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Input Variables
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Atomic Orbitals
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Calculation Modes
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Geometry Optimization
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Invert KS
--
Optimal Control
--- OCTCheckGradient
--- OCTClassicalTarget
--- OCTControlFunctionOmegaMax
--- OCTControlFunctionRepresentation
--- OCTControlFunctionType
--- OCTCurrentFunctional
--- OCTCurrentWeight
--- OCTDelta
--- OCTDirectStep
--- OCTDoubleCheck
--- OCTDumpIntermediate
--- OCTEps
--- OCTEta
--- OCTExcludedStates
--- OCTFilter
--- OCTFixFluenceTo
--- OCTFixInitialFluence
--- OCTHarmonicWeight
--- OCTInitialState
--- OCTInitialTransformStates
--- OCTInitialUserdefined
--- OCTLaserEnvelope
--- OCTLocalTarget
--- OCTMaxIter
--- OCTMomentumDerivatives
--- OCTNumberCheckPoints
--- OCTOptimizeHarmonicSpectrum
--- OCTPenalty
--- OCTPositionDerivatives
--- OCTRandomInitialGuess
--- OCTScheme
--- OCTSpatialCurrWeight
--- OCTStartIterCurrTg
--- OCTTargetDensity
--- OCTTargetDensityFromState
--- OCTTargetOperator
--- OCTTargetSpin
--- OCTTargetTransformStates
--- OCTTargetUserdefined
--- OCTTdTarget
--- OCTVelocityDerivatives
--- OCTVelocityTarget
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OCTCurrentWeight
OCTCurrentWeight
Section Calculation Modes::Optimal Control
Type float
Default 0.0
In the case of simultaneous optimization of density $n$ and current $j$, one can tune the importance
of the current functional $J1_c[j]$, as the respective functionals might not provide results on the
same scale of magnitude. $J1[n,j]= J1_d[n]+ {\tt OCTCurrentWeight}\ J1_c[j]$. Be aware that its
sign is crucial for the chosen OCTCurrentFunctional as explained there.