Metastable electronic states can be characterized by a complex Siegert energy,
(4.68) |
where the width, , is proportional to the inverse lifetime of the state: . Complex coordinate methods aim to compute this complex energy as an eigenvalue of an effective non-Hermitian Hamiltonian. One such method is the method of complex basis functions (CBFs) where a basis of Gaussians with complex exponents is used in conjunction with a symmetric (not complex-conjugated) inner product to effictively produce a finite-basis representation of a non-Hermitian operators.
812
Phys. Rev. A
(1978),
41,
pp. 1364.
Link
,
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J. Chem. Phys.
(2015),
142,
pp. 054103.
Link
,
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J. Chem. Phys.
(2015),
143,
pp. 074103.
Link
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1271
J. Chem. Phys.
(2017),
146,
pp. 234107.
Link
In cases, such as temporary anions, where the decay channel is of 1-electron character, a mean-field theory can provide approximate Siegert energies for a many-electron system.
The simplest such approximation is the static-exchange approximation. In this approximation the Siegert energies of an ()-electron state are computed by diagonalizing a Fock operator computed from the density of an -electron state.
1272
J. Chem. Phys.
(2015),
142,
pp. 054103.
Link
This approximation neglects orbital relaxation effects which can be included by a non-Hermitian self-consistent-field (NH-SCF) procedure.
812
Phys. Rev. A
(1978),
41,
pp. 1364.
Link
,
1273
J. Chem. Phys.
(2015),
143,
pp. 074103.
Link
In practice the NH-SCF energy functional is the same as the Holomorphic Hartree-Fock energy functional (Eq. 4.64), though it is used for a different purpose. Both static-exchange and NH-SCF theories using complex basis functions (CBFs) are available in Q-Chem. Specification of the complex basis set is described in Section 8.7.
COMPLEX_EXPONENTS
COMPLEX_EXPONENTS
Enable a non-Hermitian calculation with CBFs.
TYPE:
LOGICAL
DEFAULT:
FALSE
OPTIONS:
TRUE
Perform a non-Hermitian calculation with CBFs
RECOMMENDATION:
Set to TRUE if a non-Hermitian calculation using CBFs is desired.
COMPLEX_SPIN_STATE
COMPLEX_SPIN_STATE
Spin state for non-Hermitian calculation
TYPE:
INTEGER
DEFAULT:
1
Singlet
OPTIONS:
A state of spin
RECOMMENDATION:
None
COMPLEX_N_ELECTRON
COMPLEX_N_ELECTRON
Add electrons for non-Hermitian calculation.
TYPE:
INTEGER
DEFAULT:
0
Perform the non-Hermitian calculation on -electrons
OPTIONS:
Perform the non-Hermitian calculation on an electron system
RECOMMENDATION:
None
COMPLEX_STATIC_EXCHANGE
COMPLEX_STATIC_EXCHANGE
Perform a CBF static-exchange calculation.
TYPE:
LOGICAL
DEFAULT:
FALSE
OPTIONS:
TRUE
Perform a static exchange calculation
FALSE
Do not perform a static exchange calculation
RECOMMENDATION:
Set to TRUE if a static-exchange calculation is desired.
COMPLEX_SCF
COMPLEX_SCF
Perform a non-Hermitian SCF calculation with CBFs
TYPE:
INTEGER
DEFAULT:
0
OPTIONS:
0
Do not perform an NH-SCF calculation
1
Perform a restricted NH-SCF calculation
2
Perform an unrestricted NH-SCF calculation
3
Perform a restricted, open-shell NH-SCF calculation
RECOMMENDATION:
None
COMPLEX_METSCF
COMPLEX_METSCF
Specify the NH-SCF solver
TYPE:
INTEGER
DEFAULT:
1
OPTIONS:
0
Roothaan iterations
1
DIIS
3
ADIIS
21
Newton-MINRES
RECOMMENDATION:
Use the default (DIIS).
COMPLEX_SCF_GUESS
COMPLEX_SCF_GUESS
Specify the NH-SCF guess
TYPE:
INTEGER
DEFAULT:
0
OPTIONS:
0
Use a guess from a static-exchange calculation
1
Read real-basis MO coefficients
2
Read real-basis density matrix
1000
Read guess from a previous calculation
RECOMMENDATION:
Use a guess from a static exchange calculation. Note that for temporary anions, this requires the specification of COMPLEX_TARGET.
COMPLEX_TARGET
COMPLEX_TARGET
Specify the orbital index to be occupied for a temporary anion
TYPE:
INTEGER
DEFAULT:
0
OPTIONS:
Orbital index (starting at zero) for the additional electron
RECOMMENDATION:
should always be greater than .