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2024年10月30日

A relativistic continuum Hartree-Bogoliubov theory description of N=3 isotones

  • The ground-state properties of N=3 isotones and mirror nuclei have been investigated in the Rrelativistic Continuum Hartree-Bogoliubov theory with the NLSH effective interaction. Pairing correlations are taken into account by a density-dependent δ-force. The calculations show that the proton density distributions of 8B and 9C have a long tail, the core has an increasing tendency of 9C and the paired off valence protons make the halo distribution shrink. The cross sections for the 8B(9C)+12C reaction which are consistent with the experimental data are calculated using the Glauber model. On the whole, we think that 8B is a one-proton halo nucleus and 9C is a two-proton halo nucleus.
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  • [1] Tanihata I et al. Phys. Rev. Lett., 1985, 55: 26762 Riisager K. Rev. Mod. Phys., 1994, 66: 11053 Hansen P G, Jensen A S, Jonson B. Ann. Rev. Nucl. Part. Sci., 1995, 45: 5054 Tanihata I. Prog. Part. Nucl. Phys., 1995, 35: 5055 Jensen A S et al. Rev. Mod. Phys., 2004, 76: 2156 Negoita F et al. Phys. Rev. C, 1996, 54: 17877 Smedberg M H, Baumann T, Aumann T et al. Phys. Lett. B, 1999, 452: 18 Fukuda M et al. Nucl. Phys. A, 1999, 656: 2099 Guimaraes V et al. Phys. Rev. Lett., 2000, 84: 186210 Carstoiu F et al. Phys. Rev. C, 2001, 63: 05431011 Chandel S S, Dhiman S K, Shyam R. Phys. Rev. C, 2003, 68: 05432012 Ozawa A et al. Phys. Lett. B, 1994, 334: 1813 Zhukov M V, Thompson I J. Phys. Rev. C, 1995, 52: 350514 LU F et al. Chin. Phys. C (HEP NP), 2009, 33: 17015 Suzuki T, Geissel H, Bochkarev O et al. Nucl. Phys. A, 1997, 616: 286c16 Ozawa A et al. Phys. Rev. C, 2006, 74: 02130117 CHEN J G et al. Chin. Phys. Lett., 2004, 21: 214018 FANG D Q et al. Chin. Phys. Lett., 2005, 22: 57219 REN Z Z, CHEN B Q, MA Z Y, XU G. Phys. Rev. C, 1996, 53: R57220 WANG Z J et al. Science in China. G, 2003, 33: 38521 Ozawa A et al. Nucl. Phys. A, 1996, 608: 6322 Blank B et al. Nucl. Phys. A, 1997, 624: 24223 Lecture Notes in Physics. edited by Lalazissis G A, Ring P, Vretenar D. Springer-Verlag, Heidelberg, 2004. 64124 Kohn W, Sham L J. Phys. Rev. A, 1965, 137: 169725 BAI X H, HU J M. Phys. Rev. C, 1997, 56: 141026 MENG J, Ring P. Phys. Rev. Lett., 1996, 77: 396327 Poschl W et al. Phys. Rev. Lett., 1997, 79: 2028 MENG J. Prog. Part. Nucl. Phys., 2006, 57: 229 MENG J. Nucl. Phys. A, 1998, 635: 330 Audi G, Wapstra A H, Thibault C. Nucl. Phys. A, 2003, 52: 301331 WANG C B et al. Comm. Theor. Phys., 2009, 51: 895
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HAN Rui, JI Juan-Xia and LI Jia-Xing. A relativistic continuum Hartree-Bogoliubov theory description of N=3 isotones[J]. Chinese Physics C, 2011, 35(9): 821-824. doi: 10.1088/1674-1137/35/9/006
HAN Rui, JI Juan-Xia and LI Jia-Xing. A relativistic continuum Hartree-Bogoliubov theory description of N=3 isotones[J]. Chinese Physics C, 2011, 35(9): 821-824.  doi: 10.1088/1674-1137/35/9/006 shu
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Received: 2010-12-09
Revised: 2010-12-30
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A relativistic continuum Hartree-Bogoliubov theory description of N=3 isotones

    Corresponding author: LI Jia-Xing,

Abstract: The ground-state properties of N=3 isotones and mirror nuclei have been investigated in the Rrelativistic Continuum Hartree-Bogoliubov theory with the NLSH effective interaction. Pairing correlations are taken into account by a density-dependent δ-force. The calculations show that the proton density distributions of 8B and 9C have a long tail, the core has an increasing tendency of 9C and the paired off valence protons make the halo distribution shrink. The cross sections for the 8B(9C)+12C reaction which are consistent with the experimental data are calculated using the Glauber model. On the whole, we think that 8B is a one-proton halo nucleus and 9C is a two-proton halo nucleus.

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