Skyrme-Hartree-Fock results for 17 Neon


* Last modification (y/m/d):2011/11/17,18,19
This directory contains the results of Hartree-Fock calculations for Neon 17: HF calculations were done with the Skyrme Msk7, S3, SG2, SkM*, SkSC4, and SLy4 forces in the Catresian-mesh representation with a mesh spacing of 0.5fm and a cubic box=0.5fm*(50,50,50). (i.e., the length of the edge is 25 fm.) An octant of a nucleus is placed at a corner of the box, imposing D_{2h} symmetry. Nearest boundary is located at 25 fm from the center of the nucleus. The furtherst point in the box is located at 25fm*sqrt(3) from the center of the nucleus.

Summary table of the results of the calculations


N=7, Z=10 (17Ne)

[force]   [energy]     [Qz]   [gamma] deformation parameter      r.m.s. radius (fm)    [files]
             (MeV)     (fm^2)  (deg)  [mass][neutr][proto]    [mass][neutron] [proton]
ground state
  msk7    -119.530     21.798  180.000 -0.127 -0.096 -0.146   2.7471   2.5835   2.8560  detail RDP
    s3    -115.714     35.939    0.000  0.210  0.140  0.249   2.7498   2.5800   2.8627  detail RDP
   sg2    -126.379     38.930    0.000  0.228  0.149  0.274   2.7420   2.5709   2.8557  detail RDP
  skm*    -117.848     36.855    0.000  0.208  0.133  0.250   2.7985   2.6151   2.9200  detail RDP
 sksc4    -117.555     21.600  180.000 -0.127 -0.095 -0.145   2.7419   2.5761   2.8523  detail RDP
  sly4    -116.281     40.923    0.000  0.228  0.146  0.275   2.8110   2.6270   2.9329  detail RDP
                                                                                                                         
excited state
  msk7    -119.247     23.209    0.000  0.135  0.118  0.145   2.7504   2.5870   2.8593  detail RDP [NC]
    s3    -115.537     23.762  180.000 -0.140 -0.104 -0.161   2.7335   2.5723   2.8410  detail RDP
   sg2    -126.011     24.003  180.000 -0.143 -0.106 -0.164   2.7202   2.5607   2.8265  detail RDP
  skm*    -117.599     23.083  180.000 -0.132 -0.093 -0.154   2.7786   2.6057   2.8934  detail RDP
 sksc4    -117.306     21.653    0.000  0.127  0.110  0.136   2.7435   2.5778   2.8538  detail RDP [NC]
  sly4    -115.877     24.694  180.000 -0.140 -0.101 -0.162   2.7892   2.6163   2.9041  detail RDP

explanations

  1. "energy" is the binding energy of the nucleus compared with separated protons and neutrons.
  2. Qz=2z^2-x^2-y^2, i.e., the mass quadrupole moment, where z-axix is the symmetry axis.
  3. "gamma" is axial asymmetry parameter of the mass distribution. (in degree. +/-180deg and 0deg is the same)
  4. Click "detail" for the output of the program
    These output contains a character string "T=50keV" (meaning temperature is 50keV) which is not true. The temperature is exactly zero for all the calculations.
  5. Click "RDP" for the angle-averaged radial density profile data. Data columns are :
    1. radius(fm)
    2. nucleon density(1/fm^3)
    3. neutron density(1/fm^3)
    4. proton density(1/fm^3)
    5. the number of mesh points to calculate the values in columns (1)-(4) as arithmetic averages
    Use a specialized interporation program to make an equidistant spacing radial density profile data using nonuniform mesh data obtainable by clicking "RDP"
  6. [NC] means that the solution has not been converged yet but is oscillating in configuration. (A finite temperature will stop the oscillation and make the solution converged.)

References to cite when using these data

When one includes the data downloadable from this web page, one should cite the following four references. The method of calculation is described in detail in Ref.1 and Ref.2. Odd-N and/or odd-Z nuclei are treated in the manner described in Ref.3 The original version of the computer program (ev8) is described in Ref.4.
  1. N. Tajima, S. Takahara, and N. Onishi, Nuclear Physics, A603, 23 (1996).
  2. N. Tajima, Progress of Theoretical Physics, Supplement, 142, 265 (2001).
  3. H. Kitagawa, N. Tajima, and H. Sagawa, Zeitschrift fuer Physik, A358, 381 (1997).
  4. P. Bonche, H. Flocard, P.-H. Heenen, S.J. Krieger, and M.S. Weiss, Nuclear Physics, A443, 39 (1985).

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