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Spherical nucleus 40Ca is important structural and alloy material nucleus. Based on important theoretical value and application prospect of nuclear data of calcium isotopes, nucleon-nucleus scattering data on 40Ca nucleus, the main isotopes of natural calcium, are calculated by using dispersive optical model (DOM). The dispersive optical model potential is defined by energy-dependent real potentials, imaginary potentials, and also by the corresponding dispersive contributions to the real potential which are calculated analytically from the corresponding imaginary potentials by using a dispersion relation that follow from the requirement of causality. By fit simultaneously scattering experimental data for neutron and proton, an isospin-dependent dispersive optical model potential containing a dispersive term is derived. This derived potential in this work considers the nonlocality in the real “Hartree-Fock” potential
$ V_{\rm{HF}} $ and introduces the shell gap in the definition of nuclear imaginary volume, surface and spin-orbit potentials near the Fermi energy. This dispersive optical model potential shows a good description of nucleon-nucleus scattering data on 40Ca nucleus up to 200 MeV including neutron total cross sections, neutron elastic scattering angular distributions, proton elastic scattering angular distributions, neutron analyzing powers and proton analyzing powers. In addition, the energy dependencies of calculated real volume integrals of dispersive optical model potential is shown, and a typical dispersive hump is seen around the Fermi energy. This dispersive hump behavior naturally obtained from dispersion relations, and allows the dispersion optical potential to get rid of energy dependent geometry, thus avoiding the use of a radius dependent on energy.-
Keywords:
- nucleon scattering /
- dispersive optical model /
- elastic scattering
[1] Koning A J, Delaroche J P 2003 Nucl. Phys. A 713 231Google Scholar
[2] Mahaux C, Sartor R 1986 Phys. Rev. Lett. 57 3015Google Scholar
[3] Morillon B, Romain P 2004 Phys. Rev. C 70 014601Google Scholar
[4] Morillon B, Romain P 2006 Phys. Rev. C 74 014601Google Scholar
[5] Soukhovitskiĩ E Sh, Capote R, Quesada J M, Chiba S 2005 Phys. Rev. C 72 024604Google Scholar
[6] Capote R, Soukhovitskiĩ E Sh, Quesada J M, Chiba S 2005 Phys. Rev. C 72 064610Google Scholar
[7] Hao L J, Sun W L, Soukhovitskiĩ E Sh 2008 J. Phys. G: Nucl. Part. Phys. 35 095103Google Scholar
[8] Capote R, Herman M, Obložinský P, Young P G, Goriely S, Belgya T, Ignatyuk A V, Koning A J, Hilaire S, Plujko V A, Avrigeanu M, Bersillon O, Chadwick M B, Fukahori T, Ge Z G, Han Y L, Kailas S, Kopecky J, Maslov V M, Reffo G, Sin G, Soukhovitskii E Sh, Talou P 2009 Nucl. Data Sheets 110 3107Google Scholar
[9] Soukhovitskiĩ E Sh, Capote R, Quesada J M, Chiba S, Martyanov D S 2016 Phys. Rev. C 94 064605Google Scholar
[10] Dickhoff W H, Charity R J 2019 Prog. Part. Nucl. Phys. 105 252Google Scholar
[11] Zhao X N, Sun W L, Soukhovitskiĩ E Sh, Martyanov D S, Quesada J M, Capote R 2019 J. Phys. G: Nucl. Part. Phys. 46 055103Google Scholar
[12] Zhao X N, Sun W L, Capote R, Soukhovitskiĩ E Sh, Martyanov D S, Quesada J M 2020 Phys. Rev. C 101 064618Google Scholar
[13] Zhao X N, Du W Q, Capote R, Soukhovitskiĩ E Sh 2023 Phys. Rev. C 107 064606Google Scholar
[14] Perey F, Buck B 1962 Nucl. Phys. 32 353Google Scholar
[15] Brown G E, Rho M 1981 Nucl. Phys. A 372 397Google Scholar
[16] Delaroche J P, Wang Y, Rapaport J 1989 Phys. Rev. C 39 391Google Scholar
[17] Molina A, Capote R, Quesada J M, Lozano M 2002 Phys. Rev. C 65 034616Google Scholar
[18] Mahaux C, Sartor R 1991 Nucl. Phys. A 528 253Google Scholar
[19] Lane A M 1962 Phys. Rev. Lett. 8 171Google Scholar
[20] Lane A M 1962 Nucl. Phys. 35 676Google Scholar
[21] Sukhovitskiĩ E Sh, Lee Y O, Chang J, Chiba S, Iwamoto O 2000 Phys. Rev. C 62 044605Google Scholar
[22] EXchange FORmat database (EXFOR) is maintained by the Network of Nuclear Reaction Data Centers (see www-nds.iaea.org/nrdc/). Data available online (e.g., at www-nds.iaea.org/exfor/).
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图 7 40Ca的中子诱发核反应计算中DOM势实部体积分随能量的变化情况, 其中右边纵坐标度量
$V_{\rm{HF}}$ 势和总的实部势, 左边纵坐标度量色散修正项Fig. 7. Energy dependencies of calculated real volume integrals of dispersive optical model potential for neutron induced reactions on 40Ca. Volume integrals of and total real potential by using right Y-axis, the volume integrals of dispersive terms by using left Y-axis.
表 1 40Ca中子诱发核反应计算中的DOM势参数
Table 1. DOM potential parameters for nucleon induced reactions on 40Ca.
Volume Surface Spin-orbit couple Coulomb Real $V_{0}$ = 85.93$\rm{MeV}$ $ V_{\rm{so} } $ = 6.1$\rm{MeV}$ $C_{\rm{Coul}}$ = 1.0$\rm{MeV}$ potential $\lambda_{\rm{HF}}$ = 0.94$\rm{MeV}^{-1}$ Dispersive $ \lambda_{\rm{so} } $ = 0.004$\rm{MeV}^{-1}$ $ C_{\rm{viso} } $ = 24$\rm{MeV}$ Imaginary $A_{\rm{v}}$ = 13.36$\rm{MeV}$ $W_{0}$ = 17.67$\rm{MeV}$ $ W_{\rm{so} } $ = –3.1$\rm{MeV}$ potential $B_{\rm{v}}$ = 86.63$\rm{MeV}$ $B_{\rm{s}}$ = 11.74$\rm{MeV}$ $ B_{\rm{so} } $ = 160$\rm{MeV}$ $E_{\rm{a}}$ = 56$\rm{MeV}$ $C_{\rm{s}}$ = 0.02$\rm{MeV}^{-1}$ α = 0.380$\rm{MeV}^{1/2}$ $ C_{\rm{wiso} } $ = 22$\rm{MeV}$ Potential $r_{\rm{HF}}$ = 1.26$\rm{fm}$ $r_{\rm{s}}$ = 1.22$\rm{fm}$ $ r_{\rm{so} } $ = 1.35$\rm{fm}$ $r_{\rm{c}}$ = 1.03$\rm{fm}$ geometry $a_{\rm{HF}}$ = 0.622$\rm{fm}$ $a_{\rm{s}}$ = 0.502$\rm{fm}$ $ a_{\rm{so} } $ = 0.682$\rm{fm}$ $a_{\rm{c}}$ = 0.252$\rm{fm}$ $r_{\rm{v}}$ = 1.34$\rm{fm}$ $a_{\rm{v}}$ = 0.675$\rm{fm}$ -
[1] Koning A J, Delaroche J P 2003 Nucl. Phys. A 713 231Google Scholar
[2] Mahaux C, Sartor R 1986 Phys. Rev. Lett. 57 3015Google Scholar
[3] Morillon B, Romain P 2004 Phys. Rev. C 70 014601Google Scholar
[4] Morillon B, Romain P 2006 Phys. Rev. C 74 014601Google Scholar
[5] Soukhovitskiĩ E Sh, Capote R, Quesada J M, Chiba S 2005 Phys. Rev. C 72 024604Google Scholar
[6] Capote R, Soukhovitskiĩ E Sh, Quesada J M, Chiba S 2005 Phys. Rev. C 72 064610Google Scholar
[7] Hao L J, Sun W L, Soukhovitskiĩ E Sh 2008 J. Phys. G: Nucl. Part. Phys. 35 095103Google Scholar
[8] Capote R, Herman M, Obložinský P, Young P G, Goriely S, Belgya T, Ignatyuk A V, Koning A J, Hilaire S, Plujko V A, Avrigeanu M, Bersillon O, Chadwick M B, Fukahori T, Ge Z G, Han Y L, Kailas S, Kopecky J, Maslov V M, Reffo G, Sin G, Soukhovitskii E Sh, Talou P 2009 Nucl. Data Sheets 110 3107Google Scholar
[9] Soukhovitskiĩ E Sh, Capote R, Quesada J M, Chiba S, Martyanov D S 2016 Phys. Rev. C 94 064605Google Scholar
[10] Dickhoff W H, Charity R J 2019 Prog. Part. Nucl. Phys. 105 252Google Scholar
[11] Zhao X N, Sun W L, Soukhovitskiĩ E Sh, Martyanov D S, Quesada J M, Capote R 2019 J. Phys. G: Nucl. Part. Phys. 46 055103Google Scholar
[12] Zhao X N, Sun W L, Capote R, Soukhovitskiĩ E Sh, Martyanov D S, Quesada J M 2020 Phys. Rev. C 101 064618Google Scholar
[13] Zhao X N, Du W Q, Capote R, Soukhovitskiĩ E Sh 2023 Phys. Rev. C 107 064606Google Scholar
[14] Perey F, Buck B 1962 Nucl. Phys. 32 353Google Scholar
[15] Brown G E, Rho M 1981 Nucl. Phys. A 372 397Google Scholar
[16] Delaroche J P, Wang Y, Rapaport J 1989 Phys. Rev. C 39 391Google Scholar
[17] Molina A, Capote R, Quesada J M, Lozano M 2002 Phys. Rev. C 65 034616Google Scholar
[18] Mahaux C, Sartor R 1991 Nucl. Phys. A 528 253Google Scholar
[19] Lane A M 1962 Phys. Rev. Lett. 8 171Google Scholar
[20] Lane A M 1962 Nucl. Phys. 35 676Google Scholar
[21] Sukhovitskiĩ E Sh, Lee Y O, Chang J, Chiba S, Iwamoto O 2000 Phys. Rev. C 62 044605Google Scholar
[22] EXchange FORmat database (EXFOR) is maintained by the Network of Nuclear Reaction Data Centers (see www-nds.iaea.org/nrdc/). Data available online (e.g., at www-nds.iaea.org/exfor/).
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