Electromagnetic structure of A=2 and 3 nuclei in chiral effective field theory

被引:92
|
作者
Piarulli, M. [1 ]
Girlanda, L. [2 ,3 ]
Marcucci, L. E. [4 ,5 ]
Pastore, S. [6 ]
Schiavilla, R. [1 ,7 ]
Viviani, M. [5 ]
机构
[1] Old Dominion Univ, Dept Phys, Norfolk, VA 23529 USA
[2] Univ Salento, Dept Math & Phys, I-73100 Lecce, Italy
[3] INFN Lecce, I-73100 Lecce, Italy
[4] Univ Pisa, Dept Phys, I-56127 Pisa, Italy
[5] INFN Pisa, I-56127 Pisa, Italy
[6] Argonne Natl Lab, Div Phys, Argonne, IL 60439 USA
[7] Jefferson Lab, Newport News, VA 23606 USA
来源
PHYSICAL REVIEW C | 2013年 / 87卷 / 01期
关键词
ELECTRON-DEUTERON SCATTERING; MAGNETIC FORM-FACTORS; TENSOR POLARIZATION; Q2; TARGET;
D O I
10.1103/PhysRevC.87.014006
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: The A = 2 and 3 form factors are among the observables of choice for testing models of nuclear interactions and associated electromagnetic charge and current operators. Here we investigate the validity of the chiral-effective-field-theory (chi EFT) approach to describe the strong-interaction dynamics in these few-nucleon systems and their response to electromagnetic probes. Purpose: The objectives of the presentwork are twofold. The first is to address and resolve some of the differences present in independent, chi EFT derivations up to one loop, recently appearing in the literature, of the nuclear charge and current operators. The second objective is to provide a complete set of chi EFT and hybrid predictions for the structure functions and tensor polarization of the deuteron, for the charge and magnetic form factors of He-3 and H-3, and for the charge and magnetic radii of these few-nucleon systems. Methods: The calculations use wave functions derived from either chiral or conventional two-and three-nucleon potentials and Monte Carlo methods to evaluate the relevant matrix elements. Results: In reference to the two objectives mentioned earlier, we find that (i) there are no differences between the chi EFT magnetic dipole operator at one loop derived in our formalism and that obtained by Kolling et al. [Phys. Rev. C 80, 045502 (2009)] with the unitary transformation method and (ii) there is excellent agreement between theory and experiment for the static properties and elastic form factors of these A = 2 and 3 nuclei up to momentum transfers q less than or similar to 2.0-2.5 fm(-1). A complete analysis of the results is provided. Conclusions: Nuclear chi EFT provides a very satisfactory description of the isoscalar and isovector charge and magnetic structure of the A = 2 and 3 nuclei at low momentum transfers q less than or similar to 3m(pi). In particular, contributions from two-body charge and current operators are crucial for bringing theory into close agreement with experiment. At higher q values the present chi EFT predictions are similar to those obtained in the hybrid approach, as well as in older studies based on the conventional meson-exchange picture, and fail to reproduce the measured A = 2 and 3 form factors in the diffraction region. DOI: 10.1103/PhysRevC.87.014006
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页数:24
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