The dynamical QCD configurations with 2 flavors of overlap fermions listed below were generated by JLQCD Collaboration on supercomputers IBM Blue Gene/L at High Energy Accelerator Research Organization (KEK).
These gauge configurations are generated with an overlap fermion action and a renormalization-group improved gauge action accompanied by an extra Wilson fermion term. The extra Wilson fermion term fixes the topological charge of the system, and are considered as a part of the gauge action. The values of parameters are as follows; The gauge coupling: β= 6/g2=2.3, the negative mass of the Wilson kernel (domain-wall height): M0=1.6, twisted mass of the topology fixing term: μ = 0.2.
For the overlap-Dirac operator, the sign function of the hermitian Wilson kernel is approximated by the Zolotarev's partially fractional approximation. The number of poles, Npoly, is set to 10 in this work. The Zolotarev approximation is applied to the region |HW| > 0.108, and for the eigenvalues in the range [-0.108, 0.108] the eigenvectors are determined so as to treat the sign function of these modes exactly. The boundary conditions are periodic for all the directions.
The extra Wilson term is introduced to fix the topological charge of the system. The determinant of the hermitian Wilson kernel (HW)2 with the same mass parameter as in the overlap operator suppresses the near-zero modes of HW, and forbids the change of the topological charge. To decrease the effect of high mode region of HW, a determinant of twisted mass ghost is also introduced. The twisted mass parameter is set as μ=0.2 throughout this work.
The lattice size is 163x32, corresponding to the physical spatial size of about 1.9 fm. We have six ensembles corresponding to six quark mass which roughly covers (ms/6, ms). The corresponding lattice spacing, a∼0.12 fm, is set by the Sommer's hadronic radius r0=0.49 fm. All the currently available configurations have the topological charge 0.
Simulations were carried out with the hybrid Monte Carlo (HMC) algorithm. The mass preconditioning is applied to the overlap fermions together with the multi-time step. The trajectory length is τ=0.5. Two types of algorithms were applied. The one algorithm adopts the nested CG algorithm for the overlap solver, and the sign function of low-lying eigenmodes of HW is treated exactly during molecular dynamics as well as the Hamiltonian calculations. The other algorithm uses 5-dimensional CG algorithm for the overlap solver without determination of low-lying eigenvalues of HW. This effect is removed by applying the noisy Metropolis test after the usual Metropolis test of HMC, so the treatment of the low-lying modes in the sign function is finally made exact. These two algorithms are denoted '4D' and '5D' in the table of the next section.
lattice
sizeβ m0 μ a [fm] La [fm] mud Npoly Q τ 163x32 2.30 1.6 0.2 0.1184(21) 1.894(33) 0.015 10 0 0.5 0.025 10 0 0.5 0.035 10 0 0.5 0.050 10 0 0.5 0.070 10 0 0.5 0.100 10 0 0.5
The table below gives a list of ensembles of configurations. A consecutive set of trajectories for a given values of lattice size, β, m0, μ, mud and Q is called an 'ensemble'. A 'series' name (a, b) is given to distinguish the series of configurations sequentially generated with different series of random numbers. Each configuration is separated by 10 trajectories of length 0.5.
lattice
sizeβ m0 μ mud Q series algorithm traj. range #config total
#configsize/config
[MB]total
[GB]163x32 2.30 1.6 0.2 0.015 0 a
a
b
b4D
5D
4D
5D000042-000201
005001-005370
002042-002161
007001-007350160
370
120
3501000 75.5 75.5 163x32 2.30 1.6 0.2 0.025 0 a
a
b
b4D
5D
4D
5D000042-000361
005001-005300
002042-002241
007001-007180320
300
200
1801000 75.5 75.5 163x32 2.30 1.6 0.2 0.035 0 a
a4D
5D000042-000501
005001-005540460
5401000 75.5 75.5 163x32 2.30 1.6 0.2 0.050 0 a
a4D
5D000042-000521
005001-005520480
5201000 75.5 75.5 163x32 2.30 1.6 0.2 0.070 0 a
a4D
5D000042-000491
005001-005550450
5501000 75.5 75.5 163x32 2.30 1.6 0.2 0.100 0 a
a4D
5D000042-000501
005001-005540460
5401000 75.5 75.5
An ensemble is identified by markovChainURI named e.g. as
A configuration is labeled by dataLFN named e.g. as
Basename of the dataLFN is formated as
RgOvr_[spatial size]x[temporal size]_[beta]_[kernel mass]_[quark mass]_[topological charge]-series-trajectory number
To get full list of markovChainURIs and LFNs, please use QCDml faceted navigation.
Configurations are placed in the Gfarm directory
and classified in terms of the basename of markovChainURI. Filename is the same as basename of dataLFN.
All ensemble and configuration
XML files can be found in