BSE_ITERAT

Parameters influencing the iterative Bethe-Salpeter calculation. The iterative solver has not been fully implemented yet. [Edit on GitHub]

Keywords

Keyword descriptions

DAVIDSON_ABORT_COND

Type: enum
Default: EN
Usage: DAVIDSON_ABORT_COND OR

Description: Desired abortion condition for Davidson solver

Valid values:

  • EN Uses energy threshold for successfully exiting solver.

  • RES Uses residual threshold for successfully exiting solver.

  • OR Uses either energy or residual threshold for successfully exiting solver.

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EPS_EXC_EN

Type: real
Default: 2.72113839E-002 [eV]
Usage: EPS_EXC_EN 0.001

Description: Threshold for stopping the iteration for computing the transition energies. If the desired excitation energies change by less than EPS_EXC_EN (in eV), the iteration stops.

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EPS_RES

Type: real
Default: 2.72113839E-002 [eV]
Usage: EPS_RES 0.001

Description: Threshold for stopping the iteration for computing the transition energies. If the residuals inside the Davidson space change by less than EPS_RES (in eV), the iteration stops.

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FAC_MAX_Z_SPACE

Type: integer
Default: 5
Usage: FAC_MAX_Z_SPACE 5

Description: Factor to determine maximum dimension of the Davidson subspace. dimension = (NUM_EXC_EN+NUM_ADD_START_Z_SPACE)*FAC_MAX_Z_SPACE

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NUM_ADD_START_Z_SPACE

Type: integer
Default: 0
Usage: NUM_ADD_START_Z_SPACE 1

Description: Determines the initial dimension of the subspace as dim = (NUM_EXC_EN+NUM_ADD_START_Z_SPACE)

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NUM_DAVIDSON_ITER

Type: integer
Default: 100
Usage: NUM_DAVIDSON_ITER 100

Description: Maximum number of iterations for determining the transition energies.

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NUM_EXC_EN

Type: integer
Default: 3
Usage: NUM_EXC_EN 3

Description: Number of lowest excitation energies to be computed.

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NUM_NEW_T

Type: integer
Default: 1
Usage: NUM_NEW_T 4

Description: Number of new t vectors added. Must be smaller/equals (NUM_EXC_EN+NUM_ADD_START_Z_SPACE)

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Z_SPACE_ENERGY_CUTOFF

Type: real
Default: -2.72113839E+001 [eV]
Usage: Z_SPACE_ENERGY_CUTOFF 60

Description: Cutoff (in eV) for maximal energy difference entering the A matrix. Per default and for negative values, there is no cutoff applied.

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