrib><creatorcontrib>Leonid Ya Glozman</creatorcontrib><creatorcontrib>Lang, Christian B</creatorcontrib><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>Materials Science &amp; Engineering Collection</collection><collection>ProQuest Central (Alumni Edition)</collection><collection>ProQuest Central UK/Ireland</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central Korea</collection><collection>SciTech Premium Collection</collection><collection>ProQuest Engineering Collection</collection><collection>Engineering Database</collection><collection>Publicly Available Content Database</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>ProQuest Central China</collection><collection>Engineering Collection</collection><jtitle>arXiv.org</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Catillo, Marco</au><au>Leonid Ya Glozman</au><au>Lang, Christian B</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Chiral-spin symmetry emergence in baryons and eigenmodes of the Dirac operator</atitle><jtitle>arXiv.org</jtitle><date>2019-05-15</date><risdate>2019</risdate><eissn>2331-8422</eissn><abstract>Truncating the low-lying modes of the lattice Dirac operator results in an emergence of the chiral-spin symmetry \(SU(2)_{CS}\) and its flavor extension \(SU(2N_F)\) in hadrons. These are symmetries of the quark - chromo-electric interaction and include chiral symmetries as subgroups. Hence the quark - chromo-magnetic interaction, which breaks both symmetries, is located at least predominantly in the near - zero modes. Using as a tool the expansion of propagators into eigenmodes of the Dirac operator we here analytically study effects of a gap in the eigenmode spectrum on baryon correlators. We find that both \(U(1)_A\) and \(SU(2)_L \times SU(2)_R\) emerge automatically if there is a gap around zero. Emergence of larger \(SU(2)_{CS}\) and \(SU(4)\) symmetries requires in addition a microscopical dynamical input about the higher-lying modes and their symmetry structure.</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><doi>10.48550/arxiv.1904.01969</doi><oa>free_for_read</oa></addata></record>
fulltext fulltext
identifier EISSN: 2331-8422
ispartof arXiv.org, 2019-05
issn 2331-8422
language eng
recordid cdi_proquest_journals_2226271640
source Publicly Available Content Database
subjects Baryons
Correlators
Emergence
Flavor (particle physics)
Hadrons
Lattice vibration
Quarks
Subgroups
Symmetry
title Chiral-spin symmetry emergence in baryons and eigenmodes of the Dirac operator
url http://sfxeu10.hosted.exlibrisgroup.com/loughborough?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-29T00%3A58%3A44IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Chiral-spin%20symmetry%20emergence%20in%20baryons%20and%20eigenmodes%20of%20the%20Dirac%20operator&rft.jtitle=arXiv.org&rft.au=Catillo,%20Marco&rft.date=2019-05-15&rft.eissn=2331-8422&rft_id=info:doi/10.48550/arxiv.1904.01969&rft_dat=%3Cproquest%3E2226271640%3C/proquest%3E%3Cgrp_id%3Ecdi_FETCH-LOGICAL-a520-4fdc185f58ee7586ec56cd3f05fbcc4a0a0c936061586cde2991c3f62420ef643%3C/grp_id%3E%3Coa%3E%3C/oa%3E%3Curl%3E%3C/url%3E&rft_id=info:oai/&rft_pqid=2226271640&rft_id=info:pmid/&rfr_iscdi=true