Constraints

Keyword: OMISOY
0.00 = OMISOY

Isovector angular frequency $\omega_{J1y}$ in the $y$ direction, see Sec. 2.3 and Eq. (1). A non-zero value of OMISOY requires IROTAT=1 and cannot be used for the BCS pairing, i.e., for IPAIRI=1 and IPAHFB=0.

Keyword: OMEGA_XYZ
0.00, 0.00, 0.00, 0 = OMEGAX,OMEGAY,OMEGAZ,ITILAX

For ITILAX=1, values of the three Cartesian components of the isoscalar angular frequency vector $\mbox{{\boldmath {$\omega$}}}_{J0}$, see Sec. 2.3 and Eq. (1). For ITILAX=0 these values are ignored. ITILAX=1 requires IROTAT=1, ISIMPY=0, and IPAIRI=0. A non-zero value of OMEGAX, OMEGAY, or OMEGAZ requires broken symmetry ISIMTX=0, ISIMTY=0, or ISIMTZ=0, respectively.

Keyword: OMEGA_RTP
0.00, 0.00, 0.00, 0 = OMERAD,OMETHE,OMEPHI,ITILAX

Same as above but for values of the standard spherical components of the isoscalar angular frequency, i.e., $\omega_{J0r}$, $\omega_{J0\theta}$, and $\omega_{J0\phi}$.

Keyword: OMISO_XYZ
0.00, 0.00, 0.00, 0 = OMISOX,OMISOY,OMISOZ,ITISAX

For ITISAX=1, values of the three Cartesian components of the isovector angular frequency vector $\mbox{{\boldmath {$\omega$}}}_{J1}$, see Sec. 2.3 and Eq. (1). For ITISAX=0 these values are ignored. ITISAX=1 requires IROTAT=1, ISIMPY=0, and IPAIRI=0. A non-zero value of OMISOX, OMISOY, or OMISOZ requires broken symmetry ISIMTX=0, ISIMTY=0, or ISIMTZ=0, respectively.

Keyword: OMEGA_TURN
0 = IMOVAX

For IMOVAX=1 or $-$1, the isoscalar angular frequency vector $\mbox{{\boldmath {$\omega$}}}_{J0}$, see Sec. 2.3, is in each iteration set in the direction of the total angular momentum $\mbox{{\boldmath {$J$}}}_{0}$, or opposite to this direction, respectively, while its length is kept equal to that fixed by the sum of squares of OMEGAX, OMEGAY, and OMEGAZ. For IMOVAX=0, vector $\mbox{{\boldmath {$\omega$}}}_{J0}$ is not changed during the iteration. IMOVAX=1 or $-$1 requires ITILAX=1, ITISAX=0, and IFLAGA=0.

Keyword: SURFCONSTR
2, 0, 0.0, 0.0, 0 = LAMBDA, MIU, STIFFS, SASKED, IFLAGS

For IFLAGS=1, the surface mass multipole moment of the given multipolarity $\lambda$ and $\mu$ is constrained. Values of LAMBDA, MIU, STIFFS, and SASKED correspond respectively to $\lambda$, $\mu$, $C^S_{\lambda\mu}$, and $\bar{Q}^S_{\lambda\mu}$ in Eq. (4). For IFLAGS=0, there is no constraint in the given multipolarity.

	Keyword: SPICON_XYZ
			0.0, 0.0, 0 =	STIFFI(1),ASKEDI(1),IFLAGI(1)
			0.0, 0.0, 0 =	STIFFI(2),ASKEDI(2),IFLAGI(2)
			0.0, 0.0, 0 =	STIFFI(3),ASKEDI(3),IFLAGI(3)

For IFLAGI=1, the quadratic constraint on one of the Cartesian components of angular momentum is used together with the linear constraint, see Sec. 2.3 and Eq. (1). Values of STIFFI and ASKEDI correspond respectively to $C_{Ja}$ and $\bar{J}_{J0a}$ in Eq. (1), where $a$=$x$, $y$, or $z$. For IFLAGI=0, there is no quadratic constraint on a given component. IFLAGI(1)=1, IFLAGI(2)=1, or IFLAGI(3)=1 requires broken symmetry ISIMTX=0, ISIMTY=0, or ISIMTZ=0, respectively.

Keyword: SPICON_OME
0.0, 0.0, 0 = STIFFA,ASKEDA,IFLAGA

For IFLAGA=1, the quadratic constraint on the angle between the angular frequency and angular momentum vectors, see Sec. 2.3 and Eq. (1). In version (v2.07f) the angle is constrained to zero. Value of STIFFA corresponds to $C_{A}$ in Eq. (1). Value of ASKEDA must be set to 0; this variable is reserved for a future implementation of the constraint to a non-zero angle. For IFLAGA=0, there is no quadratic constraint on the angle. IFLAGA=1 requires ISIMPY=0, IROTAT=1, ITILAX=1, ITISAX=0, IFLAGI(1)=0, IFLAGI(2)=0, IFLAGI(3)=0, ISIMTX=0, ISIMTY=0, ISIMTZ=0, and a non-zero value of sum of squares of OMEGAX, OMEGAY, and OMEGAZ.