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NAME

module av18pot

PURPOSE

Argonne v18 and vn' and Super-Soft Core (C) potential package

NOTES

prepared 1 Sep 1994 by R. B. Wiringa, Physics Division, Argonne National Laboratory, Argonne, IL 60439 e-mail: wiringa@theory.phy.anl.gov

reference: 

  "Accurate nucleon-nucleon potential with charge-independence breaking"
   R. B. Wiringa, V. G. J. Stoks, and R. Schiavilla, 
   Physical Review C51, 38 (1995) - WSS95.

option for v8' reprojection of v18 potential added 10 Jan 2001

reference: 

  "Quantum Monte Carlo calculations of nuclei with A<=7"
   B. S. Pudliner, V. R. Pandharipande, J. Carlson, Steven C. Pieper,
   and R. B. Wiringa, Physical Review C56, 1720 (1997) - PPCPW97

option for v6', v4', vx', v2', v1' potentials added 16 Jul 2002

reference: 

  "Evolution of Nuclear Spectra with Nuclear Forces"
   R. B. Wiringa and Steven C. Pieper,
   Physical Review Letters 89, 182501 (2002) - WP02

option for Super-Soft Core (C) added 14 Feb 2007

reference: 

  "Construction d'un potentiel nucleon-nucleon a coeur tres mou (SSC)"
   R. de Tourreil and D. W. L. Sprung,
   Nuclear Physics A201, 193 (1973) - TS73

option for modfied Argonne v8' and modified SSC! v8' added 14 Feb 2007 

   modifications selected by Steve Pieper
   correction to modified SSC! v8' on 4 Apr 2007

this file contains 4 subroutines: 

   subroutine av18pw(lpot,l,s,j,t,t1z,t2z,r,vpw)
   subroutine av18op(lpot,r,vnn)
   subroutine empot(lpot,r,vem)
   subroutine consts(lpot,hc,mpi0,mpic,mp,mn,alpha,mup,mun)

the variable lpot selects between v18, v8' and other options

av18pw gives the full potential in a particular partial wave av18op gives the strong interaction part in operator format empot gives the electromagneti! part in operator format consts gives values of fundamental constants and masses used

notes:

  • av18pw includes full EM interaction for lpot=1; for lpot>1 it includes only C1(pp), i.e., Coulomb with a form factor for pp channels.
  • empot does not include the energy-dependence of the Coulomb interaction used in eq.(4) of WSS95, i.e., it uses alpha, not alpha'.
  • the vacuum polarization in empot is a short-range approximation to eq.(7) suitable for bound states, but not for scattering. it is taken from eq.(3.13) of Rev. Mod. Phys. 44, 48 (1972). 8/28/97 error in this formula detected and corrected: should be -(gamma+5/6) instead of printed (-gamma+5/6)
  • these subroutines should be compiled with a compiler option that forces all floating point constants to be evaluated at real(8) significance, e.g., on an IBM RS6000 the xlf compiler option qdpc=e should be used; on SGI machines, the -r8 option should be used; on a Cray no action is needed. if such an option is not available and the default precision is real*4 (32 bits), then all constants should be explicitly converted to double precision by appending a D0.
  • consts now (14 Feb 2007) depend upon potential: need to call to generate appropriate hbar**2/M