Configurations

Keyword: DIASIM_NEU
	2, 2,    1, 1,    0, 0 =	KPFLIM(0,0), KPFLIM(1,0),
		KHFLIM(0,0), KHFLIM(1,0),
		KOFLIM(0,0), KOFLIM(1,0)

Diabatic blocking of neutron single-particle simplex configurations. Matrices KPFLIM contain the indices of the particle states in the two simplex blocks denoted by (+) and (-), of given simplex values, i.e., s=+i and -i, respectively. Matrices KHFLIM contain analogous indices of the hole states, and matrices KOFLIM define type of blocking according to the following table:

KOFLIM=0	$$	$\!\!$No diabatic blocking in the given parity/signature block.
KOFLIM=+1	$$	The state which has the		larger		alignment is occupied.
KOFLIM=-1	$$	The state which has the		smaller		alignment is occupied.
KOFLIM=+2	$$	The state which has the		larger		intrinsic spin is occupied.
KOFLIM=-2	$$	The state which has the		smaller		intrinsic spin is occupied.

Within the diabatic blocking procedure one does not predefine whether the particle or the hole state is occupied (like is the case when the particle-hole excitations are defined, see Section 3.4 of II). In each iteration the code calculates the average alignments (or average intrinsic spins) of both states (those defined by KPFLIM and KHFLIM), and occupies that state for which a larger, or a smaller value is obtained. Therefore, the order of both states in the Routhian spectrum is irrelevant.

The user is responsible for choosing the particle-state indices (in KPFLIM) only among those corresponding to empty single-particle states, and the hole-state indices (in KHFLIM) only among those corresponding to occupied single-particle states, see Section 3.4 of II.

Keyword: DIASIM_PRO
	2, 2,    1, 1,    0, 0 =	KPFLIM(0,1), KPFLIM(1,1),
		KHFLIM(0,1), KHFLIM(1,1),
		KOFLIM(0,1), KOFLIM(1,1)

Same as above but for the diabatic blocking of proton single-particle simplex configurations.

Keyword: DIASIG_NEU
	2, 2, 2, 2,    1, 1, 1, 1,    0, 0, 0, 0 =
	KPFLIG(0,0,0), KPFLIG(0,1,0), KPFLIG(1,0,0), KPFLIG(1,1,0),
	KHFLIG(0,0,0), KHFLIG(0,1,0), KHFLIG(1,0,0), KHFLIG(1,1,0),
	KOFLIG(0,0,0), KOFLIG(0,1,0), KOFLIG(1,0,0), KOFLIG(1,1,0)

Diabatic blocking of neutron single-particle parity/signature configurations. Matrices KPFLIG contain the indices of particle states in the four parity/signature blocks denoted by (+,+), (+,-), (-,+), and (-,-), of given (parity,signature) combinations, i.e., $(\pi,r)$=(+1,+i), (+1,-i), (-1,+i), and (-1,-i), respectively. Matrices KHFLIG contain analogous indices of hole states, and matrices KOFLIG define the type of blocking according to the table of values identical to that defined for the simplex case above. Other rules described for the simplex case apply here analogously.

Keyword: DIASIG_PRO
	2, 2, 2, 2,    1, 1, 1, 1,    0, 0, 0, 0 =
	KPFLIG(0,0,1), KPFLIG(0,1,1), KPFLIG(1,0,1), KPFLIG(1,1,1),
	KHFLIG(0,0,1), KHFLIG(0,1,1), KHFLIG(1,0,1), KHFLIG(1,1,1),
	KOFLIG(0,0,1), KOFLIG(0,1,1), KOFLIG(1,0,1), KOFLIG(1,1,1)

Same as above but for the diabatic blocking of proton single-particle parity/signature configurations.