9
1
mirror of https://github.com/QuantumPackage/qp2.git synced 2024-12-21 11:03:29 +01:00
qp2/src/ao_one_e_ints/pot_ao_erf_ints.irp.f

795 lines
26 KiB
Fortran
Raw Normal View History

2023-03-04 17:49:48 +01:00
! ---
2019-01-25 11:39:31 +01:00
subroutine give_all_erf_kl_ao(integrals_ao,mu_in,C_center)
implicit none
BEGIN_DOC
! Subroutine that returns all integrals over $r$ of type
2019-01-29 15:40:00 +01:00
! $\frac{ \erf(\mu * | r - R_C | ) }{ | r - R_C | }$
2019-01-25 11:39:31 +01:00
END_DOC
double precision, intent(in) :: mu_in,C_center(3)
double precision, intent(out) :: integrals_ao(ao_num,ao_num)
double precision :: NAI_pol_mult_erf_ao
integer :: i,j,l,k,m
do k = 1, ao_num
do m = 1, ao_num
integrals_ao(m,k) = NAI_pol_mult_erf_ao(m,k,mu_in,C_center)
enddo
enddo
end
2023-03-04 17:49:48 +01:00
! ---
double precision function NAI_pol_mult_erf_ao(i_ao, j_ao, mu_in, C_center)
2019-01-25 11:39:31 +01:00
BEGIN_DOC
2023-03-04 17:49:48 +01:00
!
2019-01-25 11:39:31 +01:00
! Computes the following integral :
2023-03-04 17:49:48 +01:00
! $\int_{-\infty}^{infty} dr \chi_i(r) \chi_j(r) \frac{\erf(\mu |r - R_C|)}{|r - R_C|}$.
!
2019-01-25 11:39:31 +01:00
END_DOC
2023-03-04 17:49:48 +01:00
implicit none
integer, intent(in) :: i_ao, j_ao
2019-01-25 11:39:31 +01:00
double precision, intent(in) :: mu_in, C_center(3)
2023-03-04 17:49:48 +01:00
integer :: i, j, num_A, num_B, power_A(3), power_B(3), n_pt_in
double precision :: A_center(3), B_center(3), integral, alpha, beta
2019-01-25 11:39:31 +01:00
double precision :: NAI_pol_mult_erf
2023-03-04 17:49:48 +01:00
num_A = ao_nucl(i_ao)
power_A(1:3) = ao_power(i_ao,1:3)
2019-01-25 11:39:31 +01:00
A_center(1:3) = nucl_coord(num_A,1:3)
2023-03-04 17:49:48 +01:00
num_B = ao_nucl(j_ao)
power_B(1:3) = ao_power(j_ao,1:3)
2019-01-25 11:39:31 +01:00
B_center(1:3) = nucl_coord(num_B,1:3)
2023-03-04 17:49:48 +01:00
2019-01-25 11:39:31 +01:00
n_pt_in = n_pt_max_integrals
2023-03-04 17:49:48 +01:00
2019-01-25 11:39:31 +01:00
NAI_pol_mult_erf_ao = 0.d0
do i = 1, ao_prim_num(i_ao)
alpha = ao_expo_ordered_transp(i,i_ao)
do j = 1, ao_prim_num(j_ao)
beta = ao_expo_ordered_transp(j,j_ao)
2023-03-04 17:49:48 +01:00
integral = NAI_pol_mult_erf(A_center, B_center, power_A, power_B, alpha, beta, C_center, n_pt_in,mu_in)
NAI_pol_mult_erf_ao += integral * ao_coef_normalized_ordered_transp(j,j_ao) * ao_coef_normalized_ordered_transp(i,i_ao)
2019-01-25 11:39:31 +01:00
enddo
enddo
2023-03-04 17:49:48 +01:00
end function NAI_pol_mult_erf_ao
! ---
double precision function NAI_pol_mult_erf_ao_with1s(i_ao, j_ao, beta, B_center, mu_in, C_center)
BEGIN_DOC
!
! Computes the following integral :
! $\int_{-\infty}^{infty} dr \chi_i(r) \chi_j(r) e^{-\beta (r - B_center)^2} \frac{\erf(\mu |r - R_C|)}{|r - R_C|}$.
!
END_DOC
implicit none
integer, intent(in) :: i_ao, j_ao
double precision, intent(in) :: beta, B_center(3)
double precision, intent(in) :: mu_in, C_center(3)
integer :: i, j, power_A1(3), power_A2(3), n_pt_in
double precision :: A1_center(3), A2_center(3), alpha1, alpha2, coef12, coef1, integral
double precision, external :: NAI_pol_mult_erf_with1s, NAI_pol_mult_erf_ao
ASSERT(beta .ge. 0.d0)
if(beta .lt. 1d-10) then
NAI_pol_mult_erf_ao_with1s = NAI_pol_mult_erf_ao(i_ao, j_ao, mu_in, C_center)
return
endif
power_A1(1:3) = ao_power(i_ao,1:3)
power_A2(1:3) = ao_power(j_ao,1:3)
A1_center(1:3) = nucl_coord(ao_nucl(i_ao),1:3)
A2_center(1:3) = nucl_coord(ao_nucl(j_ao),1:3)
n_pt_in = n_pt_max_integrals
NAI_pol_mult_erf_ao_with1s = 0.d0
do i = 1, ao_prim_num(i_ao)
alpha1 = ao_expo_ordered_transp (i,i_ao)
coef1 = ao_coef_normalized_ordered_transp(i,i_ao)
do j = 1, ao_prim_num(j_ao)
alpha2 = ao_expo_ordered_transp(j,j_ao)
coef12 = coef1 * ao_coef_normalized_ordered_transp(j,j_ao)
if(dabs(coef12) .lt. 1d-14) cycle
integral = NAI_pol_mult_erf_with1s( A1_center, A2_center, power_A1, power_A2, alpha1, alpha2 &
, beta, B_center, C_center, n_pt_in, mu_in )
NAI_pol_mult_erf_ao_with1s += integral * coef12
enddo
enddo
end function NAI_pol_mult_erf_ao_with1s
! ---
2019-01-25 11:39:31 +01:00
2023-02-06 19:00:35 +01:00
double precision function NAI_pol_mult_erf(A_center, B_center, power_A, power_B, alpha, beta, C_center, n_pt_in, mu_in)
2019-01-25 11:39:31 +01:00
BEGIN_DOC
2023-02-06 19:00:35 +01:00
!
2019-01-25 11:39:31 +01:00
! Computes the following integral :
2019-01-29 15:40:00 +01:00
!
! .. math::
2023-02-06 19:00:35 +01:00
!
2019-01-29 15:40:00 +01:00
! \int dr (x-A_x)^a (x-B_x)^b \exp(-\alpha (x-A_x)^2 - \beta (x-B_x)^2 )
2023-02-06 19:00:35 +01:00
! \frac{\erf(\mu |r - R_C |)}{| r - R_C |}$.
2019-01-29 15:40:00 +01:00
!
2019-01-25 11:39:31 +01:00
END_DOC
include 'utils/constants.include.F'
2023-02-06 19:00:35 +01:00
implicit none
integer, intent(in) :: n_pt_in
integer, intent(in) :: power_A(3), power_B(3)
double precision, intent(in) :: C_center(3), A_center(3), B_center(3), alpha, beta, mu_in
integer :: i, n_pt, n_pt_out
double precision :: P_center(3)
double precision :: d(0:n_pt_in), coeff, dist, const, factor
double precision :: const_factor, dist_integral
double precision :: accu, p_inv, p, rho, p_inv_2
double precision :: p_new
double precision :: rint
p = alpha + beta
p_inv = 1.d0 / p
2019-01-25 11:39:31 +01:00
p_inv_2 = 0.5d0 * p_inv
2023-02-06 19:00:35 +01:00
rho = alpha * beta * p_inv
2019-01-25 11:39:31 +01:00
2023-02-06 19:00:35 +01:00
dist = 0.d0
2019-01-25 11:39:31 +01:00
dist_integral = 0.d0
do i = 1, 3
2023-02-06 19:00:35 +01:00
P_center(i) = (alpha * A_center(i) + beta * B_center(i)) * p_inv
dist += (A_center(i) - B_center(i)) * (A_center(i) - B_center(i))
dist_integral += (P_center(i) - C_center(i)) * (P_center(i) - C_center(i))
2019-01-25 11:39:31 +01:00
enddo
2023-02-06 19:00:35 +01:00
const_factor = dist * rho
if(const_factor > 80.d0) then
2019-01-25 11:39:31 +01:00
NAI_pol_mult_erf = 0.d0
return
endif
2023-02-06 19:00:35 +01:00
p_new = mu_in / dsqrt(p + mu_in * mu_in)
2019-01-25 11:39:31 +01:00
factor = dexp(-const_factor)
2023-02-06 19:00:35 +01:00
coeff = dtwo_pi * factor * p_inv * p_new
2019-01-25 11:39:31 +01:00
2023-02-06 19:00:35 +01:00
n_pt = 2 * ( (power_A(1) + power_B(1)) + (power_A(2) + power_B(2)) + (power_A(3) + power_B(3)) )
2019-01-25 11:39:31 +01:00
const = p * dist_integral * p_new * p_new
2023-02-06 19:00:35 +01:00
if(n_pt == 0) then
NAI_pol_mult_erf = coeff * rint(0, const)
2019-01-25 11:39:31 +01:00
return
endif
2023-02-06 19:00:35 +01:00
do i = 0, n_pt_in
d(i) = 0.d0
enddo
2019-01-25 11:39:31 +01:00
! call give_polynomial_mult_center_one_e_erf(A_center,B_center,alpha,beta,power_A,power_B,C_center,n_pt_in,d,n_pt_out,mu_in)
p_new = p_new * p_new
2023-02-06 19:00:35 +01:00
call give_polynomial_mult_center_one_e_erf_opt(A_center, B_center, power_A, power_B, C_center, n_pt_in, d, n_pt_out, p_inv_2, p_new, P_center)
2019-01-25 11:39:31 +01:00
2023-02-06 19:00:35 +01:00
if(n_pt_out < 0) then
2019-01-25 11:39:31 +01:00
NAI_pol_mult_erf = 0.d0
return
endif
! sum of integrals of type : int {t,[0,1]} exp-(rho.(P-Q)^2 * t^2) * t^i
2023-02-06 19:00:35 +01:00
accu = 0.d0
do i = 0, n_pt_out, 2
accu += d(i) * rint(i/2, const)
2019-01-25 11:39:31 +01:00
enddo
NAI_pol_mult_erf = accu * coeff
2023-02-06 19:00:35 +01:00
end function NAI_pol_mult_erf
2019-01-25 11:39:31 +01:00
2023-02-06 19:00:35 +01:00
! ---
2023-03-04 17:49:48 +01:00
subroutine NAI_pol_mult_erf_v(A_center, B_center, power_A, power_B, alpha, beta, C_center, LD_C, n_pt_in, mu_in, res_v, LD_resv, n_points)
2023-02-06 19:00:35 +01:00
BEGIN_DOC
!
! Computes the following integral :
2023-03-04 17:49:48 +01:00
!
! .. math::
!
! \int dr (x-A_x)^a (x-B_x)^b \exp(-\alpha (x-A_x)^2 - \beta (x-B_x)^2 )
! \frac{\erf(\mu |r - R_C |)}{| r - R_C |}$.
2023-02-06 19:00:35 +01:00
!
END_DOC
2023-03-04 17:49:48 +01:00
include 'utils/constants.include.F'
2023-02-06 19:00:35 +01:00
implicit none
2023-03-04 17:49:48 +01:00
integer, intent(in) :: n_pt_in, n_points, LD_C, LD_resv
integer, intent(in) :: power_A(3), power_B(3)
double precision, intent(in) :: A_center(3), B_center(3), alpha, beta, mu_in
double precision, intent(in) :: C_center(LD_C,3)
double precision, intent(out) :: res_v(LD_resv)
2023-02-06 19:00:35 +01:00
2023-03-04 17:49:48 +01:00
integer :: i, n_pt, n_pt_out, ipoint
double precision :: P_center(3)
double precision :: d(0:n_pt_in), coeff, dist, const, factor
double precision :: const_factor, dist_integral
double precision :: accu, p_inv, p, rho, p_inv_2
double precision :: p_new, p_new2, coef_tmp
2023-02-06 19:00:35 +01:00
2023-03-04 17:49:48 +01:00
double precision :: rint
res_V(1:LD_resv) = 0.d0
p = alpha + beta
p_inv = 1.d0 / p
p_inv_2 = 0.5d0 * p_inv
rho = alpha * beta * p_inv
p_new = mu_in / dsqrt(p + mu_in * mu_in)
p_new2 = p_new * p_new
coef_tmp = p * p_new2
dist = 0.d0
do i = 1, 3
P_center(i) = (alpha * A_center(i) + beta * B_center(i)) * p_inv
dist += (A_center(i) - B_center(i)) * (A_center(i) - B_center(i))
enddo
const_factor = dist * rho
if(const_factor > 80.d0) then
2023-02-06 19:00:35 +01:00
return
endif
2023-03-04 17:49:48 +01:00
factor = dexp(-const_factor)
coeff = dtwo_pi * factor * p_inv * p_new
2023-02-06 19:00:35 +01:00
2023-03-04 17:49:48 +01:00
n_pt = 2 * ( power_A(1) + power_B(1) + power_A(2) + power_B(2) + power_A(3) + power_B(3) )
2023-02-06 19:00:35 +01:00
2023-03-04 17:49:48 +01:00
if(n_pt == 0) then
2023-02-06 19:00:35 +01:00
2023-03-04 17:49:48 +01:00
do ipoint = 1, n_points
dist_integral = 0.d0
do i = 1, 3
dist_integral += (P_center(i) - C_center(ipoint,i)) * (P_center(i) - C_center(ipoint,i))
enddo
const = coef_tmp * dist_integral
2023-02-06 19:00:35 +01:00
2023-03-04 17:49:48 +01:00
res_v(ipoint) = coeff * rint(0, const)
enddo
2023-02-06 19:00:35 +01:00
2023-03-04 17:49:48 +01:00
else
2023-02-06 19:00:35 +01:00
2023-03-04 17:49:48 +01:00
do ipoint = 1, n_points
dist_integral = 0.d0
do i = 1, 3
dist_integral += (P_center(i) - C_center(ipoint,i)) * (P_center(i) - C_center(ipoint,i))
enddo
const = coef_tmp * dist_integral
2023-02-06 19:00:35 +01:00
2023-03-04 17:49:48 +01:00
do i = 0, n_pt_in
d(i) = 0.d0
enddo
call give_polynomial_mult_center_one_e_erf_opt(A_center, B_center, power_A, power_B, C_center(ipoint,1:3), n_pt_in, d, n_pt_out, p_inv_2, p_new2, P_center)
if(n_pt_out < 0) then
res_v(ipoint) = 0.d0
cycle
endif
! sum of integrals of type : int {t,[0,1]} exp-(rho.(P-Q)^2 * t^2) * t^i
accu = 0.d0
do i = 0, n_pt_out, 2
accu += d(i) * rint(i/2, const)
enddo
res_v(ipoint) = accu * coeff
2023-02-06 19:00:35 +01:00
enddo
2023-03-04 17:49:48 +01:00
endif
end subroutine NAI_pol_mult_erf_v
! ---
double precision function NAI_pol_mult_erf_with1s( A1_center, A2_center, power_A1, power_A2, alpha1, alpha2 &
, beta, B_center, C_center, n_pt_in, mu_in )
BEGIN_DOC
!
! Computes the following integral :
!
! .. math::
!
! \int dx (x - A1_x)^a_1 (x - B1_x)^a_2 \exp(-\alpha_1 (x - A1_x)^2 - \alpha_2 (x - A2_x)^2)
! \int dy (y - A1_y)^b_1 (y - B1_y)^b_2 \exp(-\alpha_1 (y - A1_y)^2 - \alpha_2 (y - A2_y)^2)
! \int dz (x - A1_z)^c_1 (z - B1_z)^c_2 \exp(-\alpha_1 (z - A1_z)^2 - \alpha_2 (z - A2_z)^2)
! \exp(-\beta (r - B)^2)
! \frac{\erf(\mu |r - R_C|)}{|r - R_C|}$.
!
END_DOC
include 'utils/constants.include.F'
implicit none
integer, intent(in) :: n_pt_in
integer, intent(in) :: power_A1(3), power_A2(3)
double precision, intent(in) :: C_center(3), A1_center(3), A2_center(3), B_center(3)
double precision, intent(in) :: alpha1, alpha2, beta, mu_in
integer :: i, n_pt, n_pt_out
double precision :: alpha12, alpha12_inv, alpha12_inv_2, rho12, A12_center(3), dist12, const_factor12
double precision :: p, p_inv, p_inv_2, rho, P_center(3), dist, const_factor
double precision :: dist_integral
double precision :: d(0:n_pt_in), coeff, const, factor
double precision :: accu
double precision :: p_new
double precision :: rint
! e^{-alpha1 (r - A1)^2} e^{-alpha2 (r - A2)^2} = e^{-K12} e^{-alpha12 (r - A12)^2}
alpha12 = alpha1 + alpha2
alpha12_inv = 1.d0 / alpha12
alpha12_inv_2 = 0.5d0 * alpha12_inv
rho12 = alpha1 * alpha2 * alpha12_inv
A12_center(1) = (alpha1 * A1_center(1) + alpha2 * A2_center(1)) * alpha12_inv
A12_center(2) = (alpha1 * A1_center(2) + alpha2 * A2_center(2)) * alpha12_inv
A12_center(3) = (alpha1 * A1_center(3) + alpha2 * A2_center(3)) * alpha12_inv
dist12 = (A1_center(1) - A2_center(1)) * (A1_center(1) - A2_center(1)) &
+ (A1_center(2) - A2_center(2)) * (A1_center(2) - A2_center(2)) &
+ (A1_center(3) - A2_center(3)) * (A1_center(3) - A2_center(3))
const_factor12 = dist12 * rho12
if(const_factor12 > 80.d0) then
NAI_pol_mult_erf_with1s = 0.d0
return
endif
! ---
! e^{-K12} e^{-alpha12 (r - A12)^2} e^{-beta (r - B)^2} = e^{-K} e^{-p (r - P)^2}
p = alpha12 + beta
p_inv = 1.d0 / p
p_inv_2 = 0.5d0 * p_inv
rho = alpha12 * beta * p_inv
P_center(1) = (alpha12 * A12_center(1) + beta * B_center(1)) * p_inv
P_center(2) = (alpha12 * A12_center(2) + beta * B_center(2)) * p_inv
P_center(3) = (alpha12 * A12_center(3) + beta * B_center(3)) * p_inv
dist = (A12_center(1) - B_center(1)) * (A12_center(1) - B_center(1)) &
+ (A12_center(2) - B_center(2)) * (A12_center(2) - B_center(2)) &
+ (A12_center(3) - B_center(3)) * (A12_center(3) - B_center(3))
const_factor = const_factor12 + dist * rho
if(const_factor > 80.d0) then
NAI_pol_mult_erf_with1s = 0.d0
return
endif
dist_integral = (P_center(1) - C_center(1)) * (P_center(1) - C_center(1)) &
+ (P_center(2) - C_center(2)) * (P_center(2) - C_center(2)) &
+ (P_center(3) - C_center(3)) * (P_center(3) - C_center(3))
! ---
p_new = mu_in / dsqrt(p + mu_in * mu_in)
factor = dexp(-const_factor)
coeff = dtwo_pi * factor * p_inv * p_new
n_pt = 2 * ( (power_A1(1) + power_A2(1)) + (power_A1(2) + power_A2(2)) + (power_A1(3) + power_A2(3)) )
const = p * dist_integral * p_new * p_new
if(n_pt == 0) then
NAI_pol_mult_erf_with1s = coeff * rint(0, const)
return
endif
do i = 0, n_pt_in
d(i) = 0.d0
2023-02-06 19:00:35 +01:00
enddo
2023-03-04 17:49:48 +01:00
p_new = p_new * p_new
call give_polynomial_mult_center_one_e_erf_opt( A1_center, A2_center, power_A1, power_A2, C_center, n_pt_in, d, n_pt_out, p_inv_2, p_new, P_center)
2023-02-06 19:00:35 +01:00
2023-03-04 17:49:48 +01:00
if(n_pt_out < 0) then
NAI_pol_mult_erf_with1s = 0.d0
return
endif
! sum of integrals of type : int {t,[0,1]} exp-(rho.(P-Q)^2 * t^2) * t^i
accu = 0.d0
do i = 0, n_pt_out, 2
accu += d(i) * rint(i/2, const)
enddo
NAI_pol_mult_erf_with1s = accu * coeff
end function NAI_pol_mult_erf_with1s
! ---
2023-02-06 19:00:35 +01:00
subroutine NAI_pol_mult_erf_with1s_v(A1_center, A2_center, power_A1, power_A2, alpha1, alpha2, beta, B_center, LD_B, C_center, LD_C, n_pt_in, mu_in, res_v, LD_resv, n_points)
BEGIN_DOC
!
! Computes the following integral :
!
! .. math ::
!
! \int dx (x - A1_x)^a_1 (x - B1_x)^a_2 \exp(-\alpha_1 (x - A1_x)^2 - \alpha_2 (x - A2_x)^2)
! \int dy (y - A1_y)^b_1 (y - B1_y)^b_2 \exp(-\alpha_1 (y - A1_y)^2 - \alpha_2 (y - A2_y)^2)
! \int dz (x - A1_z)^c_1 (z - B1_z)^c_2 \exp(-\alpha_1 (z - A1_z)^2 - \alpha_2 (z - A2_z)^2)
! \exp(-\beta (r - B)^2)
! \frac{\erf(\mu |r - R_C|)}{|r - R_C|}$.
!
END_DOC
include 'utils/constants.include.F'
implicit none
integer, intent(in) :: n_pt_in, LD_B, LD_C, LD_resv, n_points
integer, intent(in) :: power_A1(3), power_A2(3)
double precision, intent(in) :: A1_center(3), A2_center(3)
double precision, intent(in) :: C_center(LD_C,3), B_center(LD_B,3)
double precision, intent(in) :: alpha1, alpha2, beta, mu_in
double precision, intent(out) :: res_v(LD_resv)
integer :: i, n_pt, n_pt_out, ipoint
double precision :: alpha12, alpha12_inv, alpha12_inv_2, rho12, A12_center(3), dist12, const_factor12
double precision :: p, p_inv, p_inv_2, rho, P_center(3), dist, const_factor
double precision :: dist_integral
double precision :: d(0:n_pt_in), coeff, const, factor
double precision :: accu
double precision :: p_new, p_new2, coef_tmp, cons_tmp
double precision :: rint
res_V(1:LD_resv) = 0.d0
! e^{-alpha1 (r - A1)^2} e^{-alpha2 (r - A2)^2} = e^{-K12} e^{-alpha12 (r - A12)^2}
alpha12 = alpha1 + alpha2
alpha12_inv = 1.d0 / alpha12
alpha12_inv_2 = 0.5d0 * alpha12_inv
rho12 = alpha1 * alpha2 * alpha12_inv
A12_center(1) = (alpha1 * A1_center(1) + alpha2 * A2_center(1)) * alpha12_inv
A12_center(2) = (alpha1 * A1_center(2) + alpha2 * A2_center(2)) * alpha12_inv
A12_center(3) = (alpha1 * A1_center(3) + alpha2 * A2_center(3)) * alpha12_inv
dist12 = (A1_center(1) - A2_center(1)) * (A1_center(1) - A2_center(1))&
+ (A1_center(2) - A2_center(2)) * (A1_center(2) - A2_center(2))&
+ (A1_center(3) - A2_center(3)) * (A1_center(3) - A2_center(3))
const_factor12 = dist12 * rho12
if(const_factor12 > 80.d0) then
return
endif
! e^{-K12} e^{-alpha12 (r - A12)^2} e^{-beta (r - B)^2} = e^{-K} e^{-p (r - P)^2}
p = alpha12 + beta
p_inv = 1.d0 / p
p_inv_2 = 0.5d0 * p_inv
rho = alpha12 * beta * p_inv
p_new = mu_in / dsqrt(p + mu_in * mu_in)
p_new2 = p_new * p_new
coef_tmp = dtwo_pi * p_inv * p_new
cons_tmp = p * p_new2
n_pt = 2 * (power_A1(1) + power_A2(1) + power_A1(2) + power_A2(2) + power_A1(3) + power_A2(3) )
if(n_pt == 0) then
do ipoint = 1, n_points
dist = (A12_center(1) - B_center(ipoint,1)) * (A12_center(1) - B_center(ipoint,1))&
+ (A12_center(2) - B_center(ipoint,2)) * (A12_center(2) - B_center(ipoint,2))&
+ (A12_center(3) - B_center(ipoint,3)) * (A12_center(3) - B_center(ipoint,3))
const_factor = const_factor12 + dist * rho
if(const_factor > 80.d0) cycle
coeff = coef_tmp * dexp(-const_factor)
P_center(1) = (alpha12 * A12_center(1) + beta * B_center(ipoint,1)) * p_inv
P_center(2) = (alpha12 * A12_center(2) + beta * B_center(ipoint,2)) * p_inv
P_center(3) = (alpha12 * A12_center(3) + beta * B_center(ipoint,3)) * p_inv
dist_integral = (P_center(1) - C_center(ipoint,1)) * (P_center(1) - C_center(ipoint,1))&
+ (P_center(2) - C_center(ipoint,2)) * (P_center(2) - C_center(ipoint,2))&
+ (P_center(3) - C_center(ipoint,3)) * (P_center(3) - C_center(ipoint,3))
const = cons_tmp * dist_integral
res_v(ipoint) = coeff * rint(0, const)
enddo
else
do ipoint = 1, n_points
dist = (A12_center(1) - B_center(ipoint,1)) * (A12_center(1) - B_center(ipoint,1))&
+ (A12_center(2) - B_center(ipoint,2)) * (A12_center(2) - B_center(ipoint,2))&
+ (A12_center(3) - B_center(ipoint,3)) * (A12_center(3) - B_center(ipoint,3))
const_factor = const_factor12 + dist * rho
if(const_factor > 80.d0) cycle
coeff = coef_tmp * dexp(-const_factor)
P_center(1) = (alpha12 * A12_center(1) + beta * B_center(ipoint,1)) * p_inv
P_center(2) = (alpha12 * A12_center(2) + beta * B_center(ipoint,2)) * p_inv
P_center(3) = (alpha12 * A12_center(3) + beta * B_center(ipoint,3)) * p_inv
dist_integral = (P_center(1) - C_center(ipoint,1)) * (P_center(1) - C_center(ipoint,1))&
+ (P_center(2) - C_center(ipoint,2)) * (P_center(2) - C_center(ipoint,2))&
+ (P_center(3) - C_center(ipoint,3)) * (P_center(3) - C_center(ipoint,3))
const = cons_tmp * dist_integral
do i = 0, n_pt_in
d(i) = 0.d0
enddo
!TODO: VECTORIZE HERE
call give_polynomial_mult_center_one_e_erf_opt(A1_center, A2_center, power_A1, power_A2, C_center(ipoint,1:3), n_pt_in, d, n_pt_out, p_inv_2, p_new2, P_center)
if(n_pt_out < 0) then
cycle
endif
! sum of integrals of type : int {t,[0,1]} exp-(rho.(P-Q)^2 * t^2) * t^i
accu = 0.d0
do i = 0, n_pt_out, 2
accu += d(i) * rint(i/2, const)
enddo
res_v(ipoint) = accu * coeff
enddo
endif
end subroutine NAI_pol_mult_erf_with1s_v
! ---
subroutine give_polynomial_mult_center_one_e_erf_opt(A_center, B_center, power_A, power_B, C_center, n_pt_in, d, n_pt_out, p_inv_2, p_new, P_center)
2019-01-25 11:39:31 +01:00
BEGIN_DOC
2019-01-29 15:40:00 +01:00
! Returns the explicit polynomial in terms of the $t$ variable of the
! following polynomial:
2019-01-25 11:39:31 +01:00
!
! $I_{x1}(a_x, d_x,p,q) \times I_{x1}(a_y, d_y,p,q) \times I_{x1}(a_z, d_z,p,q)$.
END_DOC
2023-02-06 19:00:35 +01:00
2019-01-25 11:39:31 +01:00
implicit none
2023-02-06 19:00:35 +01:00
integer, intent(in) :: n_pt_in
integer, intent(in) :: power_A(3), power_B(3)
double precision, intent(in) :: A_center(3), B_center(3), C_center(3), p_inv_2, p_new, P_center(3)
integer, intent(out) :: n_pt_out
double precision, intent(out) :: d(0:n_pt_in)
integer :: a_x, b_x, a_y, b_y, a_z, b_z
integer :: n_pt1, n_pt2, n_pt3, dim, i
integer :: n_pt_tmp
double precision :: d1(0:n_pt_in)
double precision :: d2(0:n_pt_in)
double precision :: d3(0:n_pt_in)
double precision :: accu
double precision :: R1x(0:2), B01(0:2), R1xp(0:2), R2x(0:2)
2019-01-25 11:39:31 +01:00
accu = 0.d0
ASSERT (n_pt_in > 1)
2023-02-06 19:00:35 +01:00
R1x(0) = (P_center(1) - A_center(1))
R1x(1) = 0.d0
R1x(2) = -(P_center(1) - C_center(1))* p_new
2019-01-25 11:39:31 +01:00
! R1x = (P_x - A_x) - (P_x - C_x) ( t * mu/sqrt(p+mu^2) )^2
2023-02-06 19:00:35 +01:00
R1xp(0) = (P_center(1) - B_center(1))
R1xp(1) = 0.d0
R1xp(2) =-(P_center(1) - C_center(1))* p_new
2019-01-25 11:39:31 +01:00
!R1xp = (P_x - B_x) - (P_x - C_x) ( t * mu/sqrt(p+mu^2) )^2
2023-02-06 19:00:35 +01:00
R2x(0) = p_inv_2
R2x(1) = 0.d0
R2x(2) = -p_inv_2 * p_new
2019-01-25 11:39:31 +01:00
!R2x = 0.5 / p - 0.5/p ( t * mu/sqrt(p+mu^2) )^2
2023-02-06 19:00:35 +01:00
do i = 0, n_pt_in
d (i) = 0.d0
2019-01-25 11:39:31 +01:00
d1(i) = 0.d0
d2(i) = 0.d0
d3(i) = 0.d0
enddo
2023-02-06 19:00:35 +01:00
2019-01-25 11:39:31 +01:00
n_pt1 = n_pt_in
n_pt2 = n_pt_in
n_pt3 = n_pt_in
a_x = power_A(1)
b_x = power_B(1)
2023-02-06 19:00:35 +01:00
call I_x1_pol_mult_one_e(a_x, b_x, R1x, R1xp, R2x, d1, n_pt1, n_pt_in)
2019-01-25 11:39:31 +01:00
if(n_pt1<0)then
n_pt_out = -1
do i = 0,n_pt_in
d(i) = 0.d0
enddo
return
endif
2023-02-06 19:00:35 +01:00
R1x(0) = (P_center(2) - A_center(2))
R1x(1) = 0.d0
R1x(2) = -(P_center(2) - C_center(2))* p_new
2019-01-25 11:39:31 +01:00
! R1x = (P_x - A_x) - (P_x - C_x) ( t * mu/sqrt(p+mu^2) )^2
2023-02-06 19:00:35 +01:00
R1xp(0) = (P_center(2) - B_center(2))
R1xp(1) = 0.d0
R1xp(2) =-(P_center(2) - C_center(2))* p_new
2019-01-25 11:39:31 +01:00
!R1xp = (P_x - B_x) - (P_x - C_x) ( t * mu/sqrt(p+mu^2) )^2
a_y = power_A(2)
b_y = power_B(2)
2023-02-06 19:00:35 +01:00
call I_x1_pol_mult_one_e(a_y, b_y, R1x, R1xp, R2x, d2, n_pt2, n_pt_in)
2019-01-25 11:39:31 +01:00
if(n_pt2<0)then
n_pt_out = -1
do i = 0,n_pt_in
d(i) = 0.d0
enddo
return
endif
2023-02-06 19:00:35 +01:00
R1x(0) = (P_center(3) - A_center(3))
R1x(1) = 0.d0
R1x(2) = -(P_center(3) - C_center(3)) * p_new
2019-01-25 11:39:31 +01:00
! R1x = (P_x - A_x) - (P_x - C_x) ( t * mu/sqrt(p+mu^2) )^2
2023-02-06 19:00:35 +01:00
R1xp(0) = (P_center(3) - B_center(3))
R1xp(1) = 0.d0
R1xp(2) =-(P_center(3) - C_center(3)) * p_new
2019-01-25 11:39:31 +01:00
!R2x = 0.5 / p - 0.5/p ( t * mu/sqrt(p+mu^2) )^2
a_z = power_A(3)
b_z = power_B(3)
2023-02-06 19:00:35 +01:00
call I_x1_pol_mult_one_e(a_z, b_z, R1x, R1xp, R2x, d3, n_pt3, n_pt_in)
if(n_pt3 < 0) then
2019-01-25 11:39:31 +01:00
n_pt_out = -1
do i = 0,n_pt_in
d(i) = 0.d0
enddo
return
endif
2023-02-06 19:00:35 +01:00
2019-01-25 11:39:31 +01:00
n_pt_tmp = 0
2023-02-06 19:00:35 +01:00
call multiply_poly(d1, n_pt1, d2, n_pt2, d, n_pt_tmp)
do i = 0, n_pt_tmp
2019-01-25 11:39:31 +01:00
d1(i) = 0.d0
enddo
n_pt_out = 0
2023-02-06 19:00:35 +01:00
call multiply_poly(d, n_pt_tmp, d3, n_pt3, d1, n_pt_out)
2019-01-25 11:39:31 +01:00
do i = 0, n_pt_out
d(i) = d1(i)
enddo
2023-02-06 19:00:35 +01:00
end subroutine give_polynomial_mult_center_one_e_erf_opt
2019-01-25 11:39:31 +01:00
2023-02-06 19:00:35 +01:00
! ---
subroutine give_polynomial_mult_center_one_e_erf(A_center,B_center,alpha,beta,power_A,power_B,C_center,n_pt_in,d,n_pt_out,mu_in)
2019-01-25 11:39:31 +01:00
BEGIN_DOC
2023-02-06 19:00:35 +01:00
! Returns the explicit polynomial in terms of the $t$ variable of the
2019-01-29 15:40:00 +01:00
! following polynomial:
2019-01-25 11:39:31 +01:00
!
! $I_{x1}(a_x, d_x,p,q) \times I_{x1}(a_y, d_y,p,q) \times I_{x1}(a_z, d_z,p,q)$.
END_DOC
2023-02-06 19:00:35 +01:00
2019-01-25 11:39:31 +01:00
implicit none
integer, intent(in) :: n_pt_in
integer,intent(out) :: n_pt_out
double precision, intent(in) :: A_center(3), B_center(3),C_center(3)
double precision, intent(in) :: alpha,beta,mu_in
integer, intent(in) :: power_A(3), power_B(3)
integer :: a_x,b_x,a_y,b_y,a_z,b_z
double precision :: d(0:n_pt_in)
double precision :: d1(0:n_pt_in)
double precision :: d2(0:n_pt_in)
double precision :: d3(0:n_pt_in)
double precision :: accu, pq_inv, p10_1, p10_2, p01_1, p01_2
double precision :: p,P_center(3),rho,p_inv,p_inv_2
accu = 0.d0
ASSERT (n_pt_in > 1)
p = alpha+beta
p_inv = 1.d0/p
p_inv_2 = 0.5d0/p
do i =1, 3
P_center(i) = (alpha * A_center(i) + beta * B_center(i)) * p_inv
enddo
double precision :: R1x(0:2), B01(0:2), R1xp(0:2),R2x(0:2)
R1x(0) = (P_center(1) - A_center(1))
R1x(1) = 0.d0
R1x(2) = -(P_center(1) - C_center(1))* mu_in**2 / (p+mu_in*mu_in)
! R1x = (P_x - A_x) - (P_x - C_x) ( t * mu/sqrt(p+mu^2) )^2
R1xp(0) = (P_center(1) - B_center(1))
R1xp(1) = 0.d0
R1xp(2) =-(P_center(1) - C_center(1))* mu_in**2 / (p+mu_in*mu_in)
!R1xp = (P_x - B_x) - (P_x - C_x) ( t * mu/sqrt(p+mu^2) )^2
R2x(0) = p_inv_2
R2x(1) = 0.d0
R2x(2) = -p_inv_2* mu_in**2 / (p+mu_in*mu_in)
!R2x = 0.5 / p - 0.5/p ( t * mu/sqrt(p+mu^2) )^2
do i = 0,n_pt_in
d(i) = 0.d0
enddo
do i = 0,n_pt_in
d1(i) = 0.d0
enddo
do i = 0,n_pt_in
d2(i) = 0.d0
enddo
do i = 0,n_pt_in
d3(i) = 0.d0
enddo
integer :: n_pt1,n_pt2,n_pt3,dim,i
n_pt1 = n_pt_in
n_pt2 = n_pt_in
n_pt3 = n_pt_in
a_x = power_A(1)
b_x = power_B(1)
call I_x1_pol_mult_one_e(a_x,b_x,R1x,R1xp,R2x,d1,n_pt1,n_pt_in)
! print*,'passed the first I_x1'
if(n_pt1<0)then
n_pt_out = -1
do i = 0,n_pt_in
d(i) = 0.d0
enddo
return
endif
R1x(0) = (P_center(2) - A_center(2))
R1x(1) = 0.d0
R1x(2) = -(P_center(2) - C_center(2))* mu_in**2 / (p+mu_in*mu_in)
! R1x = (P_x - A_x) - (P_x - C_x) ( t * mu/sqrt(p+mu^2) )^2
R1xp(0) = (P_center(2) - B_center(2))
R1xp(1) = 0.d0
R1xp(2) =-(P_center(2) - C_center(2))* mu_in**2 / (p+mu_in*mu_in)
!R1xp = (P_x - B_x) - (P_x - C_x) ( t * mu/sqrt(p+mu^2) )^2
a_y = power_A(2)
b_y = power_B(2)
call I_x1_pol_mult_one_e(a_y,b_y,R1x,R1xp,R2x,d2,n_pt2,n_pt_in)
! print*,'passed the second I_x1'
if(n_pt2<0)then
n_pt_out = -1
do i = 0,n_pt_in
d(i) = 0.d0
enddo
return
endif
R1x(0) = (P_center(3) - A_center(3))
R1x(1) = 0.d0
R1x(2) = -(P_center(3) - C_center(3))* mu_in**2 / (p+mu_in*mu_in)
! R1x = (P_x - A_x) - (P_x - C_x) ( t * mu/sqrt(p+mu^2) )^2
R1xp(0) = (P_center(3) - B_center(3))
R1xp(1) = 0.d0
R1xp(2) =-(P_center(3) - C_center(3))* mu_in**2 / (p+mu_in*mu_in)
!R2x = 0.5 / p - 0.5/p ( t * mu/sqrt(p+mu^2) )^2
a_z = power_A(3)
b_z = power_B(3)
! print*,'a_z = ',a_z
! print*,'b_z = ',b_z
call I_x1_pol_mult_one_e(a_z,b_z,R1x,R1xp,R2x,d3,n_pt3,n_pt_in)
! print*,'passed the third I_x1'
if(n_pt3<0)then
n_pt_out = -1
do i = 0,n_pt_in
d(i) = 0.d0
enddo
return
endif
integer :: n_pt_tmp
n_pt_tmp = 0
call multiply_poly(d1,n_pt1,d2,n_pt2,d,n_pt_tmp)
do i = 0,n_pt_tmp
d1(i) = 0.d0
enddo
n_pt_out = 0
call multiply_poly(d ,n_pt_tmp ,d3,n_pt3,d1,n_pt_out)
do i = 0, n_pt_out
d(i) = d1(i)
enddo
end