# Optical Properties: Time-Dependent Current DFT¶

Time-Dependent Current Density Functional Theory (TD-CDFT) is a theoretical framework for computing optical response properties, such as the frequency-dependent dielectric function.

In this section, the TD-CDFT implementation for extended systems (1D, 2D and 3D) in BAND is described. The input keys are described in NewResponse or in OldResponse.

Some examples are available in the \$AMSHOME/examples/band directory and are discussed in the Examples section.

## Insulators, semiconductors and metals¶

The TD-CDFT module enables the calculation of real and imaginary parts of the material property tensor $$\chi_e(\omega)$$, called the electric susceptibility. The electric susceptibility is related to the macroscopic dielectric function, $$\varepsilon_M(\omega)$$.

For semi-conductors and insulator, for which the bands are either fully occupied or fully unoccupied, the dielectric function $$\varepsilon_M(\omega)$$ comprises only of the so called interband component:

$\varepsilon_M(\omega) = 1 + 4 \pi \chi_e(\omega)$

In general $$\chi_e(\omega)$$ and $$\varepsilon_M(\omega)$$ are tensors. They, however, simplify to scalars in isotropic systems.

For metals, for which partially-occupied bands exist, there is a so called intraband component arising due to transitions within a partially-occupied band:

$\varepsilon_M(\omega) = 1 + 4 \pi \chi_e(\omega) - 4 \pi i \sigma_e(\omega) / \omega$

## Frequency dependent kernel¶

It is known that the exact Vignale-Kohn (VK) kernel greatly improves the static polarizabilities of infinite polymers and nanotubes (see reference), but gives bad results for the optical spectra of semiconductors and metals. For the low frequency part one needs a frequency dependent kernel, since Drude-like tails are completely absent in the adiabatic local density approximation (ALDA). With a modified VK kernel, which neglects $$\mu_{xc}$$ so that it reduces to the ALDA form in the static limit (see reference), much better results can be obtained. BAND currently only supports the modified VK kernel in either the QV or CNT parametrization, and it should only be used for metals.

## EELS¶

From the macroscopic dielectric function it is possible to calculate the electron energy loss function (EELS). In transmission EELS one studies the inelastic scattering of a beam of high energy electrons by a target. The scattering rates obtained in these experiments are related to the dynamical structure factor $$S(q,\omega)$$ [A1]. In the special case with wavevector $$q=0$$, $$S(q,\omega)$$ is related to the longitudinal macroscopic dielectric function. This is the long-wave limit of EELS. For isotropic system the dielectric function is simply a scalar ($$1/3 \text{Tr} (\varepsilon_M(\omega))$$ ). In this case the long-wave limit of the electron energy loss function assumes the trivial form

$\lim_{q \rightarrow 0} 2 \pi \frac{S(q,\omega)}{q^2 V} = \frac{\varepsilon_2}{\varepsilon_1^2 + \varepsilon_2^2}$

with $$\varepsilon_1$$ and $$\varepsilon_2$$ as real and imaginary part of the dielectric function.

References

The three related Ph.D. theses, due to F. Kootstra (on TD-DFT for insulators), P. Romaniello (on TD-CDFT for metals), and A. Berger (on the Vignale-Kohn functional in extended systems) contain much background information, and can be downloaded from the SCM website.

The most relevant publications on this topic due to the former “Groningen” group of P.L. de Boeij are    .

[A1] S. E. Schnatterly, in Solid State Physics Vol.34, edited by H. Ehrenreich, F. Seitz, and D. Turnbull (Academic Press, Inc., New York, 1979).

## Input Options¶

In the 2017 release of BAND there are two implementations of the TD-CDFT formalism. The original implementation, relying on obsolete algorithms of BAND, is accessible via the OldResponse key block. The new code section, relying on more modern algorithms of BAND, is accessible via the NewResponse, NewResponseSCF and NewResponseKSpace key blocks. The differences between the two flavors are summarized in the following table:

 OldResponse NewResponse 3D-systems yes yes 2D-systems no yes 1D-systems (yes) yes Semiconductors yes yes Metals yes (yes) ALDA yes yes Vignale-Kohn yes no Berger2015 (3D) yes yes Scalar ZORA yes yes Spin Orbit ZORA yes no

Besides these differences, one should not expect both flavors to give the exact same result, if the reciprocal space limit is not reached! This can be explained by different approaches to evaluate the integration weights of single-particle transitions in reciprocal space.

Attention

Response properties converge slowly with respect to k-space sampling (number of k-points). Always check the convergence of $$\varepsilon_M$$ with respect to K-Space options!!! Fig. 3 Reciprocal space sampling convergence of imaginary part of susceptibility for a dihydrogen chain.

### NewResponse¶

The dielectric function is computed when the key block NewResponse is present in the input. Several important settings can be defined in this key block.

Additional details can be specified via the NewResponseKSpace and NewResponseSCF blocks.

NewResponse
NFreq integer
FreqLow float
FreqHigh float
EShift float
ActiveESpace float
DensityCutOff float
ActiveXYZ string
End

NewResponse
Type: Block The TD-CDFT calculation to obtain the dielectric function is computed when this block is present in the input. Several important settings can be defined here.
NFreq
Type: Integer 5 Number of frequencies for which a linear response TD-CDFT calculation is performed.
FreqLow
Type: Float 1.0 eV Lower limit of the frequency range for which response properties are calculated. (omega_{low})
FreqHigh
Type: Float 3.0 eV Upper limit of the frequency range for which response properties are calculated (omega_{high}).
EShift
Type: Float 0.0 eV Shift Energy shift of the virtual crystal orbitals.
ActiveESpace
Type: Float 5.0 eV Active energy space Modifies the energy threshold (DeltaE^{max}_{thresh} = omega_{high} + ActiveESpace) for which single orbital transitions (DeltaEpsilon_{ia} = Epsilon_{a}^{virtual} - Epsilon_{i}^{occupied}) are taken into account.
DensityCutOff
Type: Float 0.001 Volume cutoff For 1D and 2D systems the unit cell volume is undefined. Here, the volume is calculated as the volume bordered by the isosurface for the value DensityCutoff of the total density.
ActiveXYZ
Type: String t Expects a string consisting of three letters of either ‘T’ (for true) or ‘F’ (for false) where the first is for the X-, the second for the Y- and the third for the Z-component of the response properties. If true, then the response properties for this component will be evaluated.
NewResponseSCF
Bootstrap integer
COApproach Yes/No
COApproachBoost Yes/No
Criterion float
DIIS Yes/No
LowFreqAlgo Yes/No
Mixing float
NCycle integer
XC integer
End

NewResponseSCF
Type: Block Details for the linear-response self-consistent optimization cycle. Only influencing the NewResponse code.
Bootstrap
Type: Integer 0 defines if the Berger2015 kernel (Bootstrap 1) is used or not (Bootstrap 0). If you chose the Berger2015 kernel, you have to set NewResponseSCF%XC to ‘0’. Since it shall be used in combination with the bare Coulomb response only. Note: The evaluation of response properties using the Berger2015 is recommend for 3D systems only!
COApproach
Type: Bool Yes The program automatically decides to calculate the integrals and induced densities via the Bloch expanded atomic orbitals (AO approach) or via the cyrstal orbitals (CO approach). The option COApproach overrules this decision.
COApproachBoost
Type: Bool No CO Approach Boost Keeps the grid data of the Crystal Orbitals in memory. Requires significantly more memory for a speedup of the calculation. One might have to use multiple computing nodes to not run into memory problems.
Criterion
Type: Float 0.001 For the SCF convergence the RMS of the induced density change is tested. If this value is below the Criterion the SCF is finished. Furthermore, one can find the calculated electric susceptibility for each SCF step in the output and can therefore decide if the default value is too loose or too strict.
DIIS
Type: Bool Yes In case the DIIS method is not working, one can switch to plain mixing by setting DIIS to false.
LowFreqAlgo
Type: Bool Yes Low Frequency Algorithm Numerically more stable results for frequencies lower than 1.0 eV. Note: for a graphene monolayer the conical intersection results in a very small band gap (zero band gap semi-conductor). This leads ta a failing low frequency algorithm. One can then chose to use the algoritm as originally proposed by Kootstra by setting the input value to *false*. But, this can result in unreliable results for frequencies lower than 1.0 eV!
Mixing
Type: Float 0.2 Mixing value for the SCF optimization.
NCycle
Type: Integer 20 Cycles Number of SCF cycles for each frequency to be evaluated.
XC
Type: Integer 1 Influences if the bare induced Coulomb response (XC 0) is used for the effective, induced potential or the induced potential derived from the ALDA kernel as well (XC 1).
NewResponseKSpace
Eta float
SubSimp integer
End

NewResponseKSpace
Type: Block Modify the details for the integration weights evaluation in reciprocal space for each single-particle transition. Only influencing the NewResponse code.
Eta
Type: Float 1e-05 Defines the small, finite imaginary number i*eta which is necessary in the context of integration weights for single-particle transitions in reciprocal space.
SubSimp
Type: Integer 3 determines into how many sub-integrals each integration around a k point is split. This is only true for so-called quadratic integration grids. The larger the number the better the convergence behavior for the sampling in reciprocal space. Note: the computing time for the weights is linear for 1D, quadratic for 2D and cubic for 3D!

### OldResponse¶

OldResponse
Berger2015 Yes/No
CNT Yes/No
CNVI float
CNVJ float
Ebndtl float
Enabled Yes/No
Endfr float
Isz integer
Iyxc integer
NewVK Yes/No
Nfreq integer
QV Yes/No
Shift float
Static Yes/No
Strtfr float
End

OldResponse
Type: Block Options for the old TD-CDFT implementation.
Berger2015
Type: Bool No Use the parameter-free polarization functional by A. Berger (Phys. Rev. Lett. 115, 137402). This is possible for 3D insulators and metals. Note: The evaluation of response properties using the Berger2015 is recommend for 3D systems only!
CNT
Type: Bool Use the CNT parametrization for the longitudinal and transverse kernels of the XC kernel of the homogeneous electron gas. Use this in conjunction with the NewVK option.
CNVI
Type: Float 0.001 The first convergence criterion for the change in the fit coefficients for the fit functions, when fitting the density.
CNVJ
Type: Float 0.001 the second convergence criterion for the change in the fit coefficients for the fit functions, when fitting the density.
Ebndtl
Type: Float 0.001 Hartree the energy band tolerance, for determination which routines to use for calculating the numerical integration weights, when the energy band posses no or to less dispersion.
Enabled
Type: Bool No If true, the response function will be calculated using the old TD-CDFT implementation
Endfr
Type: Float 3.0 eV The upper bound frequency of the frequency range over which the dielectric function is calculated
Isz
Type: Integer 0 Integer indicating whether or not scalar zeroth order relativistic effects are included in the TDCDFT calculation. 0 = relativistic effects are not included, 1 = relativistic effects are included. The current implementation does NOT work with the option XC%SpinOrbitMagnetization equal NonCollinear
Iyxc
Type: Integer 0 integer for printing yxc-tensor (see http://aip.scitation.org/doi/10.1063/1.1385370). 0 = not printed, 1 = printed.
NewVK
Type: Bool Use the slightly modified version of the VK kernel (see https://aip.scitation.org/doi/10.1063/1.1385370). When using this option one uses effectively the static option, even for metals, so one should check carefully the convergence with the KSPACE parameter.
Nfreq
Type: Integer 5 the number of frequencies for which a linear response TD-CDFT calculation is performed.
QV
Type: Bool Use the QV parametrization for the longitudinal and transverse kernels of the XC kernel of the homogeneous electron gas. Use this in conjunction with the NewVK option. (see reference).
Shift
Type: Float 0.0 eV energy shift for the virtual crystal orbitals.
Static
Type: Bool An alternative method that allows an analytic evaluation of the static response (normally the static response is approximated by a finite small frequency value). This option should only be used for non-relativistic calculations on insulators, and it has no effect on metals. Note: experience shows that KSPACE convergence can be slower.
Strtfr
Type: Float 1.0 eV is the lower bound frequency of the frequency range over which the dielectric function is calculated.

References

  F. Kootstra, P.L. de Boeij and J.G. Snijders, Efficient real-space approach to time-dependent density functional theory for the dielectric response of nonmetallic crystals. Journal of Chemical Physics 112, 6517 (2000).
  P. Romaniello and P.L. de Boeij, Time-dependent current-density-functional theory for the metallic response of solids. Physical Review B 71, 155108 (2005).
  J.A. Berger, P.L. de Boeij and R. van Leeuwen, Analysis of the viscoelastic coefficients in the Vignale-Kohn functional: The cases of one- and three-dimensional polyacetylene., Physical Review B 71, 155104 (2005).
  P. Romaniello and P.L. de Boeij, Relativistic two-component formulation of time-dependent current-density functional theory: application to the linear response of solids., Journal of Chemical Physics 127, 174111 (2007).