Configurations

Keyword: PHNONE_NEU
1, 00, 00 = NUPAHO,KPNONE,KHNONE

Neutron particle-hole excitations pertaining to the situation when all neutrons are in one common block (no simplex, signature, or parity is conserved). NUPAHO is the consecutive number from 1 to 5 (up to five sets of excitations can be specified in separate items). Particles are removed from the KHNONE-th state and put in the KPNONE-th state. At every stage of constructing excitations the Pauli exclusion principle has to be respected (particle removed from an occupied state and put in an empty state). Values equal zero have no effect. Note that for all neutrons sitting in one common block the reference configuration from which the particle-hole excitations are counted is defined by the total number of neutrons.

Keyword: PHNONE_PRO
1, 00, 00 = NUPAHO,KPNONE,KHNONE

Same as above but for the proton particle-hole excitations.

Keyword: VACPAR_NEU
44, 42 = KVASIQ(0),KVASIQ(1)

Numbers of lowest neutron states occupied in the two blocks, denoted by ($+1$) and ($-1$), of given parities, $\pi$=+$1$ and $\pi$=$-$$1$, respectively. These numbers define the parity reference configuration from which the particle-hole excitations are counted. The definitions of parity reference configuration and excitations are ignored unless IPARTY=1, or IPARTY=$-$1 and ISIMPY=ISIGNY=1. They are also ignored for IPAIRI=0.

Keyword: VACPAR_PRO
32, 34 = KVASIQ(0),KVASIQ(1)

Same as above but for the numbers of proton states.

Keyword: PHPARI_NEU
1, 00, 00, 00, 00 = NUPAHO,KPSIQP,KPSIQM,KHSIQP,KHSIQM

Neutron particle-hole excitations in the parity blocks. NUPAHO is the consecutive number from 1 to 5 (up to five sets of excitations can be specified in separate items). Particles are removed from the KHSIQP-th state in the ($+1$) block and from the KHSIQM-th state in the ($-1$) block, and put in the KPSIQP-th state in the ($+1$) block and in the KPSIQM-th state in the ($-1$) block. At every stage of constructing excitations the Pauli exclusion principle has to be respected (particle removed from an occupied state and put in an empty state). Values equal zero have no effect.

Keyword: PHPARI_PRO
1, 00, 00, 00, 00 = NUPAHO,KPSIQP,KPSIQM,KHSIQP,KHSIQM

Same as above but for the proton particle-hole excitations.

	Keyword: DIAPAR_NEU
			2, 2,   1, 1,   0, 0 =	KPFLIQ(0,0),KPFLIQ(1,0),
				KHFLIQ(0,0),KHFLIQ(1,0),
				KOFLIQ(0,0),KOFLIQ(1,0)

Diabatic blocking of neutron single-particle parity configurations. Matrices KPFLIQ contain the indices of the particle states in the two parity blocks denoted by ($+1$) and ($-1$), of given parities, i.e., $\pi$=+$1$ and $-1$, respectively. Matrices KHFLIQ contain analogous indices of the hole states, and matrices KOFLIQ define type of blocking according to the following table:

KOFLIQ=0	$$	No diabatic blocking in the given parity block.
KOFLIQ=$+$1	$$	The state which has the		larger		$y$-alignment is occupied.
KOFLIQ=$-$1	$$	The state which has the		smaller		$y$-alignment is occupied.
KOFLIQ=$+$2	$$	The state which has the		larger		$y$-intrinsic spin is occupied.
KOFLIQ=$-$2	$$	The state which has the		smaller		$y$-intrinsic spin is occupied.
KOFLIQ=$+$3	$$	The state which has the		larger		$x$-alignment is occupied.
KOFLIQ=$-$3	$$	The state which has the		smaller		$x$-alignment is occupied.
KOFLIQ=$+$4	$$	The state which has the		larger		$x$-intrinsic spin is occupied.
KOFLIQ=$-$4	$$	The state which has the		smaller		$x$-intrinsic spin is occupied.
KOFLIQ=$+$5	$$	The state which has the		larger		$z$-alignment is occupied.
KOFLIQ=$-$5	$$	The state which has the		smaller		$z$-alignment is occupied.
KOFLIQ=$+$6	$$	The state which has the		larger		$z$-intrinsic spin is occupied.
KOFLIQ=$-$6	$$	The state which has the		smaller		$z$-intrinsic spin is occupied.
KOFLIQ=$+$7	$$	The state which has the		larger		$o$-alignment is occupied.
KOFLIQ=$-$7	$$	The state which has the		smaller		$o$-alignment is occupied.
KOFLIQ=$+$8	$$	The state which has the		larger		$o$-intrinsic spin is occupied.
KOFLIQ=$-$8	$$	The state which has the		smaller		$o$-intrinsic spin is occupied.
KOFLIQ=$+$9	$$	The state which has the		larger		multipole moment $Q_{20}$ is occupied.
KOFLIQ=$-$9	$$	The state which has the		smaller		multipole moment $Q_{20}$ is occupied.
KOFLIQ=$+$10	$$	The state which has the		larger		multipole moment $Q_{22}$ is occupied.
KOFLIQ=$-$10	$$	The state which has the		smaller		multipole moment $Q_{22}$ is occupied.

Here, the $x$-, $y$-, and $z$-alignments or intrinsic spins denote projections of the total angular momentum or spin, respectively, on the $x$, $y$, and $z$ axes. Similarly, the $o$-alignment or $o$-intrinsic spin denotes analogous projections on the direction of the angular velocity $\mbox{{\boldmath {$\omega$}}}_J$. In version (v2.07f), observables KOFLIQ= $\pm3,\ldots,\pm10$ have been added to the above list. Identical extension of the list was also implemented for the diabatic blocking in the simplex or parity/signature configurations, see Sec. III-3.2.

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, or average quadrupole moments) 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: DIAPAR_PRO
			2, 2,   1, 1,   0, 0 =	KPFLIQ(0,1),KPFLIQ(1,1),
				KHFLIQ(0,1),KHFLIQ(1,1),
				KOFLIQ(0,1),KOFLIQ(1,1)

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

Keyword: DIANON_NEU
2, 1, 0 = KPFLIZ,KHFLIZ,KOFLIZ

Same as above but for the diabatic blocking of neutron single-particle configurations in the situation when all neutrons are in one common block.

Keyword: DIANON_PRO
2, 1, 0 = KPFLIZ,KHFLIZ,KOFLIZ

Same as above but for the diabatic blocking of proton single-particle configurations in the situation when all protons are in one common block.