Parallel Supercomputing PC Cluster and Some Physical Results in Lattice QCD
摘要
We describe the construction of a high performance parallel computer composed of PC components, present some physical results for light hadron and hybrid meson masses from lattice QCD. We also show that the smearing technique is very useful for improving the spectrum calculations.
参考文献21
-
1X Q Luo. Comput Phys Commun. 94 (1996) 119.
-
2X Q Luo and Q Z Chen. Mod Phys Lett. A11 (1996)2435.
-
3X Q Luo, Q Z Chen, S H Guo, X Y Fang, and J M Liu. Nucl Phys . B53 (Proc Suppl) (1997) 243.
-
4X Q Luo and E B Gregory, et al. Non-perturbative Methods and Lattice QCD, World Scientific, Singapore (2001)308.
-
5X Q Luo, Mod Phys Lett. A16 (2001) 1615.
-
6E B Gregory, S H Guo, H Kroger, and X Q Luo. Phys Rev. D62 (2000) 054508.
-
7X Q Luo, E B Gregory, S H Guo, and H Kroge,arXiv:hep-ph/0011120.
-
8C Q Huang, X Q Luo, H Kroger, and K J Moriarty.Phys Lett. A299 (2002) 483.
-
9S Catterall and E B Gregory. Phys Lett. B487 (2000)349.
-
10H Jirari, H Kroger, X Q Luo, and K Moriarty. Phys Lett. A281 (2001) 1.
-
1树华.物理学家发现新介子[J].物理,2005,34(12):943-948.
-
2梅仲豪 EricB.GREGORY.Light Hadron Masses in Quantum Chromodynamics with Valence Wilson Quarks at β=6.25 from a Parallel PC Cluster[J].Chinese Physics Letters,2002,19(5):636-639.
-
3Zdenka RIE■ANOV.States on sharply dominating effect algebras[J].Science China Mathematics,2008,51(5):907-914. 被引量:1
-
4黄东阳,谭平,周福霖,颜学渊.Dynamic analysis on tuned hybrid-tanks/mass damper[J].Journal of Harbin Institute of Technology(New Series),2010,17(2):166-170.
-
5泰庆华.Hybrid-Trefftz有限元简介和展望[J].力学与实践,1993,15(3):20-22. 被引量:1
-
6刘汇慧,张晓菲,陈江川.Direct Measurement of Branching Fraction for Inclusive Semimuonic Decay of Neutral D Mesons[J].Chinese Physics Letters,2009,26(6):84-86.
-
7王福军,Y.T.FENG,D.R.J.OWEN,张静,刘洋.PARALLEL ANALYSIS OF COMBINED FINITE/DISCRETE ELEMENT SYSTEMS ON PC CLUSTER[J].Acta Mechanica Sinica,2004,20(5):534-540. 被引量:5
-
8LIGHT UNFLAVORED MESONS (S = C= B = 0)[J].Chinese Physics C,2014,38(9):34-78.
-
9K.A.Olive.LIGHT UNFLAVORED MESONS(S=C=B=0)For I=1(π,b,ρ,a):ud,(uu-dd)/2^(1/2),du;for I=0(η,η',h,h',ω,Φ,f,f'):c_1(u+dd)+c_2(s)[J].Chinese Physics C,2014,38(9):773-894.
-
10刘福虎.Anisotropic emission of charged mesons and structure characteristic of emission source in heavy ion collisions at 1-2A GeV[J].Chinese Physics B,2008,17(3):883-895.