Nature of the $a_1$ meson in lattice quantum chromodynamics studied with chiral fermions
We study the $a_1$ meson using a quenched lattice quantum chromodynamics simulation with the truncated overlap fermions formalism based on the domain wall fermions. The obtained lightest mass of the $a_1$ meson, 1272(45) MeV, is consistent with the experimental value for $a_1$(1260). Thus, $a_1$(126...
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creator | Murakami, Yuko Muroya, Shin Nakamura, Atsushi Nonaka, Chiho Sekiguchi, Motoo Wada, Hiroaki Wakayama, Masayuki |
description | We study the $a_1$ meson using a quenched lattice quantum chromodynamics
simulation with the truncated overlap fermions formalism based on the domain
wall fermions. The obtained lightest mass of the $a_1$ meson, 1272(45) MeV, is
consistent with the experimental value for $a_1$(1260). Thus, $a_1$(1260) can
be identified to have a simple two-body constituent-quark structure. Our
quenched simulation result of $a_1$(1420) can not explain the experimental mass
value, which suggests $a_1$(1420) is not a simple $q\bar{q}$ two quark state. |
doi_str_mv | 10.48550/arxiv.1812.07765 |
format | Article |
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simulation with the truncated overlap fermions formalism based on the domain
wall fermions. The obtained lightest mass of the $a_1$ meson, 1272(45) MeV, is
consistent with the experimental value for $a_1$(1260). Thus, $a_1$(1260) can
be identified to have a simple two-body constituent-quark structure. Our
quenched simulation result of $a_1$(1420) can not explain the experimental mass
value, which suggests $a_1$(1420) is not a simple $q\bar{q}$ two quark state.</description><identifier>DOI: 10.48550/arxiv.1812.07765</identifier><language>eng</language><subject>Physics - High Energy Physics - Lattice</subject><creationdate>2018-12</creationdate><rights>http://arxiv.org/licenses/nonexclusive-distrib/1.0</rights><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>228,230,776,881</link.rule.ids><linktorsrc>$$Uhttps://arxiv.org/abs/1812.07765$$EView_record_in_Cornell_University$$FView_record_in_$$GCornell_University$$Hfree_for_read</linktorsrc><backlink>$$Uhttps://doi.org/10.48550/arXiv.1812.07765$$DView paper in arXiv$$Hfree_for_read</backlink></links><search><creatorcontrib>Murakami, Yuko</creatorcontrib><creatorcontrib>Muroya, Shin</creatorcontrib><creatorcontrib>Nakamura, Atsushi</creatorcontrib><creatorcontrib>Nonaka, Chiho</creatorcontrib><creatorcontrib>Sekiguchi, Motoo</creatorcontrib><creatorcontrib>Wada, Hiroaki</creatorcontrib><creatorcontrib>Wakayama, Masayuki</creatorcontrib><title>Nature of the $a_1$ meson in lattice quantum chromodynamics studied with chiral fermions</title><description>We study the $a_1$ meson using a quenched lattice quantum chromodynamics
simulation with the truncated overlap fermions formalism based on the domain
wall fermions. The obtained lightest mass of the $a_1$ meson, 1272(45) MeV, is
consistent with the experimental value for $a_1$(1260). Thus, $a_1$(1260) can
be identified to have a simple two-body constituent-quark structure. Our
quenched simulation result of $a_1$(1420) can not explain the experimental mass
value, which suggests $a_1$(1420) is not a simple $q\bar{q}$ two quark state.</description><subject>Physics - High Energy Physics - Lattice</subject><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2018</creationdate><recordtype>article</recordtype><sourceid>GOX</sourceid><recordid>eNotz7lOxDAUhWE3FGjgAai4xbQJXuIlJRqxSSNopqCLrmNbsRQn4DjAvD0wUJ3il470EXLFaN0YKekN5q_4UTPDeE21VvKcvD5jWbOHOUAZPGyxY1tIfpkniBOMWErsPbyvOJU1QT_kOc3uOGGK_QJLWV30Dj5jGX5azDhC8DnFeVouyFnAcfGX_7shh_u7w-6x2r88PO1u9xUqLStmQ0ulC42yklMpBRO2Vwb7EBqPLQaUjgruG2Vsoz1tDTPOtVZzK6TlVGzI9d_tida95ZgwH7tfYnciim_jhUyi</recordid><startdate>20181219</startdate><enddate>20181219</enddate><creator>Murakami, Yuko</creator><creator>Muroya, Shin</creator><creator>Nakamura, Atsushi</creator><creator>Nonaka, Chiho</creator><creator>Sekiguchi, Motoo</creator><creator>Wada, Hiroaki</creator><creator>Wakayama, Masayuki</creator><scope>GOX</scope></search><sort><creationdate>20181219</creationdate><title>Nature of the $a_1$ meson in lattice quantum chromodynamics studied with chiral fermions</title><author>Murakami, Yuko ; Muroya, Shin ; Nakamura, Atsushi ; Nonaka, Chiho ; Sekiguchi, Motoo ; Wada, Hiroaki ; Wakayama, Masayuki</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a675-1bf905df46b52055313bc68acff4ea9afa5d032e468b47e09818dd9b72b35b203</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2018</creationdate><topic>Physics - High Energy Physics - Lattice</topic><toplevel>online_resources</toplevel><creatorcontrib>Murakami, Yuko</creatorcontrib><creatorcontrib>Muroya, Shin</creatorcontrib><creatorcontrib>Nakamura, Atsushi</creatorcontrib><creatorcontrib>Nonaka, Chiho</creatorcontrib><creatorcontrib>Sekiguchi, Motoo</creatorcontrib><creatorcontrib>Wada, Hiroaki</creatorcontrib><creatorcontrib>Wakayama, Masayuki</creatorcontrib><collection>arXiv.org</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Murakami, Yuko</au><au>Muroya, Shin</au><au>Nakamura, Atsushi</au><au>Nonaka, Chiho</au><au>Sekiguchi, Motoo</au><au>Wada, Hiroaki</au><au>Wakayama, Masayuki</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Nature of the $a_1$ meson in lattice quantum chromodynamics studied with chiral fermions</atitle><date>2018-12-19</date><risdate>2018</risdate><abstract>We study the $a_1$ meson using a quenched lattice quantum chromodynamics
simulation with the truncated overlap fermions formalism based on the domain
wall fermions. The obtained lightest mass of the $a_1$ meson, 1272(45) MeV, is
consistent with the experimental value for $a_1$(1260). Thus, $a_1$(1260) can
be identified to have a simple two-body constituent-quark structure. Our
quenched simulation result of $a_1$(1420) can not explain the experimental mass
value, which suggests $a_1$(1420) is not a simple $q\bar{q}$ two quark state.</abstract><doi>10.48550/arxiv.1812.07765</doi><oa>free_for_read</oa></addata></record> |
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subjects | Physics - High Energy Physics - Lattice |
title | Nature of the $a_1$ meson in lattice quantum chromodynamics studied with chiral fermions |
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