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《中国物理C》(英文)编辑部
2024年10月30日

DBHF Approach and Thermodynamic Consistency for Nuclear Matter Calculations

  • Within the framework of Dirac Brueckner-Hartree-Fock (DBHF) approach, we calculate the energy per nucleon, the pressure, the nucleon self-energy and the single-nucleon energy in the nuclear matter by adopting two different covariant representations for T-matrix. We mainly investigate the influence of different covariant representations on the satisfiable extent of the Hugenholtz-Van Hove (HVH) theorem in the nuclear medium in the framework of DBHF. By adopting the two different covariant representations of T-matrix, the predicted nucleon self-energy shows a quite different momentum and density dependence. Different covariant representations affect remarkably the satisfiable extent of the HVH theorem. By adopting the complete pseudo-vector representation of the T-matrix, HVH theorem is largely violated, which is in agreement with the result in the non-relativistic Brueckner-Hartree-Fock approach and reflects the importance of ground state correlations for single nucleon properties in nuclear medium, whereas by using the pseudo-scalar representation, the ground state correlation cannot be shown. It indicates that the complete pseudo-vector presentation is more feasible than the pseudo-scalar one.
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  • [1] . Fuchs C. Lect. Notes. Phys., 2004, 641: 1192. Anastasio M R, Celenza L S, Shakin C M. Phys. Rev. Lett.,1980, 45: 2096; Anastasio M R, Celenza L S, Pong W S etal. Phys. Rep., 1983, 100: 3273. Machleidt R. Adv. Nucl. Phys., 1986, 19: 189; BrockmannR, Machleidt R. Phys. Rev., 1990, C42: 19654. Horowitz C J, Serot B D. Nucl. Phys., 1987, A464: 6135. Haar B T, Maliet R. Phys. Rep., 1987, 149: 207; Phys.Rev. Lett., 1987, 59: 16526. Sehn L, Fuchs C, Faessler A. Phys. Rev., 1997, C56: 2167. Fuchs C et al. Phys. Rev., 1998, C58: 20228. Gross-Boelting T, Fuchs C, Faessler A. Nucl. Phys., 1999,A648: 1059. Jong F D, Lenske H. Phys. Rev., 1998, C58: 89010. Serot B D, Walecka J D. Adv. Nucl. Phys., 1986, 16: 111. MA Z Y, LIU L. Phys. Rev., 2002, C66: 02432112. Tjon J A, Wallace S J. Phys. Rev., 1985, C32: 26713. Hugenholtz N M, Hove L V. Physica (Amsterdam), 1958,24: 36314. ZUO W, Bombaci I, Lombardo U. Phys. Rev., 1999, C60:024605; ZUO W, Lombardo U, LI Z H et al. HEP NP, 2003, 27: 31(in Chinese)(左维, Lombardo U, 李增花等. 高能物理与核物理, 2003, 27: 31)15. Salpeter E E, Bethe H A. Phys. Rev., 1951, 84: 123216. Brown G E, Weise W, Baym G et al. Comments Nucl. Phys., 1987, 17: 3917. ZUO W, Lejeune A, Lombardo U et al. Nucl. Phys., 2002, A706: 418; ZUO W, Lombardo U. HEP NP, 2002, 26: 1134(in Chinese)(左维, Lombardo U. 高能物理与核物理, 2002, 26: 1134); ZUO W et al. HEP NP, 2005, 29: 1061(in Chinese)(左维等. 高能物理与核物理, 2005, 29: 1061)18. Yaes R J. Phys. Rev., 1971, D3: 3086; Brockmann R, Machleidt R. The Dirac-Brueckner Approach. In NuclearMethods and the Nuclear Equation of State. Baldo M ed.Singapore: World Scienti c, 1999. 12119. Thompson R H. Phys. Rev., 1970, D1: 11020. Blankenbecler R, Sugar R. Phys. Rev., 1966, 142: 1051; Partovi M H, Lomon E L. Phys. Rev., 1970, D2: 199921. Bethe H A, Brandow B H, Petschek A G. Phys. Rev., 1963, 129: 225; Baldo M. The Many-body Theory of the Nu-clear EOS. In Nuclear Methods and the Nuclear Equationof State. Baldo M ed. Singapore: World Scienti c, 1999. 122. Jeukenne J P, Lejeune A, Mahaux C. Phys. Rep., 1976, 25C: 8323. Baldo M, Bombaci I, Ferreira L S et al. Phys. Lett., 1988, B209: 13524. Hufner J, Mahaux C. Ann. Phys., 1972, 73: 525; Grang_eP, Cugnon J, Lejeune A. Nucl. Phys., 1987, A473: 36525. ZUO W, Lombardo U, Schulze H J. Phys. Lett., 1998, B432: 24126. ZUO W, Giansiracusa G, Lombardo U. Phys. Lett., 1998, B421: 127. Kondratyuk S, Scholten O. Phys. Rev., 1999, C59: 107028. Frick T, Gad Kh, Muther H. Phys. Rev., 2002, 65: 03432129. Baldo M, Bombaci I, Giansiracusa G et al. Phys. Rev., 1990, C41: 174830. Baldo M, Bombaci I, Giansiracusa G et al. Nucl. Phys., 1991, A530: 135
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LUO Pei-Yan, ZUO Wei, LI Zeng-Hua, YONG Gao-Chan and XU Zhong-Feng. DBHF Approach and Thermodynamic Consistency for Nuclear Matter Calculations[J]. Chinese Physics C, 2006, 30(10): 976-982.
LUO Pei-Yan, ZUO Wei, LI Zeng-Hua, YONG Gao-Chan and XU Zhong-Feng. DBHF Approach and Thermodynamic Consistency for Nuclear Matter Calculations[J]. Chinese Physics C, 2006, 30(10): 976-982. shu
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Received: 2005-12-26
Revised: 2006-01-23
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DBHF Approach and Thermodynamic Consistency for Nuclear Matter Calculations

    Corresponding author: ZUO Wei,
  • Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, China2 Graduate University of Chinese Academy of Sciences, Beijing 100049, China

Abstract: Within the framework of Dirac Brueckner-Hartree-Fock (DBHF) approach, we calculate the energy per nucleon, the pressure, the nucleon self-energy and the single-nucleon energy in the nuclear matter by adopting two different covariant representations for T-matrix. We mainly investigate the influence of different covariant representations on the satisfiable extent of the Hugenholtz-Van Hove (HVH) theorem in the nuclear medium in the framework of DBHF. By adopting the two different covariant representations of T-matrix, the predicted nucleon self-energy shows a quite different momentum and density dependence. Different covariant representations affect remarkably the satisfiable extent of the HVH theorem. By adopting the complete pseudo-vector representation of the T-matrix, HVH theorem is largely violated, which is in agreement with the result in the non-relativistic Brueckner-Hartree-Fock approach and reflects the importance of ground state correlations for single nucleon properties in nuclear medium, whereas by using the pseudo-scalar representation, the ground state correlation cannot be shown. It indicates that the complete pseudo-vector presentation is more feasible than the pseudo-scalar one.

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