Chiral effective field theory analysis of hadronic parity violation in few-nucleon systems

被引:30
|
作者
Viviani, M. [1 ]
Baroni, A. [2 ]
Girlanda, L. [3 ,4 ]
Kievsky, A. [1 ]
Marcucci, L. E. [1 ,5 ]
Schiavilla, R. [2 ,6 ]
机构
[1] Ist Nazl Fis Nucl, I-56127 Pisa, Italy
[2] Old Dominion Univ, Dept Phys, Norfolk, VA 23529 USA
[3] Univ Salento, Dept Math & Phys, I-73100 Lecce, Italy
[4] Ist Nazl Fis Nucl, I-73100 Lecce, Italy
[5] Univ Pisa, Dept Phys, I-56127 Pisa, Italy
[6] Jefferson Lab, Newport News, VA 23606 USA
来源
PHYSICAL REVIEW C | 2014年 / 89卷 / 06期
关键词
PROTON-PROTON-SCATTERING; PERTURBATION-THEORY; NONCONSERVATION; DYNAMICS; FORCES; GAMMA;
D O I
10.1103/PhysRevC.89.064004
中图分类号
O57 [原子核物理学、高能物理学];
学科分类号
070202 ;
摘要
Background: Weak interactions between quarks induce a parity-violating (PV) component in the nucleon-nucleon potential, whose effects are currently being studied in a number of experiments involving few-nucleon systems. In the present work, we reconsider the derivation of this PV component within a chiral effective field theory (chi EFT) framework. Purpose: The objectives of the present work are twofold. The first is to perform a detailed analysis of the PV nucleon-nucleon potential up to next-to-next-to-leading (N2LO) order in the chiral expansion, in particular, by determining the number of independent low-energy constants (LECs) at N2LO. The second objective is to investigate PV effects in a number of few-nucleon observables, including the (p) over right arrow -p longitudinal asymmetry, the neutron spin rotation in (n) over right arrow -p and (n) over right arrow -d scattering, and the longitudinal asymmetry in the He-3((n) over right arrow, p)H-3 charge-exchange reaction. Methods: The chi EFT PV potential includes one-pion-exchange, two-pion-exchange, and contact terms as well as 1/M (M being the nucleon mass) nonstatic corrections. Dimensional regularization is used to renormalize pion loops. The wave functions for the A = 2-4 nuclei are obtained by using strong two- and three-body potentials also derived, for consistency, from chi EFT. In the case of the A = 3-4 systems, the wave functions are computed by expanding on a hyperspherical harmonics functions basis. Results: We find that the PV potential at N2LO depends on six LECs: the pion-nucleon PV coupling constant h(pi)(1) and five parameters multiplying contact interactions. An estimate for the range of values of the various LECs is provided by using available experimental data, and these values are used to obtain predictions for the other PV observables. Conclusions: The chi EFT approach provides a very satisfactory framework to analyze PV effects in few-nucleon systems.
引用
收藏
页数:27
相关论文
共 50 条
  • [41] FEW BODY NUCLEAR STRUCTURE CALCULATIONS WITH CHIRAL PERTURBATION THEORY NUCLEON-NUCLEON POTENTIAL
    Gajdosik, Thomas
    Germanas, Darius
    Kalinauskas, Romas
    Mickevicius, Saulius
    3RD INTERNATIONAL CONFERENCE RADIATION INTERACTION WITH MATERIAL AND ITS USE IN TECHNOLOGIES 2010, 2010, : 254 - 257
  • [42] Chiral effective field theory for nuclear matter with long- and short-range multi-nucleon interactions
    Oller, J. A.
    Lacour, A.
    Meissner, U-G
    JOURNAL OF PHYSICS G-NUCLEAR AND PARTICLE PHYSICS, 2010, 37 (01)
  • [43] Nuclear axial currents in chiral effective field theory
    Baroni, A.
    Girlanda, L.
    Pastore, S.
    Schiavilla, R.
    Viviani, M.
    PHYSICAL REVIEW C, 2016, 93 (01)
  • [44] Pion production in nucleon-nucleon collisions in chiral effective field theory: Next-to-next-to-leading order contributions
    Filin, A. A.
    Baru, V.
    Epelbaum, E.
    Krebs, H.
    Hanhart, C.
    Kudryavtsev, A. E.
    Myhrer, F.
    PHYSICAL REVIEW C, 2012, 85 (05):
  • [45] Chiral Effective Theory with a Scalar Field
    Tarrus, Jaume
    IX INTERNATIONAL CONFERENCE ON QUARK CONFINEMENT AND THE HADRON SPECTRUM (QCHS IX), 2011, 1343 : 268 - 270
  • [46] Neutrinoless double beta decay in chiral effective field theory: lepton number violation at dimension seven
    Cirigliano, V.
    Dekens, W.
    de Vries, J.
    Graesser, M. L.
    Mereghetti, E.
    JOURNAL OF HIGH ENERGY PHYSICS, 2017, (12):
  • [47] Two-nucleon 1S0 amplitude zero in chiral effective field theory
    Sanchez, M. Sanchez
    Yang, C. -J.
    Long, Bingwei
    van Kolck, U.
    PHYSICAL REVIEW C, 2018, 97 (02)
  • [48] Hyperon-nucleon interaction in chiral effective field theory at next-to-next-to-leading order
    Haidenbauer, Johann
    Meissner, Ulf-G.
    Nogga, Andreas
    Le, Hoai
    EUROPEAN PHYSICAL JOURNAL A, 2023, 59 (03)
  • [49] Chiral effective field theory description of the hyperon-nucleon interaction at next-to-leading order
    Petschauer, S.
    MENU 2013 - 13TH INTERNATIONAL CONFERENCE MESON-NUCLEON PHYSICS AND THE STRUCTURE OF THE NUCLEON, 2014, 73
  • [50] Hyperon-nucleon interaction and baryonic contact terms in SU(3) chiral effective field theory
    Petschauer, S.
    CHIRAL SYMMETRY IN HADRONS AND NUCLEI, 2015, : 177 - 180