# API reference

This page provides a plain list of all documented functions, structs, modules and macros in DFTK. Note that this list is neither structured, complete nor particularly clean, so it only provides rough orientation at the moment. The best reference is the code itself.

`DFTK.DFTK`

— ModuleDFTK –- The density-functional toolkit. Provides functionality for experimenting with plane-wave density-functional theory algorithms.

`DFTK.DFTK_DATADIR`

— ConstantThe default search location for Pseudopotential data files

`DFTK.timer`

— ConstantTimerOutput object used to store DFTK timings.

`DFTK.AbstractArchitecture`

— TypeAbstract supertype for architectures supported by DFTK.

`DFTK.AdaptiveBands`

— TypeDynamically adapt number of bands to be converged to ensure that the orbitals of lowest occupation are occupied to at most `occupation_threshold`

. To obtain rapid convergence of the eigensolver a gap between the eigenvalues of the last occupied orbital and the last computed (but not converged) orbital of `gap_min`

is ensured.

`DFTK.Applyχ0Model`

— TypeFull χ0 application, optionally dropping terms or disabling Sternheimer. All keyword arguments passed to `apply_χ0`

.

`DFTK.AtomicLocal`

— TypeAtomic local potential defined by `model.atoms`

.

`DFTK.AtomicNonlocal`

— TypeNonlocal term coming from norm-conserving pseudopotentials in Kleinmann-Bylander form. $\text{Energy} = \sum_a \sum_{ij} \sum_{n} f_n <ψ_n|p_{ai}> D_{ij} <p_{aj}|ψ_n>.$

`DFTK.BlowupAbinit`

— TypeBlow-up function as used in Abinit.

`DFTK.BlowupCHV`

— TypeBlow-up function as proposed in https://arxiv.org/abs/2210.00442 The blow-up order of the function is fixed to ensure C^2 regularity of the energies bands away from crossings and Lipschitz continuity at crossings.

`DFTK.BlowupIdentity`

— TypeDefault blow-up corresponding to the standard kinetic energies.

`DFTK.DielectricMixing`

— TypeWe use a simplification of the Resta model DOI 10.1103/physrevb.16.2717 and set $χ_0(q) = \frac{C_0 G^2}{4π (1 - C_0 G^2 / k_{TF}^2)}$ where $C_0 = 1 - ε_r$ with $ε_r$ being the macroscopic relative permittivity. We neglect $K_\text{xc}$, such that $J^{-1} ≈ \frac{k_{TF}^2 - C_0 G^2}{ε_r k_{TF}^2 - C_0 G^2}$

By default it assumes a relative permittivity of 10 (similar to Silicon). `εr == 1`

is equal to `SimpleMixing`

and `εr == Inf`

to `KerkerMixing`

. The mixing is applied to $ρ$ and $ρ_\text{spin}$ in the same way.

`DFTK.DielectricModel`

— TypeA localised dielectric model for $χ_0$:

\[\sqrt{L(x)} \text{IFFT} \frac{C_0 G^2}{4π (1 - C_0 G^2 / k_{TF}^2)} \text{FFT} \sqrt{L(x)}\]

where $C_0 = 1 - ε_r$, `L(r)`

is a real-space localization function and otherwise the same conventions are used as in `DielectricMixing`

.

`DFTK.DivAgradOperator`

— TypeNonlocal "divAgrad" operator $-½ ∇ ⋅ (A ∇)$ where $A$ is a scalar field on the real-space grid. The $-½$ is included, such that this operator is a generalisation of the kinetic energy operator (which is obtained for $A=1$).

`DFTK.ElementCohenBergstresser`

— MethodElement where the interaction with electrons is modelled as in CohenBergstresser1966. Only the homonuclear lattices of the diamond structure are implemented (i.e. Si, Ge, Sn).

`key`

may be an element symbol (like `:Si`

), an atomic number (e.g. `14`

) or an element name (e.g. `"silicon"`

)

`DFTK.ElementCoulomb`

— MethodElement interacting with electrons via a bare Coulomb potential (for all-electron calculations) `key`

may be an element symbol (like `:Si`

), an atomic number (e.g. `14`

) or an element name (e.g. `"silicon"`

)

`DFTK.ElementGaussian`

— MethodElement interacting with electrons via a Gaussian potential. Symbol is non-mandatory.

`DFTK.ElementPsp`

— MethodElement interacting with electrons via a pseudopotential model. `key`

may be an element symbol (like `:Si`

), an atomic number (e.g. `14`

) or an element name (e.g. `"silicon"`

)

`DFTK.Energies`

— TypeA simple struct to contain a vector of energies, and utilities to print them in a nice format.

`DFTK.Entropy`

— TypeEntropy term -TS, where S is the electronic entropy. Turns the energy E into the free energy F=E-TS. This is in particular useful because the free energy, not the energy, is minimized at self-consistency.

`DFTK.Ewald`

— TypeEwald term: electrostatic energy per unit cell of the array of point charges defined by `model.atoms`

in a uniform background of compensating charge yielding net neutrality.

`DFTK.ExternalFromFourier`

— TypeExternal potential from the (unnormalized) Fourier coefficients `V(G)`

G is passed in cartesian coordinates

`DFTK.ExternalFromReal`

— TypeExternal potential from an analytic function `V`

(in cartesian coordinates). No low-pass filtering is performed.

`DFTK.FermiTwoStage`

— TypeTwo-stage Fermi level finding algorithm starting from a Gaussian-smearing guess.

`DFTK.FixedBands`

— TypeIn each SCF step converge exactly `n_bands_converge`

, computing along the way exactly `n_bands_compute`

(usually a few more to ease convergence in systems with small gaps).

`DFTK.FourierMultiplication`

— TypeFourier space multiplication, like a kinetic energy term: (Hψ)(G) = multiplier(G) ψ(G).

`DFTK.GPU`

— MethodConstruct a particular GPU architecture by passing the ArrayType

`DFTK.Hartree`

— TypeHartree term: for a decaying potential V the energy would be

1/2 ∫ρ(x)ρ(y)V(x-y) dxdy

with the integral on x in the unit cell and of y in the whole space. For the Coulomb potential with periodic boundary conditions, this is rather

1/2 ∫ρ(x)ρ(y) G(x-y) dx dy

where G is the Green's function of the periodic Laplacian with zero mean (-Δ G = sum*{R} 4π δ*R, integral of G zero on a unit cell).

`DFTK.KerkerDosMixing`

— TypeThe same as `KerkerMixing`

, but the Thomas-Fermi wavevector is computed from the current density of states at the Fermi level.

`DFTK.KerkerMixing`

— TypeKerker mixing: $J^{-1} ≈ \frac{|G|^2}{k_{TF}^2 + |G|^2}$ where $k_{TF}$ is the Thomas-Fermi wave vector. For spin-polarized calculations by default the spin density is not preconditioned. Unless a non-default value for $ΔDOS_Ω$ is specified. This value should roughly be the expected difference in density of states (per unit volume) between spin-up and spin-down.

Notes:

- Abinit calls $1/k_{TF}$ the dielectric screening length (parameter
*dielng*)

`DFTK.Kinetic`

— TypeKinetic energy: 1/2 sum*n f*n ∫ |∇ψn|^2 * blowup(-i∇Ψ).

`DFTK.Kpoint`

— TypeDiscretization information for $k$-point-dependent quantities such as orbitals. More generally, a $k$-point is a block of the Hamiltonian; eg collinear spin is treated by doubling the number of kpoints.

`DFTK.LazyHcat`

— TypeSimple wrapper to represent a matrix formed by the concatenation of column blocks: it is mostly equivalent to hcat, but doesn't allocate the full matrix. LazyHcat only supports a few multiplication routines: furthermore, a multiplication involving this structure will always yield a plain array (and not a LazyHcat structure). LazyHcat is a lightweight subset of BlockArrays.jl's functionalities, but has the advantage to be able to store GPU Arrays (BlockArrays is heavily built on Julia's CPU Array).

`DFTK.LdosModel`

— TypeRepresents the LDOS-based $χ_0$ model

\[χ_0(r, r') = (-D_\text{loc}(r) δ(r, r') + D_\text{loc}(r) D_\text{loc}(r') / D)\]

where $D_\text{loc}$ is the local density of states and $D$ the density of states. For details see Herbst, Levitt 2020 arXiv:2009.01665

`DFTK.LibxcDensities`

— MethodCompute density in real space and its derivatives starting from ρ

`DFTK.LocalNonlinearity`

— TypeLocal nonlinearity, with energy ∫f(ρ) where ρ is the density

`DFTK.Magnetic`

— TypeMagnetic term $A⋅(-i∇)$. It is assumed (but not checked) that $∇⋅A = 0$.

`DFTK.MagneticFieldOperator`

— TypeMagnetic field operator A⋅(-i∇).

`DFTK.Model`

— Method`Model(system::AbstractSystem; kwargs...)`

AtomsBase-compatible Model constructor. Sets structural information (`atoms`

, `positions`

, `lattice`

, `n_electrons`

etc.) from the passed `system`

.

`DFTK.Model`

— Method```
Model(lattice, atoms, positions; n_electrons, magnetic_moments, terms, temperature,
smearing, spin_polarization, symmetries)
```

Creates the physical specification of a model (without any discretization information).

`n_electrons`

is taken from `atoms`

if not specified.

`spin_polarization`

is :none by default (paired electrons) unless any of the elements has a non-zero initial magnetic moment. In this case the spin_polarization will be :collinear.

`magnetic_moments`

is only used to determine the symmetry and the `spin_polarization`

; it is not stored inside the datastructure.

`smearing`

is Fermi-Dirac if `temperature`

is non-zero, none otherwise

The `symmetries`

kwarg allows (a) to pass `true`

/ `false`

to enable / disable the automatic determination of lattice symmetries or (b) to pass an explicit list of symmetry operations to use for lowering the computational effort. The default behaviour is equal to `true`

, namely that the code checks the specified model in form of the Hamiltonian `terms`

, `lattice`

, `atoms`

and `magnetic_moments`

parameters and from these automatically determines a set of symmetries it can safely use. If you want to pass custom symmetry operations (e.g. a reduced or extended set) use the `symmetry_operations`

function. Notice that this may lead to wrong results if e.g. the external potential breaks some of the passed symmetries. Use `false`

to turn off symmetries completely.

`DFTK.Model`

— Method```
Model(model; [lattice, positions, atoms, kwargs...])
Model{T}(model; [lattice, positions, atoms, kwargs...])
```

Construct an identical model to `model`

with the option to change some of the contained parameters. This constructor is useful for changing the data type in the model or for changing `lattice`

or `positions`

in geometry/lattice optimisations.

`DFTK.NbandsAlgorithm`

— TypeNbandsAlgorithm subtypes determine how many bands to compute and converge in each SCF step.

`DFTK.NonlocalOperator`

— TypeNonlocal operator in Fourier space in Kleinman-Bylander format, defined by its projectors P matrix and coupling terms D: Hψ = PDP' ψ.

`DFTK.NoopOperator`

— TypeNoop operation: don't do anything. Useful for energy terms that don't depend on the orbitals at all (eg nuclei-nuclei interaction).

`DFTK.PairwisePotential`

— MethodPairwise terms: Pairwise potential between nuclei, e.g., Van der Waals potentials, such as Lennard—Jones terms. The potential is dependent on the distance between to atomic positions and the pairwise atomic types: For a distance `d`

between to atoms `A`

and `B`

, the potential is `V(d, params[(A, B)])`

. The parameters `max_radius`

is of `100`

by default, and gives the maximum distance (in Cartesian coordinates) between nuclei for which we consider interactions.

`DFTK.PlaneWaveBasis`

— TypeA plane-wave discretized `Model`

. Normalization conventions:

- Things that are expressed in the G basis are normalized so that if $x$ is the vector, then the actual function is $\sum_G x_G e_G$ with $e_G(x) = e^{iG x} / \sqrt(\Omega)$, where $\Omega$ is the unit cell volume. This is so that, eg $norm(ψ) = 1$ gives the correct normalization. This also holds for the density and the potentials.
- Quantities expressed on the real-space grid are in actual values.

`ifft`

and `fft`

convert between these representations.

`DFTK.PlaneWaveBasis`

— MethodCreates a `PlaneWaveBasis`

using the kinetic energy cutoff `Ecut`

and a Monkhorst-Pack $k$-point grid. The MP grid can either be specified directly with `kgrid`

providing the number of points in each dimension and `kshift`

the shift (0 or 1/2 in each direction). If not specified a grid is generated using `kgrid_from_minimal_spacing`

with a minimal spacing of `2π * 0.022`

per Bohr.

`DFTK.PlaneWaveBasis`

— MethodCreates a new basis identical to `basis`

, but with a custom set of kpoints

`DFTK.PreconditionerNone`

— TypeNo preconditioning

`DFTK.PreconditionerTPA`

— Type(simplified version of) Tetter-Payne-Allan preconditioning ↑ M.P. Teter, M.C. Payne and D.C. Allan, Phys. Rev. B 40, 12255 (1989).

`DFTK.PspCorrection`

— TypePseudopotential correction energy. TODO discuss the need for this.

`DFTK.PspHgh`

— Method`PspHgh(path[, identifier, description])`

Construct a Hartwigsen, Goedecker, Teter, Hutter separable dual-space Gaussian pseudopotential (1998) from file.

`DFTK.PspUpf`

— Method`PspUpf(path[, identifier])`

Construct a Unified Pseudopotential Format pseudopotential from file.

Does not support:

- Non-linear core correction
- Fully-realtivistic / spin-orbit pseudos
- Bare Coulomb / all-electron potentials
- Semilocal potentials
- Ultrasoft potentials
- Projector-augmented wave potentials
- GIPAW reconstruction data

`DFTK.RealFourierOperator`

— TypeLinear operators that act on tuples (real, fourier) The main entry point is `apply!(out, op, in)`

which performs the operation out += op*in where out and in are named tuples (real, fourier) They also implement mul! and Matrix(op) for exploratory use.

`DFTK.RealSpaceMultiplication`

— TypeReal space multiplication by a potential: (Hψ)(r) = V(r) ψ(r).

`DFTK.SimpleMixing`

— TypeSimple mixing: $J^{-1} ≈ 1$

`DFTK.TermNoop`

— TypeA term with a constant zero energy.

`DFTK.Xc`

— TypeExchange-correlation term, defined by a list of functionals and usually evaluated through libxc.

`DFTK.χ0Mixing`

— TypeGeneric mixing function using a model for the susceptibility composed of the sum of the `χ0terms`

. For valid `χ0terms`

See the subtypes of `χ0Model`

. The dielectric model is solved in real space using a GMRES. Either the full kernel (`RPA=false`

) or only the Hartree kernel (`RPA=true`

) are employed. `verbose=true`

lets the GMRES run in verbose mode (useful for debugging).

`AbstractFFTs.fft!`

— MethodIn-place version of `fft!`

. NOTE: If `kpt`

is given, not only `f_fourier`

but also `f_real`

is overwritten.

`AbstractFFTs.fft`

— Method`fft(basis::PlaneWaveBasis, [kpt::Kpoint, ] f_real)`

Perform an FFT to obtain the Fourier representation of `f_real`

. If `kpt`

is given, the coefficients are truncated to the k-dependent spherical basis set.

`AbstractFFTs.ifft!`

— MethodIn-place version of `ifft`

.

`AbstractFFTs.ifft`

— Method`ifft(basis::PlaneWaveBasis, [kpt::Kpoint, ] f_fourier)`

Perform an iFFT to obtain the quantity defined by `f_fourier`

defined on the k-dependent spherical basis set (if `kpt`

is given) or the k-independent cubic (if it is not) on the real-space grid.

`AtomsBase.atomic_symbol`

— MethodChemical symbol corresponding to an element

`AtomsBase.atomic_system`

— Function```
atomic_system(model::DFTK.Model, magnetic_moments=[])
atomic_system(lattice, atoms, positions, magnetic_moments=[])
```

Construct an AtomsBase atomic system from a DFTK `model`

and associated magnetic moments or from the usual `lattice`

, `atoms`

and `positions`

list used in DFTK plus magnetic moments.

`AtomsBase.periodic_system`

— Function```
periodic_system(model::DFTK.Model, magnetic_moments=[])
periodic_system(lattice, atoms, positions, magnetic_moments=[])
```

Construct an AtomsBase atomic system from a DFTK `model`

and associated magnetic moments or from the usual `lattice`

, `atoms`

and `positions`

list used in DFTK plus magnetic moments.

`Brillouin.KPaths.irrfbz_path`

— MethodExtract the high-symmetry $k$-point path corresponding to the passed `model`

using `Brillouin`

. Uses the conventions described in the reference work by Cracknell, Davies, Miller, and Love (CDML). Of note, this has minor differences to the $k$-path reference (Y. Himuma et. al. Comput. Mater. Sci. **128**, 140 (2017)) underlying the path-choices of `Brillouin.jl`

, specifically for oA and mC Bravais types.

If the cell is a supercell of a smaller primitive cell, the standard $k$-path of the associated primitive cell is returned. So, the high-symmetry $k$ points are those of the primitive cell Brillouin zone, not those of the supercell Brillouin zone.

The `dim`

argument allows to artificially truncate the dimension of the employed model, e.g. allowing to plot a 2D bandstructure of a 3D model (useful for example for plotting band structures of sheets with `dim=2`

).

Due to lacking support in `Spglib.jl`

for two-dimensional lattices it is (a) assumed that `model.lattice`

is a *conventional* lattice and (b) required to pass the space group number using the `sgnum`

keyword argument.

`DFTK.CROP`

— FunctionCROP-accelerated root-finding iteration for `f`

, starting from `x0`

and keeping a history of `m`

steps. Optionally `warming`

specifies the number of non-accelerated steps to perform for warming up the history.

`DFTK.G_vectors`

— Method```
G_vectors(basis::PlaneWaveBasis)
G_vectors(basis::PlaneWaveBasis, kpt::Kpoint)
```

The list of wave vectors $G$ in reduced (integer) coordinates of a `basis`

or a $k$-point `kpt`

.

`DFTK.G_vectors`

— Method`G_vectors([architecture=AbstractArchitecture], fft_size::Tuple)`

The wave vectors `G`

in reduced (integer) coordinates for a cubic basis set of given sizes.

`DFTK.G_vectors_cart`

— Method```
G_vectors_cart(basis::PlaneWaveBasis)
G_vectors_cart(basis::PlaneWaveBasis, kpt::Kpoint)
```

The list of $G$ vectors of a given `basis`

or `kpt`

, in cartesian coordinates.

`DFTK.Gplusk_vectors`

— Method`Gplusk_vectors(basis::PlaneWaveBasis, kpt::Kpoint)`

The list of $G + k$ vectors, in reduced coordinates.

`DFTK.Gplusk_vectors_cart`

— Method`Gplusk_vectors_cart(basis::PlaneWaveBasis, kpt::Kpoint)`

The list of $G + k$ vectors, in cartesian coordinates.

`DFTK.Gplusk_vectors_in_supercell`

— MethodMaps all $k+G$ vectors of an given basis as $G$ vectors of the supercell basis, in reduced coordinates.

`DFTK.HybridMixing`

— MethodThe model for the susceptibility is

\[\begin{aligned} χ_0(r, r') &= (-D_\text{loc}(r) δ(r, r') + D_\text{loc}(r) D_\text{loc}(r') / D) \\ &+ \sqrt{L(x)} \text{IFFT} \frac{C_0 G^2}{4π (1 - C_0 G^2 / k_{TF}^2)} \text{FFT} \sqrt{L(x)} \end{aligned}\]

where $C_0 = 1 - ε_r$, $D_\text{loc}$ is the local density of states, $D$ is the density of states and the same convention for parameters are used as in `DielectricMixing`

. Additionally there is the real-space localization function `L(r)`

. For details see Herbst, Levitt 2020 arXiv:2009.01665

Important `kwargs`

passed on to `χ0Mixing`

`RPA`

: Is the random-phase approximation used for the kernel (i.e. only Hartree kernel is used and not XC kernel)`verbose`

: Run the GMRES in verbose mode.`reltol`

: Relative tolerance for GMRES

`DFTK.IncreaseMixingTemperature`

— MethodIncrease the temperature used for computing the SCF preconditioners. Initially the temperature is increased by a `factor`

, which is then smoothly lowered towards the temperature used within the model as the SCF converges. Once the density change is below `above_ρdiff`

the mixing temperature is equal to the model temperature.

`DFTK.LdosMixing`

— MethodThe model for the susceptibility is

\[\begin{aligned} χ_0(r, r') &= (-D_\text{loc}(r) δ(r, r') + D_\text{loc}(r) D_\text{loc}(r') / D) \end{aligned}\]

where $D_\text{loc}$ is the local density of states, $D$ is the density of states. For details see Herbst, Levitt 2020 arXiv:2009.01665.

Important `kwargs`

passed on to `χ0Mixing`

`RPA`

: Is the random-phase approximation used for the kernel (i.e. only Hartree kernel is used and not XC kernel)`verbose`

: Run the GMRES in verbose mode.`reltol`

: Relative tolerance for GMRES

`DFTK.ScfAcceptImprovingStep`

— MethodAccept a step if the energy is at most increasing by `max_energy`

and the residual is at most `max_relative_residual`

times the residual in the previous step.

`DFTK.ScfConvergenceDensity`

— MethodFlag convergence by using the L2Norm of the change between input density and unpreconditioned output density (ρout)

`DFTK.ScfConvergenceEnergy`

— MethodFlag convergence as soon as total energy change drops below tolerance

`DFTK.ScfConvergenceForce`

— MethodFlag convergence on the change in cartesian force between two iterations.

`DFTK.ScfDefaultCallback`

— MethodDefault callback function for `self_consistent_field`

and `newton`

, which prints a convergence table.

`DFTK.ScfDiagtol`

— MethodDetermine the tolerance used for the next diagonalization. This function takes $|ρnext - ρin|$ and multiplies it with `ratio_ρdiff`

to get the next `diagtol`

, ensuring additionally that the returned value is between `diagtol_min`

and `diagtol_max`

and never increases.

`DFTK.ScfPlotTrace`

— FunctionPlot the trace of an SCF, i.e. the absolute error of the total energy at each iteration versus the converged energy in a semilog plot. By default a new plot canvas is generated, but an existing one can be passed and reused along with `kwargs`

for the call to `plot!`

. Requires Plots to be loaded.

`DFTK.ScfSaveCheckpoints`

— FunctionAdds simplistic checkpointing to a DFTK self-consistent field calculation. Requires JLD2 to be loaded.

`DFTK.apply_K`

— Method`apply_K(basis::PlaneWaveBasis, δψ, ψ, ρ, occupation)`

Compute the application of K defined at ψ to δψ. ρ is the density issued from ψ. δψ also generates a δρ, computed with `compute_δρ`

.

`DFTK.apply_kernel`

— Method`apply_kernel(basis::PlaneWaveBasis, δρ; kwargs...)`

Computes the potential response to a perturbation δρ in real space, as a 4D (i,j,k,σ) array.

`DFTK.apply_symop`

— MethodApply a symmetry operation to eigenvectors `ψk`

at a given `kpoint`

to obtain an equivalent point in [-0.5, 0.5)^3 and associated eigenvectors (expressed in the basis of the new $k$-point).

`DFTK.apply_symop`

— MethodApply a symmetry operation to a density.

`DFTK.apply_Ω`

— Method`apply_Ω(δψ, ψ, H::Hamiltonian, Λ)`

Compute the application of Ω defined at ψ to δψ. H is the Hamiltonian computed from ψ and Λ is the set of Rayleigh coefficients ψk' * Hk * ψk at each k-point.

`DFTK.apply_χ0`

— MethodGet the density variation δρ corresponding to a potential variation δV.

`DFTK.attach_psp`

— Method```
attach_psp(system::AbstractSystem, pspmap::AbstractDict{Symbol,String})
attach_psp(system::AbstractSystem; psps::String...)
```

Return a new system with the `pseudopotential`

property of all atoms set according to the passed `pspmap`

, which maps from the atomic symbol to a pseudopotential identifier. Alternatively the mapping from atomic symbol to pseudopotential identifier can also be passed as keyword arguments. An empty string can be used to denote elements where the full Coulomb potential should be employed.

**Examples**

Select pseudopotentials for all silicon and oxygen atoms in the system.

`julia> attach_psp(system, Dict(:Si => "hgh/lda/si-q4", :O => "hgh/lda/o-q6")`

Same thing but using the kwargs syntax:

`julia> attach_psp(system, Si="hgh/lda/si-q4", O="hgh/lda/o-q6")`

`DFTK.build_fft_plans!`

— MethodPlan a FFT of type `T`

and size `fft_size`

, spending some time on finding an optimal algorithm. (Inplace, out-of-place) x (forward, backward) FFT plans are returned.

`DFTK.build_form_factors`

— MethodBuild form factors (Fourier transforms of projectors) for an atom centered at 0.

`DFTK.build_projection_vectors_`

— MethodBuild projection vectors for a atoms array generated by term_nonlocal

\[\begin{aligned} H_{\rm at} &= \sum_{ij} C_{ij} \ket{p_i} \bra{p_j} \\ H_{\rm per} &= \sum_R \sum_{ij} C_{ij} \ket{p_i(x-R)} \bra{p_j(x-R)} \end{aligned}\]

\[\begin{aligned} \braket{e_k(G') \middle| H_{\rm per}}{e_k(G)} &= \ldots \\ &= \frac{1}{Ω} \sum_{ij} C_{ij} \hat p_i(k+G') \hat p_j^*(k+G), \end{aligned}\]

where $\hat p_i(q) = ∫_{ℝ^3} p_i(r) e^{-iq·r} dr$.

We store $\frac{1}{\sqrt Ω} \hat p_i(k+G)$ in `proj_vectors`

.

`DFTK.bzmesh_ir_wedge`

— Method` bzmesh_ir_wedge(kgrid_size, symmetries; kshift=[0, 0, 0])`

Construct the irreducible wedge of a uniform Brillouin zone mesh for sampling $k$-points, given the crystal symmetries `symmetries`

. Returns the list of irreducible $k$-point (fractional) coordinates, the associated weights and the new `symmetries`

compatible with the grid.

`DFTK.bzmesh_uniform`

— Method`bzmesh_uniform(kgrid_size; kshift=[0, 0, 0])`

Construct a (shifted) uniform Brillouin zone mesh for sampling the $k$-points. Returns all $k$-point coordinates, appropriate weights and the identity SymOp.

`DFTK.cell_to_supercell`

— MethodTranspose all data from a given self-consistent-field result from unit cell to supercell conventions. The parameters to adapt are the following:

`basis_supercell`

and`ψ_supercell`

are computed by the routines above.- The supercell occupations vector is the concatenation of all input occupations vectors.
- The supercell density is computed with supercell occupations and
`ψ_supercell`

. - Supercell energies are the multiplication of input energies by the number of unit cells in the supercell.

Other parameters stay untouched.

`DFTK.cell_to_supercell`

— MethodConstruct a plane-wave basis whose unit cell is the supercell associated to an input basis $k$-grid. All other parameters are modified so that the respective physical systems associated to both basis are equivalent.

`DFTK.cell_to_supercell`

— MethodRe-organize Bloch waves computed in a given basis as Bloch waves of the associated supercell basis. The output `ψ_supercell`

have a single component at $Γ$-point, such that `ψ_supercell[Γ][:, k+n]`

contains `ψ[k][:, n]`

, within normalization on the supercell.

`DFTK.cg!`

— MethodImplementation of the conjugate gradient method which allows for preconditioning and projection operations along iterations.

`DFTK.charge_ionic`

— MethodReturn the total ionic charge of an atom type (nuclear charge - core electrons)

`DFTK.charge_nuclear`

— MethodReturn the total nuclear charge of an atom type

`DFTK.cis2pi`

— MethodFunction to compute exp(2π i x)

`DFTK.compute_Ak_gaussian_guess`

— MethodCompute the matrix $[A_k]_{m,n} = \langle ψ_m^k | g^{\text{per}}_n \rangle$

$g^{per}_n$ are periodized gaussians whose respective centers are given as an (num_bands,1) array [ [center 1], ... ].

Centers are to be given in lattice coordinates and G_vectors in reduced coordinates. The dot product is computed in the Fourier space.

Given an orbital $g_n$, the periodized orbital is defined by : $g^{per}_n = \sum\limits_{R \in {\rm lattice}} g_n( \cdot - R)$. The Fourier coefficient of $g^{per}_n$ at any G is given by the value of the Fourier transform of $g_n$ in G.

`DFTK.compute_current`

— MethodComputes the *probability* (not charge) current, ∑ fn Im(ψn* ∇ψn)

`DFTK.compute_density`

— Method`compute_density(basis::PlaneWaveBasis, ψ::AbstractVector, occupation::AbstractVector)`

Compute the density for a wave function `ψ`

discretized on the plane-wave grid `basis`

, where the individual k-points are occupied according to `occupation`

. `ψ`

should be one coefficient matrix per $k$-point. It is possible to ask only for occupations higher than a certain level to be computed by using an optional `occupation_threshold`

. By default all occupation numbers are considered.

`DFTK.compute_dos`

— MethodTotal density of states at energy ε

`DFTK.compute_fft_size`

— MethodDetermine the minimal grid size for the cubic basis set to be able to represent product of orbitals (with the default `supersampling=2`

).

Optionally optimize the grid afterwards for the FFT procedure by ensuring factorization into small primes.

The function will determine the smallest parallelepiped containing the wave vectors $|G|^2/2 \leq E_\text{cut} ⋅ \text{supersampling}^2$. For an exact representation of the density resulting from wave functions represented in the spherical basis sets, `supersampling`

should be at least `2`

.

If `factors`

is not empty, ensure that the resulting fft_size contains all the factors

`DFTK.compute_forces`

— MethodCompute the forces of an obtained SCF solution. Returns the forces wrt. the fractional lattice vectors. To get cartesian forces use `compute_forces_cart`

. Returns a list of lists of forces (as SVector{3}) in the same order as the `atoms`

and `positions`

in the underlying `Model`

.

`DFTK.compute_forces_cart`

— MethodCompute the cartesian forces of an obtained SCF solution in Hartree / Bohr. Returns a list of lists of forces `[[force for atom in positions] for (element, positions) in atoms]`

which has the same structure as the `atoms`

object passed to the underlying `Model`

.

`DFTK.compute_inverse_lattice`

— MethodCompute the inverse of the lattice. Takes special care of 1D or 2D cases.

`DFTK.compute_kernel`

— Method`compute_kernel(basis::PlaneWaveBasis; kwargs...)`

Computes a matrix representation of the full response kernel (derivative of potential with respect to density) in real space. For non-spin-polarized calculations the matrix dimension is `prod(basis.fft_size)`

× `prod(basis.fft_size)`

and for collinear spin-polarized cases it is `2prod(basis.fft_size)`

× `2prod(basis.fft_size)`

. In this case the matrix has effectively 4 blocks

\[\left(\begin{array}{cc} K_{αα} & K_{αβ}\\ K_{βα} & K_{ββ} \end{array}\right)\]

`DFTK.compute_ldos`

— MethodLocal density of states, in real space. `weight_threshold`

is a threshold to screen away small contributions to the LDOS.

`DFTK.compute_occupation`

— MethodCompute occupation given eigenvalues and Fermi level

`DFTK.compute_occupation`

— MethodCompute occupation and Fermi level given eigenvalues and using `fermialg`

. The `tol_n_elec`

gives the accuracy on the electron count which should be at least achieved.

`DFTK.compute_recip_lattice`

— MethodCompute the reciprocal lattice. We use the convention that the reciprocal lattice is the set of G vectors such that G ⋅ R ∈ 2π ℤ for all R in the lattice.

`DFTK.compute_stresses_cart`

— MethodCompute the stresses (= 1/Vol dE/d(M*lattice), taken at M=I) of an obtained SCF solution.

`DFTK.compute_transfer_matrix`

— MethodReturn a sparse matrix that maps quantities given on `basis_in`

and `kpt_in`

to quantities on `basis_out`

and `kpt_out`

.

`DFTK.compute_transfer_matrix`

— MethodReturn a list of sparse matrices (one per $k$-point) that map quantities given in the `basis_in`

basis to quantities given in the `basis_out`

basis.

`DFTK.compute_unit_cell_volume`

— MethodCompute unit cell volume volume. In case of 1D or 2D case, the volume is the length/surface.

`DFTK.compute_δocc!`

— MethodCompute the derivatives of the occupations (and of the Fermi level). The derivatives of the occupations are in-place stored in δocc. The tuple (; δocc, δεF) is returned. It is assumed the passed `δocc`

are initialised to zero.

`DFTK.compute_δψ!`

— MethodPerform in-place computations of the derivatives of the wave functions by solving a Sternheimer equation for each `k`

-points. It is assumed the passed `δψ`

are initialised to zero.

`DFTK.compute_χ0`

— MethodCompute the independent-particle susceptibility. Will blow up for large systems. For non-spin-polarized calculations the matrix dimension is `prod(basis.fft_size)`

× `prod(basis.fft_size)`

and for collinear spin-polarized cases it is `2prod(basis.fft_size)`

× `2prod(basis.fft_size)`

. In this case the matrix has effectively 4 blocks, which are:

\[\left(\begin{array}{cc} (χ_0)_{αα} & (χ_0)_{αβ} \\ (χ_0)_{βα} & (χ_0)_{ββ} \end{array}\right)\]

`DFTK.cos2pi`

— MethodFunction to compute cos(2π x)

`DFTK.count_n_proj`

— Method`count_n_proj(psps, psp_positions)`

Number of projector functions for all angular momenta up to `psp.lmax`

and for all atoms in the system, including angular parts from `-m:m`

.

`DFTK.count_n_proj`

— Method`count_n_proj(psp, l)`

Number of projector functions for angular momentum `l`

, including angular parts from `-m:m`

.

`DFTK.count_n_proj`

— Method`count_n_proj(psp)`

Number of projector functions for all angular momenta up to `psp.lmax`

, including angular parts from `-m:m`

.

`DFTK.count_n_proj_radial`

— Method`count_n_proj_radial(psp, l)`

Number of projector radial functions at angular momentum `l`

.

`DFTK.count_n_proj_radial`

— Method`count_n_proj_radial(psp)`

Number of projector radial functions at all angular momenta up to `psp.lmax`

.

`DFTK.create_supercell`

— MethodConstruct a supercell of size `supercell_size`

from a unit cell described by its `lattice`

, `atoms`

and their `positions`

.

`DFTK.datadir_psp`

— MethodReturn the data directory with pseudopotential files

`DFTK.default_fermialg`

— MethodDefault selection of a Fermi level determination algorithm

`DFTK.default_spin_polarization`

— Method`:none`

if no element has a magnetic moment, else `:collinear`

or `:full`

.

`DFTK.default_symmetries`

— MethodDefault logic to determine the symmetry operations to be used in the model.

`DFTK.default_wannier_centres`

— MethodDefault random Gaussian guess for maximally-localised wannier functions generated in reduced coordinates.

`DFTK.diagonalize_all_kblocks`

— MethodFunction for diagonalising each $k$-Point blow of ham one step at a time. Some logic for interpolating between $k$-points is used if `interpolate_kpoints`

is true and if no guesses are given. `eigensolver`

is the iterative eigensolver that really does the work, operating on a single $k$-Block. `eigensolver`

should support the API `eigensolver(A, X0; prec, tol, maxiter)`

`prec_type`

should be a function that returns a preconditioner when called as `prec(ham, kpt)`

`DFTK.diameter`

— MethodCompute the diameter of the unit cell

`DFTK.direct_minimization`

— MethodComputes the ground state by direct minimization. `kwargs...`

are passed to `Optim.Options()`

. Note that the resulting ψ are not necessarily eigenvectors of the Hamiltonian.

`DFTK.disable_threading`

— MethodConvenience function to disable all threading in DFTK and assert that Julia threading is off as well.

`DFTK.divergence_real`

— MethodCompute divergence of an operand function, which returns the cartesian x,y,z components in real space when called with the arguments 1 to 3. The divergence is also returned as a real-space array.

`DFTK.energy_ewald`

— MethodCompute the electrostatic interaction energy per unit cell between point charges in a uniform background of compensating charge to yield net neutrality.`lattice`

should contain the lattice vectors as columns. `charges`

and `positions`

are the point charges and their positions (as an array of arrays) in fractional coordinates. If `forces`

is not nothing, minus the derivatives of the energy with respect to `positions`

is computed.

For now this function returns zero energy and force on non-3D systems. Use a pairwise potential term if you want to customise this treatment.

`DFTK.energy_pairwise`

— MethodCompute the pairwise interaction energy per unit cell between atomic sites. If `forces`

is not nothing, minus the derivatives of the energy with respect to `positions`

is computed. The potential is expected to decrease quickly at infinity.

`DFTK.energy_psp_correction`

— MethodCompute the correction term for properly modelling the interaction of the pseudopotential core with the compensating background charge induced by the `Ewald`

term.

`DFTK.enforce_real!`

— MethodEnsure its real-space equivalent of passed Fourier-space representation is entirely real by removing wavevectors `G`

that don't have a `-G`

counterpart in the basis.

`DFTK.estimate_integer_lattice_bounds`

— MethodEstimate integer bounds for dense space loops from a given inequality ||Mx|| ≤ δ. For 1D and 2D systems the limit will be zero in the auxiliary dimensions.

`DFTK.eval_psp_density_core_fourier`

— Method`eval_psp_density_core_fourier(psp, q)`

Evaluate the atomic core charge density in reciprocal space: ρval(q) = ∫*{R^3} ρcore(r) e^{-iqr} dr = 4π ∫*{R+} ρcore(r) sin(qr)/qr r^2 dr

`DFTK.eval_psp_density_core_real`

— Method`eval_psp_density_core_real(psp, r)`

Evaluate the atomic core charge density in real space.

`DFTK.eval_psp_density_valence_fourier`

— Method`eval_psp_density_valence_fourier(psp, q)`

Evaluate the atomic valence charge density in reciprocal space: ρval(q) = ∫*{R^3} ρval(r) e^{-iqr} dr = 4π ∫*{R+} ρval(r) sin(qr)/qr r^2 dr

`DFTK.eval_psp_density_valence_real`

— Method`eval_psp_density_valence_real(psp, r)`

Evaluate the atomic valence charge density in real space.

`DFTK.eval_psp_energy_correction`

— Function`eval_psp_energy_correction([T=Float64,] psp, n_electrons)`

Evaluate the energy correction to the Ewald electrostatic interaction energy of one unit cell, which is required compared the Ewald expression for point-like nuclei. `n_electrons`

is the number of electrons per unit cell. This defines the uniform compensating background charge, which is assumed here.

Notice: The returned result is the *energy per unit cell* and not the energy per volume. To obtain the latter, the caller needs to divide by the unit cell volume.

The energy correction is defined as the limit of the Fourier-transform of the local potential as $q \to 0$, using the same correction as in the Fourier-transform of the local potential: `math \lim_{q \to 0} 4π N_{\rm elec} ∫_{ℝ_+} (V(r) - C(r)) \frac{\sin(qr)}{qr} r^2 dr + F[C(r)] = 4π N_{\rm elec} ∫_{ℝ_+} (V(r) + Z/r) r^2 dr`

`DFTK.eval_psp_local_fourier`

— Method`eval_psp_local_fourier(psp, q)`

Evaluate the local part of the pseudopotential in reciprocal space:

\[\begin{aligned} V_{\rm loc}(q) &= ∫_{ℝ^3} V_{\rm loc}(r) e^{-iqr} dr \\ &= 4π ∫_{ℝ_+} V_{\rm loc}(r) \frac{\sin(qr)}{q} r dr \end{aligned}\]

In practice, the local potential should be corrected using a Coulomb-like term $C(r) = -Z/r$ to remove the long-range tail of $V_{\rm loc}(r)$ from the integral:

\[\begin{aligned} V_{\rm loc}(q) &= ∫_{ℝ^3} (V_{\rm loc}(r) - C(r)) e^{-iq·r} dr + F[C(r)] \\ &= 4π ∫_{ℝ_+} (V_{\rm loc}(r) + Z/r) \frac{\sin(qr)}{qr} r^2 dr - Z/q^2 \end{aligned}\]

`DFTK.eval_psp_local_real`

— Method`eval_psp_local_real(psp, r)`

Evaluate the local part of the pseudopotential in real space.

`DFTK.eval_psp_projector_fourier`

— Method`eval_psp_projector_fourier(psp, i, l, q)`

Evaluate the radial part of the `i`

-th projector for angular momentum `l`

at the reciprocal vector with modulus `q`

:

\[\begin{aligned} p(q) &= ∫_{ℝ^3} p_{il}(r) e^{-iq·r} dr \\ &= 4π ∫_{ℝ_+} r^2 p_{il}(r) j_l(qr) dr \end{aligned}\]

`DFTK.eval_psp_projector_real`

— Method`eval_psp_projector_real(psp, i, l, r)`

Evaluate the radial part of the `i`

-th projector for angular momentum `l`

in real-space at the vector with modulus `r`

.

`DFTK.filled_occupation`

— MethodMaximal occupation of a state (2 for non-spin-polarized electrons, 1 otherwise).

`DFTK.find_equivalent_kpt`

— MethodFind the equivalent index of the coordinate `kcoord`

∈ ℝ³ in a list `kcoords`

∈ [-½, ½)³. `ΔG`

is the vector of ℤ³ such that `kcoords[index] = kcoord + ΔG`

.

`DFTK.gather_kpts`

— MethodGather the distributed data of a quantity depending on `k`

-Points on the master process and return it. On the other (non-master) processes `nothing`

is returned.

`DFTK.gather_kpts`

— MethodGather the distributed $k$-point data on the master process and return it as a `PlaneWaveBasis`

. On the other (non-master) processes `nothing`

is returned. The returned object should not be used for computations and only to extract data for post-processing and serialisation to disk.

`DFTK.gaussian_valence_charge_density_fourier`

— MethodGaussian valence charge density using Abinit's coefficient table, in Fourier space.

`DFTK.guess_density`

— Function```
guess_density(basis::PlaneWaveBasis, method::DensityConstructionMethod,
magnetic_moments=[]; n_electrons=basis.model.n_electrons)
```

Build a superposition of atomic densities (SAD) guess density or a rarndom guess density.

The guess atomic densities are taken as one of the following depending on the input `method`

:

-`RandomDensity()`

: A random density, normalized to the number of electrons `basis.model.n_electrons`

. Does not support magnetic moments. -`ValenceDensityAuto()`

: A combination of the `ValenceDensityGaussian`

and `ValenceDensityPseudo`

methods where elements whose pseudopotentials provide numeric valence charge density data use them and elements without use Gaussians. -`ValenceDensityGaussian()`

: Gaussians of length specified by `atom_decay_length`

normalized for the correct number of electrons:

\[\hat{ρ}(G) = Z_{\mathrm{valence}} \exp\left(-(2π \text{length} |G|)^2\right)\]

`ValenceDensityPseudo()`

: Numerical pseudo-atomic valence charge densities from the

pseudopotentials. Will fail if one or more elements in the system has a pseudopotential that does not have valence charge density data.

When magnetic moments are provided, construct a symmetry-broken density guess. The magnetic moments should be specified in units of $μ_B$.

`DFTK.hamiltonian_with_total_potential`

— MethodReturns a new Hamiltonian with local potential replaced by the given one

`DFTK.has_core_density`

— MethodCheck presence of model core charge density (non-linear core correction).

`DFTK.index_G_vectors`

— MethodReturn the index tuple `I`

such that `G_vectors(basis)[I] == G`

or the index `i`

such that `G_vectors(basis, kpoint)[i] == G`

. Returns nothing if outside the range of valid wave vectors.

`DFTK.interpolate_density`

— MethodInterpolate a function expressed in a basis `basis_in`

to a basis `basis_out`

. This interpolation uses a very basic real-space algorithm, and makes a DWIM-y attempt to take into account the fact that `basis_out`

can be a supercell of `basis_in`

.

`DFTK.interpolate_kpoint`

— MethodInterpolate some data from one $k$-point to another. The interpolation is fast, but not necessarily exact. Intended only to construct guesses for iterative solvers.

`DFTK.irfft`

— MethodPerform a real valued iFFT; see `ifft`

.

`DFTK.is_metal`

— Method`is_metal(eigenvalues, εF; tol)`

Determine whether the provided bands indicate the material is a metal, i.e. where bands are cut by the Fermi level.

`DFTK.k_to_kpq_mapping`

— MethodReturn the indices of the `kpoints`

shifted by `q`

. That is for each `kpoint`

of the `basis`

: `kpoints[ik].coordinate + q = kpoints[indices[ik]].coordinate`

.

`DFTK.kgrid_from_minimal_n_kpoints`

— MethodSelects a kgrid size which ensures that at least a `n_kpoints`

total number of $k$-points are used. The distribution of $k$-points amongst coordinate directions is as uniformly as possible, trying to achieve an identical minimal spacing in all directions.

`DFTK.kgrid_from_minimal_spacing`

— MethodSelects a kgrid size to ensure a minimal spacing (in inverse Bohrs) between kpoints. A reasonable spacing is `0.13`

inverse Bohrs (around $2π * 0.04 \AA^{-1}$).

`DFTK.kgrid_monkhorst_pack`

— MethodConstruct the coordinates of the $k$-points in a (shifted) Monkorst-Pack grid

`DFTK.kpath_get_kcoords`

— MethodReturn kpoint coordinates in reduced coordinates

`DFTK.krange_spin`

— MethodReturn the index range of $k$-points that have a particular spin component.

`DFTK.list_psp`

— Function`list_psp(element; functional, family, core, datadir_psp)`

List the pseudopotential files known to DFTK. Allows various ways to restrict the displayed files.

**Examples**

`julia> list_psp(family="hgh")`

will list all HGH-type pseudopotentials and

`julia> list_psp(family="hgh", functional="lda")`

will only list those for LDA (also known as Pade in this context) and

`julia> list_psp(:O, core=:semicore)`

will list all oxygen semicore pseudopotentials known to DFTK.

`DFTK.load_psp`

— MethodLoad a pseudopotential file from the library of pseudopotentials. The file is searched in the directory `datadir_psp()`

and by the `key`

. If the `key`

is a path to a valid file, the extension is used to determine the type of the pseudopotential file format and a respective class is returned.

`DFTK.load_scfres`

— Function`load_scfres(filename)`

Load back an `scfres`

, which has previously been stored with `save_scfres`

. Note the warning in `save_scfres`

.

`DFTK.model_DFT`

— MethodBuild a DFT model from the specified atoms, with the specified functionals.

`DFTK.model_LDA`

— MethodBuild an LDA model (Perdew & Wang parametrization) from the specified atoms. DOI:10.1103/PhysRevB.45.13244

`DFTK.model_PBE`

— MethodBuild an PBE-GGA model from the specified atoms. DOI:10.1103/PhysRevLett.77.3865

`DFTK.model_SCAN`

— MethodBuild a SCAN meta-GGA model from the specified atoms. DOI:10.1103/PhysRevLett.115.036402

`DFTK.model_atomic`

— MethodConvenience constructor, which builds a standard atomic (kinetic + atomic potential) model. Use `extra_terms`

to add additional terms.

`DFTK.mpi_nprocs`

— FunctionNumber of processors used in MPI. Can be called without ensuring initialization.

`DFTK.multiply_by_expiqr`

— MethodReturn the Fourier coefficients for `ψk · e^{i q·r}`

in the basis of `kpt_out`

, where `ψk`

is defined on a basis `kpt_in`

.

`DFTK.n_elec_core`

— MethodReturn the number of core electrons

`DFTK.n_elec_valence`

— MethodReturn the number of valence electrons

`DFTK.n_electrons_from_atoms`

— MethodNumber of valence electrons.

`DFTK.newton`

— Method```
newton(basis::PlaneWaveBasis{T}, ψ0;
tol=1e-6, tol_cg=tol / 100, maxiter=20, callback=ScfDefaultCallback(),
is_converged=ScfConvergenceDensity(tol))
```

Newton algorithm. Be careful that the starting point needs to be not too far from the solution.

`DFTK.next_compatible_fft_size`

— MethodFind the next compatible FFT size Sizes must (a) be a product of small primes only and (b) contain the factors. If smallprimes is empty (a) is skipped.

`DFTK.next_density`

— FunctionObtain new density ρ by diagonalizing `ham`

. Follows the policy imposed by the `bands`

data structure to determine and adjust the number of bands to be computed.

`DFTK.norm2`

— MethodSquare of the ℓ²-norm.

`DFTK.norm_cplx`

— MethodComplex-analytic extension of `LinearAlgebra.norm(x)`

from real to complex inputs. Needed for phonons as we want to perform a matrix-vector product `f'(x)·h`

, where `f`

is a real-to-real function and `h`

a complex vector. To do this using automatic differentiation, we can extend analytically f to accept complex inputs, then differentiate `t -> f(x+t·h)`

. This will fail if non-analytic functions like norm are used for complex inputs, and therefore we have to redefine it.

`DFTK.normalize_kpoint_coordinate`

— MethodBring $k$-point coordinates into the range [-0.5, 0.5)

`DFTK.overlap_Mmn_k_kpb`

— MethodComputes the matrix $[M^{k,b}]_{m,n} = \langle u_{m,k} | u_{n,k+b} \rangle$ for given `k`

, `kpb`

= $k+b$.

`G_shift`

is the "shifting" vector, correction due to the periodicity conditions imposed on $k \to ψ_k$. It is non zero if `kpb`

is taken in another unit cell of the reciprocal lattice. We use here that: $u_{n(k + G_{\rm shift})}(r) = e^{-i*\langle G_{\rm shift},r \rangle} u_{nk}$.

`DFTK.plot_bandstructure`

— FunctionCompute and plot the band structure. `n_bands`

selects the number of bands to compute. If this value is absent and an `scfres`

is used to start the calculation a default of `n_bands_scf + 5sqrt(n_bands_scf)`

is used. The unit used to plot the bands can be selected using the `unit`

parameter. Like in the rest of DFTK Hartree is used by default. Another standard choices is `unit=u"eV"`

(electron volts). The `kline_density`

is given in number of $k$-points per inverse bohrs (i.e. overall in units of length).

`DFTK.plot_dos`

— FunctionPlot the density of states over a reasonable range. Requires to load `Plots.jl`

beforehand.

`DFTK.psp_local_polynomial`

— FunctionThe local potential of a HGH pseudopotentials in reciprocal space can be brought to the form $Q(t) / (t^2 exp(t^2 / 2))$ where $t = r_\text{loc} q$ and `Q`

is a polynomial of at most degree 8. This function returns `Q`

.

`DFTK.psp_projector_polynomial`

— FunctionThe nonlocal projectors of a HGH pseudopotentials in reciprocal space can be brought to the form $Q(t) exp(-t^2 / 2)$ where $t = r_l q$ and `Q`

is a polynomial. This function returns `Q`

.

`DFTK.qcut_psp_local`

— MethodEstimate an upper bound for the argument `q`

after which `abs(eval_psp_local_fourier(psp, q))`

is a strictly decreasing function.

`DFTK.qcut_psp_projector`

— MethodEstimate an upper bound for the argument `q`

after which `eval_psp_projector_fourier(psp, q)`

is a strictly decreasing function.

`DFTK.r_vectors`

— Method`r_vectors(basis::PlaneWaveBasis)`

The list of $r$ vectors, in reduced coordinates. By convention, this is in [0,1)^3.

`DFTK.r_vectors_cart`

— Method`r_vectors_cart(basis::PlaneWaveBasis)`

The list of $r$ vectors, in cartesian coordinates.

`DFTK.random_density`

— MethodBuild a random charge density normalized to the provided number of electrons.

`DFTK.read_w90_nnkp`

— MethodRead the .nnkp file provided by the preprocessing routine of Wannier90 (i.e. "wannier90.x -pp prefix") Returns:

- the array 'nnkpts' of k points, their respective nearest neighbors and associated shifing vectors (non zero if the neighbor is located in another cell).
- the number 'nntot' of neighbors per k point.

TODO: add the possibility to exclude bands

`DFTK.run_wannier90`

— FunctionWannerize the obtained bands using wannier90. By default all converged bands from the `scfres`

are employed (change with `n_bands`

kwargs) and `n_wannier = n_bands`

wannier functions are computed using random Gaussians as guesses. All keyword arguments supported by Wannier90 for the disentanglement may be added as keyword arguments. The function returns the `fileprefix`

.

Currently this is an experimental feature, which has not yet been tested to full depth. The interface is considered unstable and may change incompatibly in the future. Use at your own risk and please report bugs in case you encounter any.

`DFTK.save_scfres`

— Method`save_scfres(filename, scfres)`

Save an `scfres`

obtained from `self_consistent_field`

to a file. The format is determined from the file extension. Currently the following file extensions are recognized and supported:

**jld2**: A JLD2 file. Stores the complete state and can be used (with`load_scfres`

) to restart an SCF from a checkpoint or post-process an SCF solution. See Saving SCF results on disk and SCF checkpoints for details.**vts**: A VTK file for visualisation e.g. in paraview. Stores the density, spin density and some metadata (energy, Fermi level, occupation etc.). Supports these keyword arguments:`save_ψ`

: Save the real-space representation of the orbitals as well (may lead to larger files).`extra_data`

:`Dict{String,Array}`

with additional data on the 3D real-space grid to store into the VTK file.

No guarantees are made with respect to this function at this point. It may change incompatibly between DFTK versions or stop working / be removed in the future.

`DFTK.scf_anderson_solver`

— FunctionCreate a simple anderson-accelerated SCF solver. `m`

specifies the number of steps to keep the history of.

`DFTK.scf_damping_quadratic_model`

— MethodUse the two iteration states `info`

and `info_next`

to find a damping value from a quadratic model for the SCF energy. Returns `nothing`

if the constructed model is not considered trustworthy, else returns the suggested damping.

`DFTK.scf_damping_solver`

— FunctionCreate a damped SCF solver updating the density as `x = β * x_new + (1 - β) * x`

`DFTK.select_eigenpairs_all_kblocks`

— MethodFunction to select a subset of eigenpairs on each $k$-Point. Works on the Tuple returned by `diagonalize_all_kblocks`

.

`DFTK.self_consistent_field`

— Method`self_consistent_field(basis; [tol, mixing, damping, ρ, ψ])`

Solve the Kohn-Sham equations with a density-based SCF algorithm using damped, preconditioned iterations where $ρ_\text{next} = α P^{-1} (ρ_\text{out} - ρ_\text{in})$.

Overview of parameters:

`ρ`

: Initial density`ψ`

: Initial orbitals`tol`

: Tolerance for the density change ($\|ρ_\text{out} - ρ_\text{in}\|$) to flag convergence. Default is`1e-6`

.`is_converged`

: Convergence control callback. Typical objects passed here are`DFTK.ScfConvergenceDensity(tol)`

(the default),`DFTK.ScfConvergenceEnergy(tol)`

or`DFTK.ScfConvergenceForce(tol)`

.`maxiter`

: Maximal number of SCF iterations`mixing`

: Mixing method, which determines the preconditioner $P^{-1}$ in the above equation. Typical mixings are`LdosMixing`

,`KerkerMixing`

,`SimpleMixing`

or`DielectricMixing`

. Default is`LdosMixing()`

`damping`

: Damping parameter $α$ in the above equation. Default is`0.8`

.`nbandsalg`

: By default DFTK uses`nbandsalg=AdaptiveBands(model)`

, which adaptively determines the number of bands to compute. If you want to influence this algorithm or use a predefined number of bands in each SCF step, pass a`FixedBands`

or`AdaptiveBands`

.`callback`

: Function called at each SCF iteration. Usually takes care of printing the intermediate state.

`DFTK.sin2pi`

— MethodFunction to compute sin(2π x)

`DFTK.solve_ΩplusK`

— Method```
solve_ΩplusK(basis::PlaneWaveBasis{T}, ψ, res, occupation;
tol=1e-10, verbose=false) where {T}
```

Return δψ where (Ω+K) δψ = rhs

`DFTK.solve_ΩplusK_split`

— MethodSolve the problem `(Ω+K) δψ = rhs`

using a split algorithm, where `rhs`

is typically `-δHextψ`

(the negative matvec of an external perturbation with the SCF orbitals `ψ`

) and `δψ`

is the corresponding total variation in the orbitals `ψ`

. Additionally returns: - `δρ`

: Total variation in density) - `δHψ`

: Total variation in Hamiltonian applied to orbitals - `δeigenvalues`

: Total variation in eigenvalues - `δVind`

: Change in potential induced by `δρ`

(the term needed on top of `δHextψ`

to get `δHψ`

).

`DFTK.spglib_atoms`

— MethodConvert the DFTK atom groups and positions datastructure into a tuple of datastructures for use with spglib. Validity of the input data is assumed. The output `positions`

contains positions per atom, `numbers`

contains the mapping atom to a unique number for each group of indistinguishable atoms, `spins`

contains the $z$-component of the initial magnetic moment on each atom, `mapping`

contains the mapping of the `numbers`

to the element objects in DFTK and `collinear`

whether the atoms mark a case of collinear spin or not. Notice that if `collinear`

is false then `spins`

is garbage.

`DFTK.spglib_standardize_cell`

— MethodReturns crystallographic conventional cell according to the International Table of Crystallography Vol A (ITA) in case `primitive=false`

. If `primitive=true`

the primitive lattice is returned in the convention of the reference work of Cracknell, Davies, Miller, and Love (CDML). Of note this has minor differences to the primitive setting choice made in the ITA.

`DFTK.sphericalbesselj_fast`

— Method`sphericalbesselj_fast(l::Integer, x::Number)`

Returns the spherical Bessel function of the first kind j*l(x). Consistent with https://en.wikipedia.org/wiki/Bessel*function#Spherical*Bessel*functions and with `SpecialFunctions.sphericalbesselj`

. Specialized for integer `0 <= l <= 5`

.

`DFTK.spin_components`

— MethodExplicit spin components of the KS orbitals and the density

`DFTK.split_evenly`

— MethodSplit an iterable evenly into N chunks, which will be returned.

`DFTK.standardize_atoms`

— FunctionApply various standardisations to a lattice and a list of atoms. It uses spglib to detect symmetries (within `tol_symmetry`

), then cleans up the lattice according to the symmetries (unless `correct_symmetry`

is `false`

) and returns the resulting standard lattice and atoms. If `primitive`

is `true`

(default) the primitive unit cell is returned, else the conventional unit cell is returned.

`DFTK.symmetries_preserving_kgrid`

— MethodFilter out the symmetry operations that don't respect the symmetries of the discrete BZ grid

`DFTK.symmetries_preserving_rgrid`

— MethodFilter out the symmetry operations that don't respect the symmetries of the discrete real-space grid

`DFTK.symmetrize_forces`

— MethodSymmetrize the forces in *reduced coordinates*, forces given as an array forces[iel][α,i]

`DFTK.symmetrize_stresses`

— MethodSymmetrize the stress tensor, given as a Matrix in cartesian coordinates

`DFTK.symmetrize_ρ`

— MethodSymmetrize a density by applying all the basis (by default) symmetries and forming the average.

`DFTK.symmetry_operations`

— FunctionReturn the $k$-point symmetry operations associated to a lattice and atoms.

`DFTK.synchronize_device`

— MethodSynchronize data and finish all operations on the execution stream of the device. This needs to be called explicitly before a task finishes (e.g. in an `@spawn`

block).

`DFTK.to_cpu`

— MethodTransfer an array from a device (typically a GPU) to the CPU.

`DFTK.to_device`

— MethodTransfer an array to a particular device (typically a GPU)

`DFTK.total_local_potential`

— MethodGet the total local potential of the given Hamiltonian, in real space in the spin components.

`DFTK.transfer_blochwave`

— MethodTransfer Bloch wave between two basis sets. Limited feature set.

`DFTK.transfer_blochwave_kpt`

— MethodTransfer an array `ψk_in`

expanded on `kpt_in`

, and produce $ψ(r) e^{i ΔG·r}$ expanded on `kpt_out`

. It is mostly useful for phonons. Beware: `ψk_out`

can lose information if the shift `ΔG`

is large or if the `G_vectors`

differ between `k`

-points.

`DFTK.transfer_blochwave_kpt`

— MethodTransfer an array `ψk`

defined on basis*in $k$-point kpt*in to basis*out $k$-point kpt*out.

`DFTK.transfer_mapping`

— MethodCompute the index mapping between two bases. Returns two arrays `idcs_in`

and `idcs_out`

such that `ψkout[idcs_out] = ψkin[idcs_in]`

does the transfer from `ψkin`

(defined on `basis_in`

and `kpt_in`

) to `ψkout`

(defined on `basis_out`

and `kpt_out`

).

`DFTK.unfold_bz`

— Method" Convert a `basis`

into one that doesn't use BZ symmetry. This is mainly useful for debug purposes (e.g. in cases we don't want to bother thinking about symmetries).

`DFTK.weighted_ksum`

— MethodSum an array over kpoints, taking weights into account

`DFTK.write_w90_eig`

— MethodWrite the eigenvalues in a format readable by Wannier90.

`DFTK.write_w90_win`

— MethodWrite a win file at the indicated prefix. Parameters to Wannier90 can be added as kwargs: e.g. `num_iter=500`

.

`DFTK.ylm_real`

— MethodReturns the (l,m) real spherical harmonic Y*lm(r). Consistent with https://en.wikipedia.org/wiki/Table*of*spherical*harmonics#Real*spherical*harmonics

`DFTK.zeros_like`

— FunctionCreate an array of same "array type" as X filled with zeros, minimizing the number of allocations. This unifies CPU and GPU code, as the output will always be on the same device as the input.

`DFTK.@timing`

— MacroShortened version of the `@timeit`

macro from `TimerOutputs`

, which writes to the DFTK timer.

`DFTK.Smearing.A`

— Method`A`

term in the Hermite delta expansion

`DFTK.Smearing.H`

— MethodStandard Hermite function using physicist's convention.

`DFTK.Smearing.entropy`

— MethodEntropy. Note that this is a function of the energy `x`

, not of `occupation(x)`

. This function satisfies s' = x f' (see https://www.vasp.at/vasp-workshop/k-points.pdf p. 12 and https://arxiv.org/pdf/1805.07144.pdf p. 18.

`DFTK.Smearing.occupation`

— Function`occupation(S::SmearingFunction, x)`

Occupation at `x`

, where in practice `x = (ε - εF) / temperature`

. If temperature is zero, `(ε-εF)/temperature = ±∞`

. The occupation function is required to give 1 and 0 respectively in these cases.

`DFTK.Smearing.occupation_derivative`

— MethodDerivative of the occupation function, approximation to minus the delta function.

`DFTK.Smearing.occupation_divided_difference`

— Method(f(x) - f(y))/(x - y), computed stably in the case where x and y are close