Nucleon scalar and tensor charges using lattice QCD simulations at the physical value of the pion mass

被引:45
|
作者
Alexandrou, C. [1 ,2 ]
Constantinou, M. [3 ]
Dimopoulos, P. [4 ,5 ,6 ]
Frezzotti, R. [6 ]
Hadjiyiannakou, K. [2 ]
Jansen, K. [7 ]
Kallidonis, C. [2 ]
Kostrzewa, B. [8 ]
Koutsou, G. [2 ]
Mangin-Brinet, M. [9 ]
Aviles-Casco, A. Vaquero [10 ]
Wenger, U. [11 ]
机构
[1] Univ Cyprus, Dept Phys, POB 20537, CY-1678 Nicosia, Cyprus
[2] Cyprus Inst, Computat Based Sci & Technol Res Ctr, 20 Kavafi St, CY-2121 Nicosia, Cyprus
[3] Temple Univ, Dept Phys, 1925 North 12th St, Philadelphia, PA 19122 USA
[4] Museo Stor Fis, Ctr Fermi, Piazza Viminiale 1, I-00184 Rome, Italy
[5] Ctr Studi & Ric Enrico Fermi, Compendio Viminale, Piazza Viminiale 1, I-00184 Rome, Italy
[6] Univ Roma Tor Vergata, Dipartimento Fis, Via Ric Sci 1, I-00133 Rome, Italy
[7] DESY, NIC, Platanenallee 6, D-15738 Zeuthen, Germany
[8] Rhein Freidrich Wilhelms Univ Bonn, HISKP Theory, D-53115 Bonn, Germany
[9] Lab Phys Subatom & Cosmol, Theory Grp, F-38026 Grenoble, France
[10] Univ Utah, Dept Phys & Astron, Salt Lake City, UT 84112 USA
[11] Univ Bern, Albert Einstein Ctr Fundamental Phys, CH-3012 Bern, Switzerland
基金
欧盟地平线“2020”;
关键词
DARK-MATTER; QUARKS; RENORMALIZATION; FERMIONS;
D O I
10.1103/PhysRevD.95.114514
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We present results on the light, strange and charm nucleon scalar and tensor charges from lattice QCD, using simulations with N-f = 2 flavors of twisted mass clover-improved fermions with a physical value of the pion mass. Both connected and disconnected contributions are included, enabling us to extract the isoscalar, strange and charm charges for the first time directly at the physical point. Furthermore, the renormalization is computed nonperturbatively for both isovector and isoscalar quantities. We investigate excited state effects by analyzing several sink-source time separations and by employing a set of methods to probe ground state dominance. Our final results for the scalar charges are g(S)(u) = 5.20(42)(15)(12), g(S)(d) = 4.27(26) (15)(12), g(S)(s) = 0.33(7)(1)(4), and g(S)(c) = 0.062(13)(3)(5) and for the tensor charges g(T)(u) = 0.794(16)(2)(13), g(T)(d) = - 0.210(10)(2)(13), g(T)(d) = 0.00032(24)(0), and g(T)(c) = 0.00062(85)(0) in the (MS) over bar scheme at 2 GeV. The first error is statistical, the second is the systematic error due to the renormalization and the third the systematic arising from estimating the contamination due to the excited states, when our data are precise enough to probe the first excited state.
引用
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页数:19
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