QCDTHERMO

QCD thermodynamics on the lattice

 Coordinatore EOTVOS LORAND TUDOMANYEGYETEM 

Spiacenti, non ci sono informazioni su questo coordinatore. Contattare Fabio per maggiori infomrazioni, grazie.

 Nazionalità Coordinatore Hungary [HU]
 Totale costo 1˙300˙000 €
 EC contributo 1˙300˙000 €
 Programma FP7-IDEAS-ERC
Specific programme: "Ideas" implementing the Seventh Framework Programme of the European Community for research, technological development and demonstration activities (2007 to 2013)
 Code Call ERC-2007-StG
 Funding Scheme ERC-SG
 Anno di inizio 2008
 Periodo (anno-mese-giorno) 2008-07-01   -   2014-03-31

 Partecipanti

# participant  country  role  EC contrib. [€] 
1    EOTVOS LORAND TUDOMANYEGYETEM

 Organization address address: EGYETEM TER 1-3
city: BUDAPEST
postcode: 1053

contact info
Titolo: Dr.
Nome: Katalin
Cognome: Juhászné Huszty
Email: send email
Telefono: 3614116724
Fax: 3614116711

HU (BUDAPEST) hostInstitution 0.00
2    EOTVOS LORAND TUDOMANYEGYETEM

 Organization address address: EGYETEM TER 1-3
city: BUDAPEST
postcode: 1053

contact info
Titolo: Dr.
Nome: Sándor
Cognome: Katz
Email: send email
Telefono: 3613722546
Fax: 3613722509

HU (BUDAPEST) hostInstitution 0.00

Mappa


 Word cloud

Esplora la "nuvola delle parole (Word Cloud) per avere un'idea di massima del progetto.

baryon    chiral    zero    vanishing    sign    studied    densities    lattice    fermions    qcd    transition    determined    staggered    wilson    simulations    density    continuum    plan    temperature    problem   

 Obiettivo del progetto (Objective)

'Quantum Chromodynamics (QCD) at finite temperature and non-zero density describes phenomena relevant to the early universe and heavy-ion collisions. The applicability of perturbation theory is limited to large temperatures and densities. We plan to use lattice simulations to study QCD thermodynamics. There are different regularizations of QCD on the lattice. The computationally most effective one is the staggered formulation, while Wilson or chiral fermions are theoretically more established. We have to distinguish studies at vanishing baryon densities from the ones concerning non-zero density. At vanishing densities the order of the QCD transition between the hadronic phase and the quark-gluon plasma was studied using staggered fermions. In the physical, continuum limit the transition was found to be a crossover. The transition temperature has also been determined. These studies should be and will be extended using Wilson and chiral fermions. This way the staggered results can be checked. At non-vanishing densities direct lattice simulations are prohibited by the infamous sign problem. Recently the multi-parameter reweighting method was developed to study moderate densities using simulations at zero baryon density. The phase diagram as well as the critical point of QCD was determined using staggered fermions with a single lattice resolution. We plan to extend these studies in two ways. In the first step finer lattices will be studied with staggered fermions and a continuum extrapolation will be attempted. In the second step Wilson and possibly chiral fermions will be used. At large densities where the sign problem is the most severe the density of states method will be used. Based on our experience with PC clusters we will build a new, high performance cluster to achieve these goals. The establishment of a strong new research group certainly will improve the competitivity of the European lattice community.'

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