Year |
Citation |
Score |
2020 |
Abramczyk M, Blum T, Izubuchi T, Jung C, Lin M, Lytle A, Ohta S, Shintani E, Collaborations U. Nucleon mass and isovector couplings in 2 +1 -flavor dynamical domain-wall lattice QCD near physical mass Physical Review D. 101: 34510. DOI: 10.1103/Physrevd.101.034510 |
0.501 |
|
2011 |
Appelquist T, Fleming GT, Lin MF, Neil ET, Schaich DA. Lattice simulations and infrared conformality Physical Review D - Particles, Fields, Gravitation and Cosmology. 84. DOI: 10.1103/Physrevd.84.054501 |
0.34 |
|
2010 |
Cheng M, Christ NH, Li M, Mawhinney RD, Renfrew D, Hegde P, Karsch F, Lin M, Vranas P. Finite temperature QCD using 2+1 flavors of domain wall fermions at Nt=8 Physical Review D - Particles, Fields, Gravitation and Cosmology. 81. DOI: 10.1103/Physrevd.81.054510 |
0.667 |
|
2008 |
Yamazaki T, Aoki Y, Blum T, Lin H, Lin M, Ohta S, Sasaki S, Tweedie R, Zanotti J. Nucleon axial charge in 2+1 flavor dynamical lattice QCD with domain wall fermions Physical Review Letters. 100: 171602. PMID 18518272 DOI: 10.1103/Physrevlett.100.171602 |
0.366 |
|
2008 |
Antonio DJ, Boyle PA, Blum T, Christ NH, Cohen SD, Dawson C, Izubuchi T, Kenway RD, Jung C, Li S, Lin MF, Mawhinney RD, Noaki J, Ohta S, Pendleton BJ, et al. Neutral-kaon mixing from (2+1)-flavor domain-wall QCD. Physical Review Letters. 100: 032001. PMID 18232967 DOI: 10.1103/Physrevlett.100.032001 |
0.635 |
|
2008 |
Antonio DJ, Bowler KC, Boyle PA, Christ NH, Clark MA, Cohen SD, Dawson C, Hart A, Joó B, Jung C, Kenway RD, Li S, Lin M, Mawhinney RD, Maynard CM, et al. Localization and chiral symmetry in three flavor domain wall QCD Physical Review D - Particles, Fields, Gravitation and Cosmology. 77. DOI: 10.1103/Physrevd.77.014509 |
0.621 |
|
2005 |
Aoki Y, Blum T, Christ N, Dawson C, Hashimoto K, Izubuchi T, Laiho JW, Levkova L, Lin M, Mawhinney R, Noaki J, Ohta S, Orginos K, Soni A. Lattice QCD with two dynamical flavors of domain wall fermions Physical Review D - Particles, Fields, Gravitation and Cosmology. 72. DOI: 10.1103/Physrevd.72.114505 |
0.606 |
|
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