Meson screening mass in a strongly coupled pion superfluid

Abstract We calculate the meson screening mass in a pion superfluid in the framework of Nambu–Jona-Lasinio model. The minimum of the attractive quark potential is always located at the phase boundary of pion superfluid. Different from the temperature and baryon density effect, the potential at finit...
Ausführliche Beschreibung

Gespeichert in:

Autor*in:	Jiang, Yin [verfasserIn] Ren, Ke [verfasserIn] Xia, Tao [verfasserIn] Zhuang, Pengfei [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2011

Schlagwörter:	Chiral Symmetry Normal Phase Quark Matter Baryon Density Polyakov Loop

Übergeordnetes Werk:	Enthalten in: The European physical journal - Berlin : Springer, 1998, 71(2011), 12 vom: 06. Dez.
Übergeordnetes Werk:	volume:71 ; year:2011 ; number:12 ; day:06 ; month:12

Links:	Volltext

DOI / URN:	10.1140/epjc/s10052-011-1822-z

Katalog-ID:	SPR008324026

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520			\|a Abstract We calculate the meson screening mass in a pion superfluid in the framework of Nambu–Jona-Lasinio model. The minimum of the attractive quark potential is always located at the phase boundary of pion superfluid. Different from the temperature and baryon density effect, the potential at finite isospin density cannot be efficiently suppressed and the matter is always in a strongly coupled phase due to the Goldstone mode in the pion superfluid.
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allfields	10.1140/epjc/s10052-011-1822-z doi (DE-627)SPR008324026 (SPR)s10052-011-1822-z-e DE-627 ger DE-627 rakwb eng 530 ASE 33.50 bkl Jiang, Yin verfasserin aut Meson screening mass in a strongly coupled pion superfluid 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We calculate the meson screening mass in a pion superfluid in the framework of Nambu–Jona-Lasinio model. The minimum of the attractive quark potential is always located at the phase boundary of pion superfluid. Different from the temperature and baryon density effect, the potential at finite isospin density cannot be efficiently suppressed and the matter is always in a strongly coupled phase due to the Goldstone mode in the pion superfluid. Chiral Symmetry (dpeaa)DE-He213 Normal Phase (dpeaa)DE-He213 Quark Matter (dpeaa)DE-He213 Baryon Density (dpeaa)DE-He213 Polyakov Loop (dpeaa)DE-He213 Ren, Ke verfasserin aut Xia, Tao verfasserin aut Zhuang, Pengfei verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 71(2011), 12 vom: 06. Dez. (DE-627)253722934 (DE-600)1459069-4 1434-6052 nnns volume:71 year:2011 number:12 day:06 month:12 https://dx.doi.org/10.1140/epjc/s10052-011-1822-z lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_63 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_110 GBV_ILN_120 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_206 GBV_ILN_267 GBV_ILN_293 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2068 GBV_ILN_2106 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_4012 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 GBV_ILN_4305 GBV_ILN_4307 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4338 33.50 ASE AR 71 2011 12 06 12
spelling	10.1140/epjc/s10052-011-1822-z doi (DE-627)SPR008324026 (SPR)s10052-011-1822-z-e DE-627 ger DE-627 rakwb eng 530 ASE 33.50 bkl Jiang, Yin verfasserin aut Meson screening mass in a strongly coupled pion superfluid 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We calculate the meson screening mass in a pion superfluid in the framework of Nambu–Jona-Lasinio model. The minimum of the attractive quark potential is always located at the phase boundary of pion superfluid. Different from the temperature and baryon density effect, the potential at finite isospin density cannot be efficiently suppressed and the matter is always in a strongly coupled phase due to the Goldstone mode in the pion superfluid. Chiral Symmetry (dpeaa)DE-He213 Normal Phase (dpeaa)DE-He213 Quark Matter (dpeaa)DE-He213 Baryon Density (dpeaa)DE-He213 Polyakov Loop (dpeaa)DE-He213 Ren, Ke verfasserin aut Xia, Tao verfasserin aut Zhuang, Pengfei verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 71(2011), 12 vom: 06. Dez. (DE-627)253722934 (DE-600)1459069-4 1434-6052 nnns volume:71 year:2011 number:12 day:06 month:12 https://dx.doi.org/10.1140/epjc/s10052-011-1822-z lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_63 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_110 GBV_ILN_120 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_206 GBV_ILN_267 GBV_ILN_293 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2068 GBV_ILN_2106 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_4012 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 GBV_ILN_4305 GBV_ILN_4307 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4338 33.50 ASE AR 71 2011 12 06 12
allfields_unstemmed	10.1140/epjc/s10052-011-1822-z doi (DE-627)SPR008324026 (SPR)s10052-011-1822-z-e DE-627 ger DE-627 rakwb eng 530 ASE 33.50 bkl Jiang, Yin verfasserin aut Meson screening mass in a strongly coupled pion superfluid 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We calculate the meson screening mass in a pion superfluid in the framework of Nambu–Jona-Lasinio model. The minimum of the attractive quark potential is always located at the phase boundary of pion superfluid. Different from the temperature and baryon density effect, the potential at finite isospin density cannot be efficiently suppressed and the matter is always in a strongly coupled phase due to the Goldstone mode in the pion superfluid. Chiral Symmetry (dpeaa)DE-He213 Normal Phase (dpeaa)DE-He213 Quark Matter (dpeaa)DE-He213 Baryon Density (dpeaa)DE-He213 Polyakov Loop (dpeaa)DE-He213 Ren, Ke verfasserin aut Xia, Tao verfasserin aut Zhuang, Pengfei verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 71(2011), 12 vom: 06. Dez. (DE-627)253722934 (DE-600)1459069-4 1434-6052 nnns volume:71 year:2011 number:12 day:06 month:12 https://dx.doi.org/10.1140/epjc/s10052-011-1822-z lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_63 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_110 GBV_ILN_120 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_206 GBV_ILN_267 GBV_ILN_293 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2068 GBV_ILN_2106 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_4012 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 GBV_ILN_4305 GBV_ILN_4307 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4338 33.50 ASE AR 71 2011 12 06 12
allfieldsGer	10.1140/epjc/s10052-011-1822-z doi (DE-627)SPR008324026 (SPR)s10052-011-1822-z-e DE-627 ger DE-627 rakwb eng 530 ASE 33.50 bkl Jiang, Yin verfasserin aut Meson screening mass in a strongly coupled pion superfluid 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We calculate the meson screening mass in a pion superfluid in the framework of Nambu–Jona-Lasinio model. The minimum of the attractive quark potential is always located at the phase boundary of pion superfluid. Different from the temperature and baryon density effect, the potential at finite isospin density cannot be efficiently suppressed and the matter is always in a strongly coupled phase due to the Goldstone mode in the pion superfluid. Chiral Symmetry (dpeaa)DE-He213 Normal Phase (dpeaa)DE-He213 Quark Matter (dpeaa)DE-He213 Baryon Density (dpeaa)DE-He213 Polyakov Loop (dpeaa)DE-He213 Ren, Ke verfasserin aut Xia, Tao verfasserin aut Zhuang, Pengfei verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 71(2011), 12 vom: 06. Dez. (DE-627)253722934 (DE-600)1459069-4 1434-6052 nnns volume:71 year:2011 number:12 day:06 month:12 https://dx.doi.org/10.1140/epjc/s10052-011-1822-z lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_63 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_110 GBV_ILN_120 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_206 GBV_ILN_267 GBV_ILN_293 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2068 GBV_ILN_2106 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_4012 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 GBV_ILN_4305 GBV_ILN_4307 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4338 33.50 ASE AR 71 2011 12 06 12
allfieldsSound	10.1140/epjc/s10052-011-1822-z doi (DE-627)SPR008324026 (SPR)s10052-011-1822-z-e DE-627 ger DE-627 rakwb eng 530 ASE 33.50 bkl Jiang, Yin verfasserin aut Meson screening mass in a strongly coupled pion superfluid 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract We calculate the meson screening mass in a pion superfluid in the framework of Nambu–Jona-Lasinio model. The minimum of the attractive quark potential is always located at the phase boundary of pion superfluid. Different from the temperature and baryon density effect, the potential at finite isospin density cannot be efficiently suppressed and the matter is always in a strongly coupled phase due to the Goldstone mode in the pion superfluid. Chiral Symmetry (dpeaa)DE-He213 Normal Phase (dpeaa)DE-He213 Quark Matter (dpeaa)DE-He213 Baryon Density (dpeaa)DE-He213 Polyakov Loop (dpeaa)DE-He213 Ren, Ke verfasserin aut Xia, Tao verfasserin aut Zhuang, Pengfei verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 71(2011), 12 vom: 06. Dez. (DE-627)253722934 (DE-600)1459069-4 1434-6052 nnns volume:71 year:2011 number:12 day:06 month:12 https://dx.doi.org/10.1140/epjc/s10052-011-1822-z lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_63 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_110 GBV_ILN_120 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_206 GBV_ILN_267 GBV_ILN_293 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2068 GBV_ILN_2106 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_4012 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 GBV_ILN_4305 GBV_ILN_4307 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4338 33.50 ASE AR 71 2011 12 06 12
language	English
source	Enthalten in The European physical journal 71(2011), 12 vom: 06. Dez. volume:71 year:2011 number:12 day:06 month:12
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topic_facet	Chiral Symmetry Normal Phase Quark Matter Baryon Density Polyakov Loop
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author	Jiang, Yin
spellingShingle	Jiang, Yin ddc 530 bkl 33.50 misc Chiral Symmetry misc Normal Phase misc Quark Matter misc Baryon Density misc Polyakov Loop Meson screening mass in a strongly coupled pion superfluid
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topic_title	530 ASE 33.50 bkl Meson screening mass in a strongly coupled pion superfluid Chiral Symmetry (dpeaa)DE-He213 Normal Phase (dpeaa)DE-He213 Quark Matter (dpeaa)DE-He213 Baryon Density (dpeaa)DE-He213 Polyakov Loop (dpeaa)DE-He213
topic	ddc 530 bkl 33.50 misc Chiral Symmetry misc Normal Phase misc Quark Matter misc Baryon Density misc Polyakov Loop
topic_unstemmed	ddc 530 bkl 33.50 misc Chiral Symmetry misc Normal Phase misc Quark Matter misc Baryon Density misc Polyakov Loop
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title	Meson screening mass in a strongly coupled pion superfluid
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title_full	Meson screening mass in a strongly coupled pion superfluid
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author_browse	Jiang, Yin Ren, Ke Xia, Tao Zhuang, Pengfei
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title_sort	meson screening mass in a strongly coupled pion superfluid
title_auth	Meson screening mass in a strongly coupled pion superfluid
abstract	Abstract We calculate the meson screening mass in a pion superfluid in the framework of Nambu–Jona-Lasinio model. The minimum of the attractive quark potential is always located at the phase boundary of pion superfluid. Different from the temperature and baryon density effect, the potential at finite isospin density cannot be efficiently suppressed and the matter is always in a strongly coupled phase due to the Goldstone mode in the pion superfluid.
abstractGer	Abstract We calculate the meson screening mass in a pion superfluid in the framework of Nambu–Jona-Lasinio model. The minimum of the attractive quark potential is always located at the phase boundary of pion superfluid. Different from the temperature and baryon density effect, the potential at finite isospin density cannot be efficiently suppressed and the matter is always in a strongly coupled phase due to the Goldstone mode in the pion superfluid.
abstract_unstemmed	Abstract We calculate the meson screening mass in a pion superfluid in the framework of Nambu–Jona-Lasinio model. The minimum of the attractive quark potential is always located at the phase boundary of pion superfluid. Different from the temperature and baryon density effect, the potential at finite isospin density cannot be efficiently suppressed and the matter is always in a strongly coupled phase due to the Goldstone mode in the pion superfluid.
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title_short	Meson screening mass in a strongly coupled pion superfluid
url	https://dx.doi.org/10.1140/epjc/s10052-011-1822-z
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author2	Ren, Ke Xia, Tao Zhuang, Pengfei
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up_date	2024-07-03T18:44:56.437Z
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The minimum of the attractive quark potential is always located at the phase boundary of pion superfluid. 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Meson screening mass in a strongly coupled pion superfluid

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