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Roper state from overlap fermions
The Roper state is extracted with valence overlap fermions on a 2 + 1 -flavor domain-wall fermion lattice (spacing a = 0.114 fm and mπ = 330 MeV) using both the sequential empirical Bayes (SEB) method and the variational method. The results are consistent, provided that a large smearing-size interpo...
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Published in: | Physical review. D 2020-03, Vol.101 (5), p.1, Article 054511 |
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creator | Sun, Mingyang Chen, Ying Wang, Gen Alexandru, Andrei Dong, Shao-Jing Draper, Terrence Fallica, Jacob Gong, Ming Lee, Frank X. Li, Anyi Liang, Jian Liu, Keh-Fei Mathur, Nilmani Yang, Yi-Bo |
description | The Roper state is extracted with valence overlap fermions on a 2 + 1 -flavor domain-wall fermion lattice (spacing a = 0.114 fm and mπ = 330 MeV) using both the sequential empirical Bayes (SEB) method and the variational method. The results are consistent, provided that a large smearing-size interpolation operator is included in the variational calculation to have better overlap with the lowest radial excitation. The SEB and variational calculation with large smearing size are also carried out for an anisotropic clover lattice with similar parameters (spatial lattice spacing as = 0.12 fm and pion mass mπ = 396 MeV) and obtain consistent results. However, these calculations with clover fermions give a Roper mass of mR = 1.92 (6) GeV, while the same approach with overlap fermions finds the Roper ≈ 280 MeV lower, at mR = 1.64 (9) GeV, for identical valence pion mass. The fact that the prediction of the Roper state by overlap fermions is consistently lower than those of clover fermions, chirally improved fermions, and twisted-mass fermions over a wide range of pion masses has been dubbed a "Roper puzzle." To understand the origin of this difference, we study the hairpin Z -diagram in the isovector scalar meson (a0) correlator in the quenched approximation. The lack of quark loops in the quenched approximation turns the a0 correlator negative; giving rise to a ghost "would-be" η π state. Comparing the a0 correlators for valence clover and overlap fermions, at a valence pion mass of 290 MeV, on three quenched Wilson-gauge lattices, we find that the spectral weight of the ghost state with clover fermions is smaller than that of the overlap at a = 0.12 fm and 0.09 fm-the ratios of the Wilson ghost-state magnitudes (correlator minima) are about half of those of overlap-whereas, the whole a0 correlators of clover and overlap at a = 0.06 fm coincide within errors. This suggests that chiral symmetry is restored for clover at a ≤ 0.06 fm and that the Roper mass should agree between clover and overlap fermions toward the continuum limit. We conclude that the present work supports a resolution of the "Roper puzzle" due to Z-graph type chiral dynamics. This entails coupling to higher components in the Fock space (e.g., Nπ, Nππ states) to induce the effective flavor-spin interaction between quarks as prescribed in the chiral quark model, resulting in the parity-reversal pattern as observed in the experimental excited states of N, Δ and Λ. |
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The results are consistent, provided that a large smearing-size interpolation operator is included in the variational calculation to have better overlap with the lowest radial excitation. The SEB and variational calculation with large smearing size are also carried out for an anisotropic clover lattice with similar parameters (spatial lattice spacing as = 0.12 fm and pion mass mπ = 396 MeV) and obtain consistent results. However, these calculations with clover fermions give a Roper mass of mR = 1.92 (6) GeV, while the same approach with overlap fermions finds the Roper ≈ 280 MeV lower, at mR = 1.64 (9) GeV, for identical valence pion mass. The fact that the prediction of the Roper state by overlap fermions is consistently lower than those of clover fermions, chirally improved fermions, and twisted-mass fermions over a wide range of pion masses has been dubbed a "Roper puzzle." To understand the origin of this difference, we study the hairpin Z -diagram in the isovector scalar meson (a0) correlator in the quenched approximation. The lack of quark loops in the quenched approximation turns the a0 correlator negative; giving rise to a ghost "would-be" η π state. Comparing the a0 correlators for valence clover and overlap fermions, at a valence pion mass of 290 MeV, on three quenched Wilson-gauge lattices, we find that the spectral weight of the ghost state with clover fermions is smaller than that of the overlap at a = 0.12 fm and 0.09 fm-the ratios of the Wilson ghost-state magnitudes (correlator minima) are about half of those of overlap-whereas, the whole a0 correlators of clover and overlap at a = 0.06 fm coincide within errors. This suggests that chiral symmetry is restored for clover at a ≤ 0.06 fm and that the Roper mass should agree between clover and overlap fermions toward the continuum limit. We conclude that the present work supports a resolution of the "Roper puzzle" due to Z-graph type chiral dynamics. This entails coupling to higher components in the Fock space (e.g., Nπ, Nππ states) to induce the effective flavor-spin interaction between quarks as prescribed in the chiral quark model, resulting in the parity-reversal pattern as observed in the experimental excited states of N, Δ and Λ.</description><identifier>ISSN: 2470-0010</identifier><identifier>EISSN: 2470-0029</identifier><identifier>DOI: 10.1103/PhysRevD.101.054511</identifier><language>eng</language><publisher>College Park: American Physical Society</publisher><subject>Approximation ; Chiral dynamics ; correlation function ; Correlators ; Domain walls ; fermion: clover ; fermion: domain wall ; fermion: overlap ; Fermions ; Flavor (particle physics) ; Fock space ; Galling ; Interpolation ; Lattice field theories, lattice QCD ; Lattices ; NUCLEAR PHYSICS AND RADIATION PHYSICS ; nucleon resonance ; numerical calculations: variational ; PHYSICS OF ELEMENTARY PARTICLES AND FIELDS ; pi: mass ; Pions ; quantum chromodynamics: lattice ; quantum chromodynamics: quenching ; quark model: chiral ; Quark models ; Quarks ; Quenching ; scalar meson: isovector</subject><ispartof>Physical review. D, 2020-03, Vol.101 (5), p.1, Article 054511</ispartof><rights>Copyright American Physical Society Mar 1, 2020</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c349t-9110f33feaa843dc5e133af03278395b7b1b26b4a04e43feb9f39d7178d434f33</citedby><cites>FETCH-LOGICAL-c349t-9110f33feaa843dc5e133af03278395b7b1b26b4a04e43feb9f39d7178d434f33</cites><orcidid>0000-0002-8562-8918 ; 0000-0002-5231-4795 ; 0000-0002-8943-8011 ; 0000-0003-3104-1211 ; 0000000285628918 ; 0000000331041211 ; 0000000252314795 ; 0000000289438011</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,314,780,784,885,27924,27925</link.rule.ids><backlink>$$Uhttps://www.osti.gov/biblio/1607612$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Sun, Mingyang</creatorcontrib><creatorcontrib>Chen, Ying</creatorcontrib><creatorcontrib>Wang, Gen</creatorcontrib><creatorcontrib>Alexandru, Andrei</creatorcontrib><creatorcontrib>Dong, Shao-Jing</creatorcontrib><creatorcontrib>Draper, Terrence</creatorcontrib><creatorcontrib>Fallica, Jacob</creatorcontrib><creatorcontrib>Gong, Ming</creatorcontrib><creatorcontrib>Lee, Frank X.</creatorcontrib><creatorcontrib>Li, Anyi</creatorcontrib><creatorcontrib>Liang, Jian</creatorcontrib><creatorcontrib>Liu, Keh-Fei</creatorcontrib><creatorcontrib>Mathur, Nilmani</creatorcontrib><creatorcontrib>Yang, Yi-Bo</creatorcontrib><creatorcontrib>χQCD Collaboration</creatorcontrib><creatorcontrib>Univ. of Kentucky, Lexington, KY (United States)</creatorcontrib><title>Roper state from overlap fermions</title><title>Physical review. D</title><description>The Roper state is extracted with valence overlap fermions on a 2 + 1 -flavor domain-wall fermion lattice (spacing a = 0.114 fm and mπ = 330 MeV) using both the sequential empirical Bayes (SEB) method and the variational method. The results are consistent, provided that a large smearing-size interpolation operator is included in the variational calculation to have better overlap with the lowest radial excitation. The SEB and variational calculation with large smearing size are also carried out for an anisotropic clover lattice with similar parameters (spatial lattice spacing as = 0.12 fm and pion mass mπ = 396 MeV) and obtain consistent results. However, these calculations with clover fermions give a Roper mass of mR = 1.92 (6) GeV, while the same approach with overlap fermions finds the Roper ≈ 280 MeV lower, at mR = 1.64 (9) GeV, for identical valence pion mass. The fact that the prediction of the Roper state by overlap fermions is consistently lower than those of clover fermions, chirally improved fermions, and twisted-mass fermions over a wide range of pion masses has been dubbed a "Roper puzzle." To understand the origin of this difference, we study the hairpin Z -diagram in the isovector scalar meson (a0) correlator in the quenched approximation. The lack of quark loops in the quenched approximation turns the a0 correlator negative; giving rise to a ghost "would-be" η π state. Comparing the a0 correlators for valence clover and overlap fermions, at a valence pion mass of 290 MeV, on three quenched Wilson-gauge lattices, we find that the spectral weight of the ghost state with clover fermions is smaller than that of the overlap at a = 0.12 fm and 0.09 fm-the ratios of the Wilson ghost-state magnitudes (correlator minima) are about half of those of overlap-whereas, the whole a0 correlators of clover and overlap at a = 0.06 fm coincide within errors. This suggests that chiral symmetry is restored for clover at a ≤ 0.06 fm and that the Roper mass should agree between clover and overlap fermions toward the continuum limit. We conclude that the present work supports a resolution of the "Roper puzzle" due to Z-graph type chiral dynamics. This entails coupling to higher components in the Fock space (e.g., Nπ, Nππ states) to induce the effective flavor-spin interaction between quarks as prescribed in the chiral quark model, resulting in the parity-reversal pattern as observed in the experimental excited states of N, Δ and Λ.</description><subject>Approximation</subject><subject>Chiral dynamics</subject><subject>correlation function</subject><subject>Correlators</subject><subject>Domain walls</subject><subject>fermion: clover</subject><subject>fermion: domain wall</subject><subject>fermion: overlap</subject><subject>Fermions</subject><subject>Flavor (particle physics)</subject><subject>Fock space</subject><subject>Galling</subject><subject>Interpolation</subject><subject>Lattice field theories, lattice QCD</subject><subject>Lattices</subject><subject>NUCLEAR PHYSICS AND RADIATION PHYSICS</subject><subject>nucleon resonance</subject><subject>numerical calculations: variational</subject><subject>PHYSICS OF ELEMENTARY PARTICLES AND FIELDS</subject><subject>pi: mass</subject><subject>Pions</subject><subject>quantum chromodynamics: lattice</subject><subject>quantum chromodynamics: quenching</subject><subject>quark model: chiral</subject><subject>Quark models</subject><subject>Quarks</subject><subject>Quenching</subject><subject>scalar meson: isovector</subject><issn>2470-0010</issn><issn>2470-0029</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2020</creationdate><recordtype>article</recordtype><recordid>eNo9kNFKwzAUhoMoOOaewJuq1505PWnTXMp0KgyUodchTRPWsTU1yQZ7eyNVr87P4TuHn4-Qa6BzAIr375tTWJvj4xwozGnJSoAzMikYpzmlhTj_z0AvySyELU2xooIDTMjN2g3GZyGqaDLr3T5zR-N3asis8fvO9eGKXFi1C2b2O6fkc_n0sXjJV2_Pr4uHVa6RiZiL1MUiWqNUzbDVpQFEZSkWvEZRNryBpqgapigzLGGNsChaDrxuGbJ0OSW3418XYieD7qLRG-363ugoU19eQZGguxEavPs6mBDl1h18n3rJAuu65pwJligcKe1dCN5YOfhur_xJApU_zuSfs7QAOTrDb7BFXj4</recordid><startdate>20200301</startdate><enddate>20200301</enddate><creator>Sun, Mingyang</creator><creator>Chen, Ying</creator><creator>Wang, Gen</creator><creator>Alexandru, Andrei</creator><creator>Dong, Shao-Jing</creator><creator>Draper, Terrence</creator><creator>Fallica, Jacob</creator><creator>Gong, Ming</creator><creator>Lee, Frank X.</creator><creator>Li, Anyi</creator><creator>Liang, Jian</creator><creator>Liu, Keh-Fei</creator><creator>Mathur, Nilmani</creator><creator>Yang, Yi-Bo</creator><general>American Physical Society</general><general>American Physical Society (APS)</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7U5</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><scope>OTOTI</scope><orcidid>https://orcid.org/0000-0002-8562-8918</orcidid><orcidid>https://orcid.org/0000-0002-5231-4795</orcidid><orcidid>https://orcid.org/0000-0002-8943-8011</orcidid><orcidid>https://orcid.org/0000-0003-3104-1211</orcidid><orcidid>https://orcid.org/0000000285628918</orcidid><orcidid>https://orcid.org/0000000331041211</orcidid><orcidid>https://orcid.org/0000000252314795</orcidid><orcidid>https://orcid.org/0000000289438011</orcidid></search><sort><creationdate>20200301</creationdate><title>Roper state from overlap fermions</title><author>Sun, Mingyang ; Chen, Ying ; Wang, Gen ; Alexandru, Andrei ; Dong, Shao-Jing ; Draper, Terrence ; Fallica, Jacob ; Gong, Ming ; Lee, Frank X. ; Li, Anyi ; Liang, Jian ; Liu, Keh-Fei ; Mathur, Nilmani ; Yang, Yi-Bo</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c349t-9110f33feaa843dc5e133af03278395b7b1b26b4a04e43feb9f39d7178d434f33</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2020</creationdate><topic>Approximation</topic><topic>Chiral dynamics</topic><topic>correlation function</topic><topic>Correlators</topic><topic>Domain walls</topic><topic>fermion: clover</topic><topic>fermion: domain wall</topic><topic>fermion: overlap</topic><topic>Fermions</topic><topic>Flavor (particle physics)</topic><topic>Fock space</topic><topic>Galling</topic><topic>Interpolation</topic><topic>Lattice field theories, lattice QCD</topic><topic>Lattices</topic><topic>NUCLEAR PHYSICS AND RADIATION PHYSICS</topic><topic>nucleon resonance</topic><topic>numerical calculations: variational</topic><topic>PHYSICS OF ELEMENTARY PARTICLES AND FIELDS</topic><topic>pi: mass</topic><topic>Pions</topic><topic>quantum chromodynamics: lattice</topic><topic>quantum chromodynamics: quenching</topic><topic>quark model: chiral</topic><topic>Quark models</topic><topic>Quarks</topic><topic>Quenching</topic><topic>scalar meson: isovector</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Sun, Mingyang</creatorcontrib><creatorcontrib>Chen, Ying</creatorcontrib><creatorcontrib>Wang, Gen</creatorcontrib><creatorcontrib>Alexandru, Andrei</creatorcontrib><creatorcontrib>Dong, Shao-Jing</creatorcontrib><creatorcontrib>Draper, Terrence</creatorcontrib><creatorcontrib>Fallica, Jacob</creatorcontrib><creatorcontrib>Gong, Ming</creatorcontrib><creatorcontrib>Lee, Frank X.</creatorcontrib><creatorcontrib>Li, Anyi</creatorcontrib><creatorcontrib>Liang, Jian</creatorcontrib><creatorcontrib>Liu, Keh-Fei</creatorcontrib><creatorcontrib>Mathur, Nilmani</creatorcontrib><creatorcontrib>Yang, Yi-Bo</creatorcontrib><creatorcontrib>χQCD Collaboration</creatorcontrib><creatorcontrib>Univ. of Kentucky, Lexington, KY (United States)</creatorcontrib><collection>CrossRef</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>OSTI.GOV</collection><jtitle>Physical review. D</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Sun, Mingyang</au><au>Chen, Ying</au><au>Wang, Gen</au><au>Alexandru, Andrei</au><au>Dong, Shao-Jing</au><au>Draper, Terrence</au><au>Fallica, Jacob</au><au>Gong, Ming</au><au>Lee, Frank X.</au><au>Li, Anyi</au><au>Liang, Jian</au><au>Liu, Keh-Fei</au><au>Mathur, Nilmani</au><au>Yang, Yi-Bo</au><aucorp>χQCD Collaboration</aucorp><aucorp>Univ. of Kentucky, Lexington, KY (United States)</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Roper state from overlap fermions</atitle><jtitle>Physical review. D</jtitle><date>2020-03-01</date><risdate>2020</risdate><volume>101</volume><issue>5</issue><spage>1</spage><pages>1-</pages><artnum>054511</artnum><issn>2470-0010</issn><eissn>2470-0029</eissn><abstract>The Roper state is extracted with valence overlap fermions on a 2 + 1 -flavor domain-wall fermion lattice (spacing a = 0.114 fm and mπ = 330 MeV) using both the sequential empirical Bayes (SEB) method and the variational method. The results are consistent, provided that a large smearing-size interpolation operator is included in the variational calculation to have better overlap with the lowest radial excitation. The SEB and variational calculation with large smearing size are also carried out for an anisotropic clover lattice with similar parameters (spatial lattice spacing as = 0.12 fm and pion mass mπ = 396 MeV) and obtain consistent results. However, these calculations with clover fermions give a Roper mass of mR = 1.92 (6) GeV, while the same approach with overlap fermions finds the Roper ≈ 280 MeV lower, at mR = 1.64 (9) GeV, for identical valence pion mass. The fact that the prediction of the Roper state by overlap fermions is consistently lower than those of clover fermions, chirally improved fermions, and twisted-mass fermions over a wide range of pion masses has been dubbed a "Roper puzzle." To understand the origin of this difference, we study the hairpin Z -diagram in the isovector scalar meson (a0) correlator in the quenched approximation. The lack of quark loops in the quenched approximation turns the a0 correlator negative; giving rise to a ghost "would-be" η π state. Comparing the a0 correlators for valence clover and overlap fermions, at a valence pion mass of 290 MeV, on three quenched Wilson-gauge lattices, we find that the spectral weight of the ghost state with clover fermions is smaller than that of the overlap at a = 0.12 fm and 0.09 fm-the ratios of the Wilson ghost-state magnitudes (correlator minima) are about half of those of overlap-whereas, the whole a0 correlators of clover and overlap at a = 0.06 fm coincide within errors. This suggests that chiral symmetry is restored for clover at a ≤ 0.06 fm and that the Roper mass should agree between clover and overlap fermions toward the continuum limit. We conclude that the present work supports a resolution of the "Roper puzzle" due to Z-graph type chiral dynamics. This entails coupling to higher components in the Fock space (e.g., Nπ, Nππ states) to induce the effective flavor-spin interaction between quarks as prescribed in the chiral quark model, resulting in the parity-reversal pattern as observed in the experimental excited states of N, Δ and Λ.</abstract><cop>College Park</cop><pub>American Physical Society</pub><doi>10.1103/PhysRevD.101.054511</doi><orcidid>https://orcid.org/0000-0002-8562-8918</orcidid><orcidid>https://orcid.org/0000-0002-5231-4795</orcidid><orcidid>https://orcid.org/0000-0002-8943-8011</orcidid><orcidid>https://orcid.org/0000-0003-3104-1211</orcidid><orcidid>https://orcid.org/0000000285628918</orcidid><orcidid>https://orcid.org/0000000331041211</orcidid><orcidid>https://orcid.org/0000000252314795</orcidid><orcidid>https://orcid.org/0000000289438011</orcidid><oa>free_for_read</oa></addata></record> |
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subjects | Approximation Chiral dynamics correlation function Correlators Domain walls fermion: clover fermion: domain wall fermion: overlap Fermions Flavor (particle physics) Fock space Galling Interpolation Lattice field theories, lattice QCD Lattices NUCLEAR PHYSICS AND RADIATION PHYSICS nucleon resonance numerical calculations: variational PHYSICS OF ELEMENTARY PARTICLES AND FIELDS pi: mass Pions quantum chromodynamics: lattice quantum chromodynamics: quenching quark model: chiral Quark models Quarks Quenching scalar meson: isovector |
title | Roper state from overlap fermions |
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