Finite size effect on vector meson and baryon sectors in 2+1 flavor QCD at the physical point

被引:5
作者
Ishikawa, K. -I. [1 ]
Ishizuka, N. [2 ]
Kuramashi, Y. [2 ]
Nakamura, Y. [3 ]
Namekawa, Y. [4 ]
Shintani, E. [3 ]
Taniguchi, Y. [2 ]
Ukita, N. [2 ]
Yamazaki, T. [5 ]
Yoshie, T. [2 ]
机构
[1] Hiroshima Univ, Grad Sch Sci, Higashihiroshima, Hiroshima 7398526, Japan
[2] Univ Tsukuba, Ctr Computat Sci, Tsukuba, Ibaraki 3058577, Japan
[3] RIKEN Ctr Computat Sci, Kobe, Hyogo 6500047, Japan
[4] High Energy Accelerator Res Org KEK, Tsukuba, Ibaraki 3050801, Japan
[5] Univ Tsukuba, Fac Pure & Appl Sci, Tsukuba, Ibaraki 3058571, Japan
关键词
LATTICE QCD; MASSES;
D O I
10.1103/PhysRevD.100.094502
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We investigate the finite size effect on the vector meson and the baryon sectors using a subset of the "PACS10" configurations which are generated, keeping the space-time volumes over (10 fm)(4) in 2 + 1 flavor QCD at the physical point. Comparing the results on (5.5 fm)(4) and (10.9 fm)(4) lattices, the ground states of octet baryons, which are stable on the lattice, show no finite size effect within less than 0.5% level of statistical errors. For those of vector mesons, which are unstable on the lattice, we observe that the effective masses are well below the experimental resonance levels both on (5.5 fm)(4) and (10.9 fm)(4) lattices. For the decuplet baryon sector, we have found that the time dependence of the effective mass looks quite similar to that for the vector meson sector, including the Omega baryon channel. We discuss its origin due to a possible mixing with the nearby multihadron states. Since the Xi baryon mass can be determined with the smallest ambiguity among the vector meson and the baryon masses, we use it together with the pion and kaon masses as the physical inputs to determine the physical point.
引用
收藏
页数:9
相关论文
共 27 条
[1]  
[Anonymous], 2012, POS LATTICE2012
[2]  
[Anonymous], ARXIV11117054
[3]   Light hadron spectrum and quark masses from quenched lattice QCD -: art. no. 034503 [J].
Aoki, S ;
Boyd, G ;
Burkhalter, R ;
Ejiri, S ;
Fukugita, M ;
Hashimoto, S ;
Iwasaki, Y ;
Kanaya, K ;
Kaneko, T ;
Kuramashi, Y ;
Nagai, K ;
Okawa, M ;
Shanahan, HP ;
Ukawa, A ;
Yoshié, T .
PHYSICAL REVIEW D, 2003, 67 (03)
[4]   Physical point simulation in 2+1 flavor lattice QCD [J].
Aoki, S. ;
Ishikawa, K. -I. ;
Ishizuka, N. ;
Izubuchi, T. ;
Kadoh, D. ;
Kanaya, K. ;
Kuramashi, Y. ;
Namekawa, Y. ;
Okawa, M. ;
Taniguchi, Y. ;
Ukawa, A. ;
Ukita, N. ;
Yamazaki, T. ;
Yoshie, T. .
PHYSICAL REVIEW D, 2010, 81 (07)
[5]   2+1 flavor lattice QCD toward the physical point [J].
Aoki, S. ;
Ishikawa, K. -I. ;
Ishizuka, N. ;
Izubuchi, T. ;
Kadoh, D. ;
Kanaya, K. ;
Kuramashi, Y. ;
Namekawa, Y. ;
Okawa, M. ;
Taniguchi, Y. ;
Ukawa, A. ;
Ukita, N. ;
Yoshie, T. .
PHYSICAL REVIEW D, 2009, 79 (03)
[6]   Continuum limit physics from 2+1 flavor domain wall QCD [J].
Aoki, Y. ;
Arthur, R. ;
Blum, T. ;
Boyle, P. A. ;
Broemmel, D. ;
Christ, N. H. ;
Dawson, C. ;
Flynn, J. M. ;
Izubuchi, T. ;
Jin, X-Y. ;
Jung, C. ;
Kelly, C. ;
Li, M. ;
Lichtl, A. ;
Lightman, M. ;
Lin, M. F. ;
Mawhinney, R. D. ;
Maynard, C. M. ;
Ohta, S. ;
Pendleton, B. J. ;
Sachrajda, C. T. ;
Scholz, E. E. ;
Soni, A. ;
Wennekers, J. ;
Zanotti, J. M. ;
Zhou, R. .
PHYSICAL REVIEW D, 2011, 83 (07)
[7]   Finite volume effects for meson masses and decay constants [J].
Colangelo, G ;
Dürr, S ;
Haefeli, C .
NUCLEAR PHYSICS B, 2005, 721 :136-174
[8]   HADRON SCATTERING LENGTHS IN LATTICE QCD [J].
FUKUGITA, M ;
KURAMASHI, Y ;
OKAWA, M ;
MINO, H ;
UKAWA, A .
PHYSICAL REVIEW D, 1995, 52 (05) :3003-3023
[9]  
Giusti L, 2019, EUR PHYS J C, V79, DOI 10.1140/epjc/s10052-019-6706-7
[10]   Strangeness and charmness content of the nucleon from overlap fermions on 2+1-flavor domain-wall fermion configurations [J].
Gong, M. ;
Alexandru, A. ;
Chen, Y. ;
Doi, T. ;
Dong, S. J. ;
Draper, T. ;
Freeman, W. ;
Glatzmaier, M. ;
Li, A. ;
Liu, K. F. ;
Liu, Z. .
PHYSICAL REVIEW D, 2013, 88 (01)