User Tools

Site Tools


codes

Differences

This shows you the differences between two versions of the page.

Link to this comparison view

Both sides previous revision Previous revision
Next revision
Previous revision
codes [2014/08/08 15:07]
bogner
codes [2014/08/08 15:15]
bogner
Line 1: Line 1:
 ====== Codes and Useful Links ====== ====== Codes and Useful Links ======
 ==== Some useful black boxes ==== ==== Some useful black boxes ====
-  * One of the files (renorm-modules.f90) in the TBME package had a subtle but important bug where matrix elements in the spin-triplet channel, which should vanish due to the structure of the Minnesota potential, were non-zero. Here is a fixed version of the file in question {{:​renorm-modules.f90.gz|}}.+
    
   * {{:​relcom2labsystem.tar.gz|}} A f90 package that generates both m-scheme and J-coupled TBMEs in the oscillator basis. We will discuss how to use this before the afternoon session on Thursday. ​   * {{:​relcom2labsystem.tar.gz|}} A f90 package that generates both m-scheme and J-coupled TBMEs in the oscillator basis. We will discuss how to use this before the afternoon session on Thursday. ​
  
   * {{:​coulomboscrelmeV1.f90.zip|}} Some f90 subroutines (NOT a standalone code) from a larger code that calculates relative two-body matrix element $\langle nl|V|n'​l\rangle$ of the Coulomb potential in the HO basis. The main purpose of this code is to illustrate the algorithm to calculate generalized Laguerre polynomials $L^{l+1/​2}_n$ that enter the definition of the HO wf's $R_{nl}$. {{makefile.gz|Here}} is the Makefile that was missing. ​   * {{:​coulomboscrelmeV1.f90.zip|}} Some f90 subroutines (NOT a standalone code) from a larger code that calculates relative two-body matrix element $\langle nl|V|n'​l\rangle$ of the Coulomb potential in the HO basis. The main purpose of this code is to illustrate the algorithm to calculate generalized Laguerre polynomials $L^{l+1/​2}_n$ that enter the definition of the HO wf's $R_{nl}$. {{makefile.gz|Here}} is the Makefile that was missing. ​
 +
 +UPDATE: One of the files (renorm-modules.f90) in the TBME package had a subtle but important bug where matrix elements in the spin-triplet channel, which should vanish due to the structure of the Minnesota potential, were non-zero. Here is a fixed version of the file in question {{:​renorm-modules.f90.gz|}}.
  
   * {{:​eigen_basis.zip|}} C++ code adapted from Dick Furnstahl'​s Computational Physics course at Ohio State to calculate the Coulomb hamiltonian on a HO basis for $l=0$. This calculates the HO wf's a bit differently than Fortran code above.   * {{:​eigen_basis.zip|}} C++ code adapted from Dick Furnstahl'​s Computational Physics course at Ohio State to calculate the Coulomb hamiltonian on a HO basis for $l=0$. This calculates the HO wf's a bit differently than Fortran code above.
codes.txt ยท Last modified: 2014/08/08 15:15 by bogner