Phase structure of 2+1-flavour QCD and the magnetic equation of state

We determine the chiral phase structure of $2+1$-flavour QCD in dependence of temperature and the light flavour quark mass with Dyson-Schwinger equations. Specifically, we compute the renormalised chiral condensate and its susceptibility. The latter is used to determine the (pseudo)critical temperat...

Full description

Saved in:
Bibliographic Details
Main Authors: Gao, Fei (Author) , Pawlowski, Jan M. (Author)
Format: Article (Journal) Chapter/Article
Language:English
Published: 1 Dec 2021
In: Arxiv
Year: 2021, Pages: 1-20
Online Access:Verlag, lizenzpflichtig, Volltext: http://arxiv.org/abs/2112.01395
Get full text
Author Notes:Fei Gao and Jan M. Pawlowski

MARC

LEADER 00000caa a2200000 c 4500
001 1805515675
003 DE-627
005 20220927143316.0
007 cr uuu---uuuuu
008 220601s2021 xx |||||o 00| ||eng c
024 7 |a 10.48550/arXiv.2112.01395  |2 doi 
035 |a (DE-627)1805515675 
035 |a (DE-599)KXP1805515675 
035 |a (OCoLC)1341461070 
040 |a DE-627  |b ger  |c DE-627  |e rda 
041 |a eng 
084 |a 29  |2 sdnb 
100 1 |a Gao, Fei  |d 1989-  |e VerfasserIn  |0 (DE-588)1203090102  |0 (DE-627)1687872406  |4 aut 
245 1 0 |a Phase structure of 2+1-flavour QCD and the magnetic equation of state  |c Fei Gao and Jan M. Pawlowski 
246 3 0 |a two one 
264 1 |c 1 Dec 2021 
300 |a 20 
336 |a Text  |b txt  |2 rdacontent 
337 |a Computermedien  |b c  |2 rdamedia 
338 |a Online-Ressource  |b cr  |2 rdacarrier 
500 |a Gesehen am 27.09.2022 
520 |a We determine the chiral phase structure of $2+1$-flavour QCD in dependence of temperature and the light flavour quark mass with Dyson-Schwinger equations. Specifically, we compute the renormalised chiral condensate and its susceptibility. The latter is used to determine the (pseudo)critical temperature for general light current quark masses. In the chiral limit we obtain a critical temperature of about 141\,MeV. This result is in quantitative agreement with recent functional renormalisation group results in QCD, and is compatible with the respective lattice results. We also compute the order parameter potential of the light chiral condensate and map out the regime in the phase diagram which exhibits quasi-massless modes, and discuss the respective chiral dynamics. 
650 4 |a High Energy Physics - Lattice 
650 4 |a High Energy Physics - Phenomenology 
650 4 |a High Energy Physics - Theory 
650 4 |a Nuclear Theory 
700 1 |a Pawlowski, Jan M.  |d 1965-  |e VerfasserIn  |0 (DE-588)1047077388  |0 (DE-627)777525925  |0 (DE-576)400331381  |4 aut 
773 0 8 |i Enthalten in  |t Arxiv  |d Ithaca, NY : Cornell University, 1991  |g (2021), Artikel-ID 2112.01395, Seite 1-20  |h Online-Ressource  |w (DE-627)509006531  |w (DE-600)2225896-6  |w (DE-576)28130436X  |7 nnas  |a Phase structure of 2+1-flavour QCD and the magnetic equation of state 
773 1 8 |g year:2021  |g elocationid:2112.01395  |g pages:1-20  |g extent:20  |a Phase structure of 2+1-flavour QCD and the magnetic equation of state 
856 4 0 |u http://arxiv.org/abs/2112.01395  |x Verlag  |z lizenzpflichtig  |3 Volltext 
951 |a AR 
992 |a 20220601 
993 |a Article 
998 |g 1047077388  |a Pawlowski, Jan M.  |m 1047077388:Pawlowski, Jan M.  |d 130000  |d 130300  |d 700000  |d 728500  |e 130000PP1047077388  |e 130300PP1047077388  |e 700000PP1047077388  |e 728500PP1047077388  |k 0/130000/  |k 1/130000/130300/  |k 0/700000/  |k 1/700000/728500/  |p 2  |y j 
999 |a KXP-PPN1805515675  |e 4142123645 
BIB |a Y 
JSO |a {"name":{"displayForm":["Fei Gao and Jan M. Pawlowski"]},"origin":[{"dateIssuedDisp":"1 Dec 2021","dateIssuedKey":"2021"}],"recId":"1805515675","person":[{"given":"Fei","display":"Gao, Fei","family":"Gao","roleDisplay":"VerfasserIn","role":"aut"},{"given":"Jan M.","display":"Pawlowski, Jan M.","family":"Pawlowski","roleDisplay":"VerfasserIn","role":"aut"}],"id":{"doi":["10.48550/arXiv.2112.01395"],"eki":["1805515675"]},"title":[{"title":"Phase structure of 2+1-flavour QCD and the magnetic equation of state","title_sort":"Phase structure of 2+1-flavour QCD and the magnetic equation of state"}],"language":["eng"],"type":{"media":"Online-Ressource","bibl":"chapter"},"physDesc":[{"extent":"20 S."}],"note":["Gesehen am 27.09.2022"],"relHost":[{"note":["Gesehen am 28.05.2024"],"physDesc":[{"extent":"Online-Ressource"}],"id":{"eki":["509006531"],"zdb":["2225896-6"]},"language":["eng"],"title":[{"title":"Arxiv","title_sort":"Arxiv"}],"part":{"pages":"1-20","text":"(2021), Artikel-ID 2112.01395, Seite 1-20","year":"2021","extent":"20"},"titleAlt":[{"title":"Arxiv.org"},{"title":"Arxiv.org e-print archive"},{"title":"Arxiv e-print archive"},{"title":"De.arxiv.org"}],"origin":[{"publisherPlace":"Ithaca, NY ; [Erscheinungsort nicht ermittelbar]","dateIssuedKey":"1991","publisher":"Cornell University ; Arxiv.org","dateIssuedDisp":"1991-"}],"pubHistory":["1991 -"],"disp":"Phase structure of 2+1-flavour QCD and the magnetic equation of stateArxiv","type":{"media":"Online-Ressource","bibl":"edited-book"},"recId":"509006531"}]} 
SRT |a GAOFEIPAWLPHASESTRUC1202