File: attenuation.mpl

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(*
 Copyright (C) 2017 M.A.L. Marques
               2020-2021 Susi Lehtola

 This Source Code Form is subject to the terms of the Mozilla Public
 License, v. 2.0. If a copy of the MPL was not distributed with this
 file, You can obtain one at http://mozilla.org/MPL/2.0/.
*)

(* NOTE: the implementations in this file are for short-range exchange functionals.
   The naming merely implicates which type of kernel is used.
*)

(* error function:
    Toulouse et al, Int. J. Quantum Chem. 100, 1047 (2004); doi:10.1002/qua.20259
    Tawada et al, J. Chem. Phys. 120, 8425 (2004); doi:10.1063/1.1688752

    The implementation follows Tawada et al.
*)
att_erf_aux1 := a -> sqrt(Pi)*erf(1/(2*a)):
att_erf_aux2 := a -> exp(-1/(4*a^2)) - 1:
att_erf_aux3 := a -> 2*a^2*att_erf_aux2(a) + 1/2:
(* This is the full function, which is numerically unstable for large a *)
attenuation_erf0 := a ->
  1 - 8/3*a*(att_erf_aux1(a) + 2*a*(att_erf_aux2(a) - att_erf_aux3(a))):
(* The cutoff and order are determined by check_attenuation.mpl *)
attenuation_erf := a -> enforce_smooth_lr(attenuation_erf0, a, 1.35, 16):

(* These are for hyb_mgga_x_js18 and hyb_mgga_x_pjs18. This is the
bracket in eqn (10) in Patra et al, 2018 *)
attenuation_erf_f20 := a ->
  1 + 24*a^2*( (20*a^2 - 64*a^4)*exp(-1/(4*a^2))
    - 3 - 36*a^2 + 64*a^4
    + 10*a*sqrt(Pi)*erf(1/(2*a))):
(* The cutoff and order are determined by check_attenuation.mpl *)
attenuation_erf_f2 := a -> enforce_smooth_lr(attenuation_erf_f20, a, 0.27, 46):

(* This is eqn (11) in Patra et al, 2018  *)
attenuation_erf_f30 := a ->
  1 + 8/7*a*(
        (-8*a + 256*a^3 - 576*a^5 + 3840*a^7 - 122880*a^9)*exp(-1/(4*a^2))
      + 24*a^3*(-35 + 224*a^2 - 1440*a^4 + 5120*a^6)
      + 2*sqrt(Pi)*(-2 + 60*a^2)*erf(1/(2*a))):
(* The cutoff and order are determined by check_attenuation.mpl *)
attenuation_erf_f3 := a -> enforce_smooth_lr(attenuation_erf_f30, a, 0.32, 38):

(* erf_gau - screening function = + 2 mu/sqrt(pi) exp(-mu^2 r^2)
    Song et al, J. Chem. Phys. 127, 154109 (2007); doi:10.1063/1.2790017
    You can recover the result in Int. J. Quantum Chem. 100, 1047 (2004)
    by putting a = a/sqrt(3) and multiplying the whole attenuation function by -sqrt(3)
*)
attenuation_gau0 := a -> -8/3*a*(att_erf_aux1(a) + 2*a*att_erf_aux2(a)*(1 - 8*a^2) - 4*a):
(* The cutoff and order are determined by check_attenuation.mpl *)
attenuation_gau := a -> enforce_smooth_lr(attenuation_gau0, a, 2.07, 14):

(* yukawa
    Akinaga and Ten-no, Chem. Phys. Lett. 462, 348 (2008); doi:10.1016/j.cplett.2008.07.103
*)
att_yuk_aux1 := a -> arctan(1, a):
att_yuk_aux2 := a -> log(1 + 1/a^2):
att_yuk_aux3 := a -> a^2 + 1:
attenuation_yukawa0 := a -> 1 - 8/3*a*(att_yuk_aux1(a) + a/4*(1 - (att_yuk_aux3(a) + 2)*att_yuk_aux2(a))):
(* The cutoff and order are determined by check_attenuation.mpl *)
attenuation_yukawa := a -> enforce_smooth_lr(attenuation_yukawa0, a, 1.92, 36):