53 research outputs found
Towards the Nf = 2 deconfinement transition temperature with O(a) improved Wilson fermions
A lot of effort in lattice simulations over the last years has been devoted to studies of the QCD deconfinement transition. Most state-of-the-art simulations use rooted staggered fermions, while Wilson fermions are affected by large systematic uncertainties, such as coarse lattices or heavy sea quarks. Here we report on an ongoing study of the transition, using two degenerate flavours of nonperturbatively O(a) improved Wilson fermions. We start with Nt = 12 and 16 lattices and pion masses of 600 to 450 MeV, aiming at chiral and continuum limits with light quarks
Towards the N_f=2 deconfinement transition temperature with O(a) improved Wilson fermions: An update
We give an update on our current project to determine the transition
temperature and the order of the deconfinement transition in the chiral limit
of two flavour QCD. We use nonperturbatively O(a) improved Wilson fermions of
the Sheikholeslami-Wohlert type, employing the efficient deflation accelerated
DDHMC algorithm. We start at lattices with N_t>=12 and pion masses below 600
MeV, aiming at chiral and continuum limits with light quarks.Comment: 3 pages, 4 figures, talk given at "Quark Confinement and the Hadron
Spectrum IX", Madrid, Spain, Aug. 30-Sep. 3, 2010, submitted to AIP
Conference Proceeding
Cutoff effects of Wilson fermions on the QCD equation of state to O(g^2)
We compute the O(g^2) contribution to the thermodynamic pressure for Wilson
fermions in the standard, the twisted mass, and clover improved formulation in
lattice perturbation theory, including finite mass effects. We compare the
continuum approaches of these discretizations for the massive ideal and
interacting gas. In all cases, for N_t \geq 8 cutoff effects of Wilson type
fermions are comparable to those of staggered fermions, but asymptotic scaling
requires .Comment: 9 pages, 4 figures. Version shortened to a brief report accepted by
PR
The finite-temperature phase structure of lattice QCD with twisted-mass Wilson fermions
We report progress in our exploration of the finite-temperature phase structure of two-flavour lattice
QCD with twisted-mass Wilson fermions and a tree-level Symanzik-improved gauge action
for a temporal lattice size Nt = 8. Extending our investigations to a wider region of parameter
space we gain a global view of the rich phase structure. We identify the finite temperature transition/
crossover for a non-vanishing twisted-mass parameter in the neighbourhood of the zerotemperature
critical line at sufficiently high b . Our findings are consistent with Creutz’s conjecture
of a conical shape of the finite temperature transition surface. Comparing with NLO lattice
cPT we achieve an improved understanding of this shape
Pseudo-Critical Temperature and Thermal Equation of State from Nf = 2 Twisted Mass Lattice QCD
We report about the current status of our ongoing study of the chiral limit of two-flavor QCD at finite temperature with twisted mass quarks. We estimate the pseudo-critical temperature Tc for three values of the pion mass in the range of mPS ~ 300 and 500 MeV and discuss different chiral scenarios. Furthermore, we present first preliminary results for the trace anomaly, pressure and energy density. We have studied several discretizations of Euclidean time up to Nt = 12 in order to assess the continuum limit of the trace anomaly. From its interpolation we evaluate the pressure and energy density employing the integral method. Here, we have focussed on two pion masses with mPS ~ 400 and 700 MeV
LatticeQCD using OpenCL
We report on our implementation of LatticeQCD applications using OpenCL. We
focus on the general concept and on distributing different parts on hybrid
systems, consisting of both CPUs (Central Processing Units) and GPUs (Graphic
Processing Units).Comment: 7 pages, 13 figures, proceedings of the XXIX International Symposium
on Lattice Field Theory - Lattice 2011, July 10-16, 2011, Squaw Valley, Lake
Tahoe, Californi
Twisted mass QCD at finite temperature
We discuss the use of Wilson fermions with twisted mass for simulations of QCD thermodynamics.
As a prerequisite for a future analysis of the finite-temperature transition making use
of automatic O(a) improvement, we investigate the phase structure in the space spanned by the
hopping parameter k , the coupling b , and the twisted mass parameter m. We present results for
Nf = 2 degenerate quarks on a 163×8 lattice, for which we investigate the possibility of an Aoki
phase existing at strong coupling and vanishing m, as well as of a thermal phase transition at
moderate gauge couplings and non-vanishing m
Cutoff effects of Wilson fermions on the QCD equation of state to O(g^2)
We compute the O(g^2) contribution to the thermodynamic pressure for Wilson
fermions in the standard, the twisted mass, and clover improved formulation in
lattice perturbation theory, including finite mass effects. We compare the
continuum approaches of these discretizations for the massive ideal and
interacting gas. In all cases, for N_t \geq 8 cutoff effects of Wilson type
fermions are comparable to those of staggered fermions, but asymptotic scaling
requires .Comment: 9 pages, 4 figures. Version shortened to a brief report accepted by
PR
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