{jobnam} the jobname under which the S matrices have been stored {jobname}n.smt. Here n denotes the value of the parameter ienerg (see below). These S matrices must have been previously generated using
JTOT1 = 1 (ensuring the determination of S-matrices at every partial wave)
WRSMAT = .true. (ensuring that the S-matrices are written to file {jobname}.smt).
The default value of {jobname} is the value you have set with the command JOB, or, if no value has been set, {jobname}=JOB
j1,in1 rotational quantum number and additional index for the initial state
j2,in2 rotational quantum number and additional index for the final state
ang1,ang2 initial and final angle (in degrees)
dang step size (in degrees) for scan through angles.
ienerg the cardinal value of the energy for which the differential cross section is computed. i.e. if ienerg = 2, then the second energy S matrices [{jobname}2.smt] are used
jtotend the maximum value of Jtot included in determining the scattering amplitude. N. B. This can not be larger than the variable JTOT2 used in the initial calculation
ipr
if ipr .ne. 0, the differential cross sections and the alignment (A0(2)) and hexapole moments (A0(4)) of the products are also printed to the normal output file and to stdout.
If mflag .ne. 0, then all m->m' differential cross sections are calculated and printed. Quantization is in the collision frame, where the initial relative velocity vector defines the z axis. ALSO, if mflag .ne.0 , the integral m-> m' cross sections are determined, by integration from ang1 to ang2 in steps of dang.
alpha, beta parameters which define the mixture of e and f lamda-doublet states in the "heads" or "tails" orientation.
| heads > = alpha | jme > - beta | jmf >