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289 KiB
289 KiB
Forces
- Introduction
- Context
- Finite-difference function
- Forces of the Jastrow function
- Electron-nucleus Jastrow
- Electron-electron-nucleus Jastrow
- Force of tmp_c matrix
- Force of dtmp_c matrix
- Force of electron-electron-nucleus Jastrow value
- Force of derivatives of electron-nucleus rescaled distance
- Force of electron-electron-nucleus Jastrow gradient
- Force of electron-electron-nucleus Jastrow Laplacian
- Force of delta_p matrix
- Force of single electron-electron-nucleus Jastrow value
- Forces of the orbitals
Introduction
To calculate interatomic forces, a derivative (with respect to nuclei) of the values, gradient and Laplacian of the Jastrow and the molecular orbitals (MO) is required. Furthermore, for the nonlocal pseudopotential, also the forces of the values of the single-electron move Jastrows are required.
Context
Data structure
typedef struct qmckl_forces_struct{
double * restrict forces_jastrow_en;
uint64_t forces_jastrow_en_date;
double * restrict forces_jastrow_en_g;
uint64_t forces_jastrow_en_g_date;
double * restrict forces_jastrow_en_l;
uint64_t forces_jastrow_en_l_date;
double * restrict forces_tmp_c;
uint64_t forces_tmp_c_date;
double * restrict forces_dtmp_c;
uint64_t forces_dtmp_c_date;
double * restrict forces_een_n;
uint64_t forces_een_n_date;
double * restrict forces_jastrow_een;
uint64_t forces_jastrow_een_date;
double * restrict forces_jastrow_een_g;
uint64_t forces_jastrow_een_g_date;
double * restrict forces_jastrow_een_l;
uint64_t forces_jastrow_een_l_date;
double * restrict forces_ao_value;
uint64_t forces_ao_value_date;
uint64_t forces_ao_value_maxsize;
double * restrict forces_mo_value;
uint64_t forces_mo_value_date;
uint64_t forces_mo_value_maxsize;
double * restrict forces_mo_g;
uint64_t forces_mo_g_date;
double * restrict forces_mo_l;
uint64_t forces_mo_l_date;
double * forces_jastrow_single_en;
uint64_t forces_jastrow_single_en_date;
double * forces_jastrow_single_een;
uint64_t forces_jastrow_single_een_date;
double * forces_delta_p;
uint64_t forces_delta_p_date;
} qmckl_forces_struct;Finite-difference function
We introduce here a general function to compute the derivatives of any quantity with respect to nuclear coordinates. using finite-differences.
typedef qmckl_exit_code (*function_callback)(qmckl_context context, double* const output, const int64_t size);
qmckl_exit_code qmckl_finite_difference_deriv_n(
qmckl_context context,
const double delta_x,
function_callback get_function,
double* const derivative_output,
int64_t const size)
{
// Finite difference coefficients for a 9-point stencil
double coef[9] = { 1.0/280.0, -4.0/105.0, 1.0/5.0, -4.0/5.0, 0.0, 4.0/5.0, -1.0/5.0, 4.0/105.0, -1.0/280.0 };
qmckl_exit_code rc;
int64_t walk_num;
rc = qmckl_get_electron_walk_num(context, &walk_num);
if (rc != QMCKL_SUCCESS) {
return rc;
}
int64_t nucl_num;
rc = qmckl_get_nucleus_num(context, &nucl_num);
if (rc != QMCKL_SUCCESS) {
return rc;
}
double* nucleus_coord = (double*) malloc(3 * nucl_num * sizeof(double));
if (nucleus_coord == NULL) {
return QMCKL_ALLOCATION_FAILED;
}
rc = qmckl_get_nucleus_coord (context, 'N', nucleus_coord, 3*nucl_num);
double* temp_coord = (double*) malloc(3 * nucl_num * sizeof(double));
if (temp_coord == NULL) {
free(nucleus_coord);
return QMCKL_ALLOCATION_FAILED;
}
double* function_values = (double*) malloc(walk_num*size * sizeof(double));
if (function_values == NULL) {
free(nucleus_coord);
free(temp_coord);
return QMCKL_ALLOCATION_FAILED;
}
memset(derivative_output, 0, nucl_num*3*walk_num*size*sizeof(double));
// Copy original coordinates
for (int i = 0; i < 3 * nucl_num; i++) {
temp_coord[i] = nucleus_coord[i];
}
for (int64_t a = 0; a < nucl_num; a++) {
for (int64_t k = 0; k < 3; k++) {
for (int64_t m = -4; m <= 4; m++) {
// Apply finite difference displacement
temp_coord[k+a*3] = nucleus_coord[k+3*a] + (double) m * delta_x;
// Update coordinates in the context
rc = qmckl_set_nucleus_coord(context, 'N', temp_coord, 3*nucl_num);
assert(rc == QMCKL_SUCCESS);
rc = qmckl_context_touch(context);
assert(rc == QMCKL_SUCCESS);
rc = qmckl_single_touch(context);
assert(rc == QMCKL_SUCCESS);
// Call the provided function
rc = get_function(context, function_values, walk_num*size);
assert(rc == QMCKL_SUCCESS);
// Accumulate derivative using finite-difference coefficients
for (int64_t nw=0 ; nw<walk_num ; nw++) {
int64_t shift = nucl_num*3*size*nw + size*(k + 3*a);
for (int64_t i = 0; i < size; i++) {
derivative_output[i+shift] += coef[m + 4] * function_values[nw*size+i];
}
}
}
temp_coord[k+a*3] = nucleus_coord[k+3*a];
}
}
// Reset coordinates in the context
rc = qmckl_set_nucleus_coord(context, 'N', temp_coord, 3*nucl_num);
assert(rc == QMCKL_SUCCESS);
rc = qmckl_context_touch(context);
assert(rc == QMCKL_SUCCESS);
// Normalize by the step size
for (int64_t i = 0; i < size*3*nucl_num*walk_num ; i++) {
derivative_output[i] /= delta_x;
}
free(nucleus_coord);
free(temp_coord);
free(function_values);
return QMCKL_SUCCESS;
}Forces of the Jastrow function
For the forces of the Jastrow function, there is only a contribution from the electron-nucleus and electron-electron-nucleus Jastrow, since the electron-electron Jastrow does not depend on nuclear coordinates.
Electron-nucleus Jastrow
Force of electron-nucleus Jastrow value
Calculates the force of the electron-nucleus Jastrow value. The terms of the force of the electron-nucleus Jastrow value are identical to the gradient of this Jastrow, up to a minus sign. \[ \partial_{\alpha,m} J_{en} = -\sum_i \left( \frac{a_1 \partial_{i,m} \widetilde{R}_{i\alpha}}{(1+a_2 \widetilde{R}_{i\alpha} )^2} + \sum_{k=2}^{N_\text{aord}} a_k k \widetilde{R}_{i\alpha}^{k-1} \partial_{i,m} \widetilde{R}_{i\alpha} \right) \]
Get
qmckl_exit_code
qmckl_get_forces_jastrow_en(qmckl_context context,
double* const forces_jastrow_en,
const int64_t size_max);interface
integer(qmckl_exit_code) function qmckl_get_forces_jastrow_en (context, &
forces_jastrow_en, size_max) bind(C)
use, intrinsic :: iso_c_binding
import
implicit none
integer (qmckl_context) , intent(in), value :: context
integer(c_int64_t), intent(in), value :: size_max
real(c_double), intent(out) :: forces_jastrow_en(size_max)
end function qmckl_get_forces_jastrow_en
end interfaceCompute
| Variable | Type | In/Out | Description |
|---|---|---|---|
context |
qmckl_context |
in | Global state |
walk_num |
int64_t |
in | Number of walkers |
elec_num |
int64_t |
in | Number of electrons |
nucl_num |
int64_t |
in | Number of nuclei |
type_nucl_num |
int64_t |
in | Number of unique nuclei |
type_nucl_vector |
int64_t[nucl_num] |
in | IDs of unique nuclei |
aord_num |
int64_t |
in | Number of coefficients |
a_vector |
double[type_nucl_num][aord_num+1] |
in | List of coefficients |
en_distance_rescaled |
double[walk_num][nucl_num][elec_num] |
in | Electron-nucleus distances |
en_distance_rescaled_gl |
double[walk_num][nucl_num][elec_num][4] |
in | Electron-nucleus distance derivatives |
forces_jastrow_en |
double[walk_num][nucl_num][3] |
out | Electron-nucleus forces |
function qmckl_compute_forces_jastrow_en_doc( &
context, walk_num, elec_num, nucl_num, type_nucl_num, &
type_nucl_vector, aord_num, a_vector, &
en_distance_rescaled, en_distance_rescaled_gl, forces_jastrow_en) &
bind(C) result(info)
use qmckl
implicit none
integer (qmckl_context), intent(in), value :: context
integer (c_int64_t) , intent(in) , value :: walk_num
integer (c_int64_t) , intent(in) , value :: elec_num
integer (c_int64_t) , intent(in) , value :: nucl_num
integer (c_int64_t) , intent(in) , value :: type_nucl_num
integer (c_int64_t) , intent(in) :: type_nucl_vector(nucl_num)
integer (c_int64_t) , intent(in) , value :: aord_num
real (c_double ) , intent(in) :: a_vector(aord_num+1,type_nucl_num)
real (c_double ) , intent(in) :: en_distance_rescaled(elec_num,nucl_num,walk_num)
real (c_double ) , intent(in) :: en_distance_rescaled_gl(4, elec_num,nucl_num,walk_num)
real (c_double ) , intent(out) :: forces_jastrow_en(3,nucl_num,walk_num)
integer(qmckl_exit_code) :: info
integer*8 :: i, a, k, nw, ii
double precision :: x, x1, kf
double precision :: denom, invdenom, invdenom2, f
double precision :: dx(3)
info = QMCKL_SUCCESS
if (context == QMCKL_NULL_CONTEXT) then
info = QMCKL_INVALID_CONTEXT
return
endif
if (walk_num <= 0) then
info = QMCKL_INVALID_ARG_2
return
endif
if (elec_num <= 0) then
info = QMCKL_INVALID_ARG_3
return
endif
if (nucl_num <= 0) then
info = QMCKL_INVALID_ARG_4
return
endif
if (aord_num < 0) then
info = QMCKL_INVALID_ARG_7
return
endif
do nw =1, walk_num
forces_jastrow_en(:,:,nw) = 0.0d0
do a = 1, nucl_num
do i = 1, elec_num
x = en_distance_rescaled(i,a,nw)
if(abs(x) < 1.d-12) continue
denom = 1.0d0 + a_vector(2, type_nucl_vector(a)+1) * x
invdenom = 1.0d0 / denom
invdenom2 = invdenom*invdenom
dx(1) = -en_distance_rescaled_gl(1,i,a,nw)
dx(2) = -en_distance_rescaled_gl(2,i,a,nw)
dx(3) = -en_distance_rescaled_gl(3,i,a,nw)
f = a_vector(1, type_nucl_vector(a)+1) * invdenom2
forces_jastrow_en(1,a,nw) = forces_jastrow_en(1,a,nw) + f * dx(1)
forces_jastrow_en(2,a,nw) = forces_jastrow_en(2,a,nw) + f * dx(2)
forces_jastrow_en(3,a,nw) = forces_jastrow_en(3,a,nw) + f * dx(3)
kf = 2.d0
x1 = x
x = 1.d0
do k=2, aord_num
f = a_vector(k+1,type_nucl_vector(a)+1) * kf * x
forces_jastrow_en(1,a,nw) = forces_jastrow_en(1,a,nw) + f * x1 * dx(1)
forces_jastrow_en(2,a,nw) = forces_jastrow_en(2,a,nw) + f * x1 * dx(2)
forces_jastrow_en(3,a,nw) = forces_jastrow_en(3,a,nw) + f * x1 * dx(3)
x = x*x1
kf = kf + 1.d0
end do
end do
end do
end do
end function qmckl_compute_forces_jastrow_en_docForce of electron-nucleus Jastrow gradient
To avoid having to create new arrays for the Hessian of the rescaled distances, we compute parts of it manually in this routine.
\begin{eqnarray} \partial_{\alpha,m} \partial_{i,n} J_{en} & = \frac{a_1 \partial_{\alpha,m} \partial_{i,n} \widetilde{R}_{i\alpha} }{(1+a_2 \widetilde{R}_{i\alpha})^2} - 2 \frac{a_1 a_2 \partial_{\alpha,m} \widetilde{R}_{i\alpha} \partial_{i,n} \widetilde{R}_{i\alpha}}{(1+a_2 \widetilde{R}_{i\alpha})^3} + \sum_{k=2}^{N_\text{aord}} a_k k \left((k-1) \widetilde{R}_{i\alpha}^{k-2} \partial_{\alpha,m} \widetilde{R}_{i\alpha} \partial_{i,n} \widetilde{R}_{i\alpha} + \widetilde{R}_{i\alpha}^{k-1} \partial_{\alpha,m}\partial_{i,n} \widetilde{R}_{i\alpha} \right) \\ & = -\frac{a_1 e^{-\kappa R_{i\alpha}}}{R_{i\alpha }(1+a_2 \widetilde{R}_{i\alpha})^2} + \frac{a_1 \partial_{i,m} \widetilde{R}_{i\alpha} \partial_{i,n} \widetilde{R}_{i\alpha} }{(1+a_2 \widetilde{R}_{i\alpha})^2}\left (\frac{e^{\kappa R_{i\alpha}}}{R_{i\alpha}} + \kappa e^{\kappa R_{i\alpha}} \right) + 2 \frac{a_1 a_2 \partial_{i,m} \widetilde{R}_{i\alpha} \partial_{i,n} \widetilde{R}_{i\alpha}}{(1+a_2 \widetilde{R}_{i\alpha})^3} \\ &- \sum_{k=2}^{N_\text{aord}} a_k k \left((k-1) \widetilde{R}_{i\alpha}^{k-2} \partial_{\alpha,m} \widetilde{R}_{i\alpha} \partial_{i,n} \widetilde{R}_{i\alpha} - \widetilde{R}_{i\alpha}^{k-1} \partial_{i,m}\widetilde{R}_{i\alpha}\partial_{i,n} \widetilde{R}_{i\alpha} e^{\kappa R_{i\alpha}} (\kappa + \frac{1}{R_{i\alpha}}) + \delta_{n,m} e^{-\kappa R_{i\alpha}}\frac{1}{R_{i\alpha}} \right)\\ \end{eqnarray}Get
qmckl_exit_code
qmckl_get_forces_jastrow_en_g(qmckl_context context,
double* const forces_jastrow_en_g,
const int64_t size_max);interface
integer(qmckl_exit_code) function qmckl_get_forces_jastrow_en_g (context, &
forces_jastrow_en_g, size_max) bind(C)
use, intrinsic :: iso_c_binding
import
implicit none
integer (qmckl_context) , intent(in), value :: context
integer(c_int64_t), intent(in), value :: size_max
real(c_double), intent(out) :: forces_jastrow_en_g(size_max)
end function qmckl_get_forces_jastrow_en_g
end interfaceCompute
| Variable | Type | In/Out | Description |
|---|---|---|---|
context |
qmckl_context |
in | Global state |
walk_num |
int64_t |
in | Number of walkers |
elec_num |
int64_t |
in | Number of electrons |
nucl_num |
int64_t |
in | Number of nuclei |
type_nucl_num |
int64_t |
in | Number of unique nuclei |
type_nucl_vector |
int64_t[nucl_num] |
in | IDs of unique nuclei |
aord_num |
int64_t |
in | Number of coefficients |
a_vector |
double[type_nucl_num][aord_num+1] |
in | List of coefficients |
rescale_factor_en |
double[type_nucl_num] |
in | Rescale factor for electron-nucleus |
en_distance |
double[walk_num][elec_num][nucl_num] |
in | Electron-nucleus distances |
en_distance_rescaled |
double[walk_num][nucl_num][elec_num] |
in | Electron-nucleus distances |
en_distance_rescaled_gl |
double[walk_num][nucl_num][elec_num][4] |
in | Electron-nucleus distance derivatives |
forces_jastrow_en_g |
double[walk_num][nucl_num][3][elec_num][3] |
out | Force of electron-nucleus gradient |
function qmckl_compute_forces_jastrow_en_g_doc( &
context, walk_num, elec_num, nucl_num, type_nucl_num, &
type_nucl_vector, aord_num, a_vector, rescale_factor_en, en_distance, &
en_distance_rescaled, en_distance_rescaled_gl, forces_jastrow_en_g) &
bind(C) result(info)
use qmckl
implicit none
integer (qmckl_context), intent(in), value :: context
integer (c_int64_t) , intent(in) , value :: walk_num
integer (c_int64_t) , intent(in) , value :: elec_num
integer (c_int64_t) , intent(in) , value :: nucl_num
integer (c_int64_t) , intent(in) , value :: type_nucl_num
integer (c_int64_t) , intent(in) :: type_nucl_vector(nucl_num)
integer (c_int64_t) , intent(in) , value :: aord_num
real (c_double ) , intent(in) :: a_vector(aord_num+1,type_nucl_num)
real (c_double ) , intent(in) :: rescale_factor_en(type_nucl_num)
real (c_double ) , intent(in) :: en_distance(nucl_num,elec_num,walk_num)
real (c_double ) , intent(in) :: en_distance_rescaled(elec_num,nucl_num,walk_num)
real (c_double ) , intent(in) :: en_distance_rescaled_gl(4, elec_num,nucl_num,walk_num)
real (c_double ) , intent(out) :: forces_jastrow_en_g(3,elec_num,3,nucl_num,walk_num)
integer(qmckl_exit_code) :: info
integer*8 :: i, a, k, nw, ii, m,l
double precision :: x, x1, kf
double precision :: denom, invdenom, invdenom2, f, f2, expk, invdist
double precision :: dx(4)
info = QMCKL_SUCCESS
if (context == QMCKL_NULL_CONTEXT) then
info = QMCKL_INVALID_CONTEXT
return
endif
if (walk_num <= 0) then
info = QMCKL_INVALID_ARG_2
return
endif
if (elec_num <= 0) then
info = QMCKL_INVALID_ARG_3
return
endif
if (nucl_num <= 0) then
info = QMCKL_INVALID_ARG_4
return
endif
if (aord_num < 0) then
info = QMCKL_INVALID_ARG_7
return
endif
do nw =1, walk_num
forces_jastrow_en_g(:,:,:,:,nw) = 0.0d0
do a = 1, nucl_num
do i = 1, elec_num
expk = dexp(rescale_factor_en(type_nucl_vector(a)+1) * en_distance(a,i,nw))
invdist = 1.d0 / en_distance(a,i,nw)
x = en_distance_rescaled(i,a,nw)
if(abs(x) < 1.d-12) continue
denom = 1.0d0 + a_vector(2, type_nucl_vector(a)+1) * x
invdenom = 1.0d0 / denom
invdenom2 = invdenom*invdenom
f = a_vector(1, type_nucl_vector(a)+1) * invdenom2
do m = 1, 3
dx(m) = en_distance_rescaled_gl(m,i,a,nw)
end do
do m = 1, 3
do l = 1,3
if (m == l) then
forces_jastrow_en_g(m,i,l,a,nw) = forces_jastrow_en_g(m,i,l,a,nw) - f * invdist / expk
end if
forces_jastrow_en_g(m,i,l,a,nw) = forces_jastrow_en_g(m,i,l,a,nw) + &
f * dx(m) * dx(l) * expk * (invdist + rescale_factor_en(type_nucl_vector(a)+1))
forces_jastrow_en_g(m,i,l,a,nw) = forces_jastrow_en_g(m,i,l,a,nw) + 2.d0 * f * invdenom * &
a_vector(2, type_nucl_vector(a)+1) * dx(m) * dx(l)
end do
end do
kf = 2.d0
x1 = x
x = 1.d0
do k=2, aord_num
f = a_vector(k+1,type_nucl_vector(a)+1) * kf * x
f2 = a_vector(k+1,type_nucl_vector(a)+1) * kf * x * (kf-1.d0)
do m = 1, 3
do l = 1, 3
if (m == l) then
forces_jastrow_en_g(m,i,l,a,nw) = forces_jastrow_en_g(m,i,l,a,nw) - f * x1 * invdist / expk
end if
forces_jastrow_en_g(m,i,l,a,nw) = forces_jastrow_en_g(m,i,l,a,nw) - f2 * dx(m) * dx(l) &
+ f * x1 * dx(m) * dx(l) * rescale_factor_en(type_nucl_vector(a)+1) * expk &
+ f * x1 * dx(m) * dx(l) * invdist * expk
end do
end do
x = x*x1
kf = kf + 1.d0
end do
end do
end do
end do
end function qmckl_compute_forces_jastrow_en_g_docForce of electron-nucleus Jastrow Laplacian
Calculates the force of the electron-nucleus Jastrow Laplacian. To avoid having to calculate higher order derivatives of the rescaled distances elsewhere, the neccessery terms are calcuculated on the fly.
\begin{eqnarray} \partial_{\alpha,m} \nabla^2 J_{en} =& \sum_i \left(\partial_{\alpha,m}\frac{a_1 \nabla^2 \widetilde{R}_{i\alpha}}{(1+a_2 \widetilde{R}_{i\alpha})^2} - \partial_{\alpha,m} \frac{2a_1a_2 (\nabla\widetilde{R}_{i\alpha}\cdot \nabla \widetilde{R}_{i\alpha})}{(1+a_2\widetilde{R}_{i\alpha})^3} + \partial_{\alpha,m} \sum_{k=2}^{N_\text{aord}} a_k k \left( \widetilde{R}_{i\alpha}^{k-1} \nabla^2\widetilde{R}_{i\alpha} + (k-1)\widetilde{R}_{i\alpha}^{k-2} (\nabla \widetilde{R}_{i\alpha}\cdot \nabla \widetilde{R}_{i\alpha} ) \right) \right)\\ =&\sum_i \left( \frac{a_1 \partial_{i,m} \widetilde{R}_{i\alpha}}{(1+a_2 \widetilde{R}_{i\alpha})^2}\left( \frac{2\kappa}{R_{i\alpha}} - \kappa^2 + \frac{2}{R^2_{i\alpha}}\right) + \frac{2a_1a_2\partial_{i,m}\widetilde{R}_{i\alpha}\nabla^2\widetilde{R}_{i\alpha}}{(1+a_2 \widetilde{R}_{i\alpha})^3} - \frac{4a_1a_2\kappa e^{-\kappa R_{i\alpha}}\partial_{i,m}\widetilde{R}_{i\alpha}}{(1+a_2 \widetilde{R}_{i\alpha})^3} - \frac{6 a_1 a_2^2 (\nabla \widetilde{R}_{i\alpha} \cdot \nabla \widetilde{R}_{i\alpha})\partial_{i,m}\widetilde{R}_{i\alpha}}{(1+a_2 \widetilde{R}_{i\alpha})^4} \right.\\ &\left.+ \sum_{k=2}^{N_\text{aord}} a_k k \left( -(k-1) \widetilde{R}_{i\alpha}^{k-2}\partial_{i,m}\widetilde{R}_{i\alpha} \nabla^2\widetilde{R}_{i\alpha} + \widetilde{R}_{i\alpha}^{k-1}\partial_{i,m}\widetilde{R}_{i\alpha}\left(\frac{2\kappa}{R_{i\alpha}} - \kappa^2 + \frac{2}{R_{i\alpha}^2} \right) - (k-1)(k-2)\widetilde{R}_{i\alpha}^{k-3}\partial_{i,m}\widetilde{R}_{i\alpha}(\nabla\widetilde{R}_{i\alpha} \cdot \nabla \widetilde{R}_{i\alpha}) + 2\kappa(k-1)\widetilde{R}_{i\alpha}^{k-2} e^{-\kappa R_{i\alpha}} \partial_{i,m}\widetilde{R}_{i\alpha} \right) \right) \end{eqnarray}Get
qmckl_exit_code
qmckl_get_forces_jastrow_en_l(qmckl_context context,
double* const forces_jastrow_en_l,
const int64_t size_max);interface
integer(qmckl_exit_code) function qmckl_get_forces_jastrow_en_l (context, &
forces_jastrow_en_l, size_max) bind(C)
use, intrinsic :: iso_c_binding
import
implicit none
integer (qmckl_context) , intent(in), value :: context
integer(c_int64_t), intent(in), value :: size_max
real(c_double), intent(out) :: forces_jastrow_en_l(size_max)
end function qmckl_get_forces_jastrow_en_l
end interfaceCompute
| Variable | Type | In/Out | Description |
|---|---|---|---|
context |
qmckl_context |
in | Global state |
walk_num |
int64_t |
in | Number of walkers |
elec_num |
int64_t |
in | Number of electrons |
nucl_num |
int64_t |
in | Number of nuclei |
type_nucl_num |
int64_t |
in | Number of unique nuclei |
type_nucl_vector |
int64_t[nucl_num] |
in | IDs of unique nuclei |
aord_num |
int64_t |
in | Number of coefficients |
a_vector |
double[type_nucl_num][aord_num+1] |
in | List of coefficients |
rescale_factor_en |
double[type_nucl_num] |
in | Rescale factor for electron-nucleus |
en_distance |
double[walk_num][elec_num][nucl_num] |
in | Electron-nucleus distances |
en_distance_rescaled |
double[walk_num][nucl_num][elec_num] |
in | Electron-nucleus distances |
en_distance_rescaled_gl |
double[walk_num][nucl_num][elec_num][4] |
in | Electron-nucleus distance derivatives |
forces_jastrow_en_l |
double[walk_num][nucl_num][3] |
out | Forces of electron-nucleus Laplacian |
function qmckl_compute_forces_jastrow_en_l_doc( &
context, walk_num, elec_num, nucl_num, type_nucl_num, &
type_nucl_vector, aord_num, a_vector, rescale_factor_en, en_distance, &
en_distance_rescaled, en_distance_rescaled_gl, forces_jastrow_en_l) &
bind(C) result(info)
use qmckl
implicit none
integer (qmckl_context), intent(in), value :: context
integer (c_int64_t) , intent(in) , value :: walk_num
integer (c_int64_t) , intent(in) , value :: elec_num
integer (c_int64_t) , intent(in) , value :: nucl_num
integer (c_int64_t) , intent(in) , value :: type_nucl_num
integer (c_int64_t) , intent(in) :: type_nucl_vector(nucl_num)
integer (c_int64_t) , intent(in) , value :: aord_num
real (c_double ) , intent(in) :: a_vector(aord_num+1,type_nucl_num)
real (c_double ) , intent(in) :: rescale_factor_en(type_nucl_num)
real (c_double ) , intent(in) :: en_distance(nucl_num, elec_num, walk_num)
real (c_double ) , intent(in) :: en_distance_rescaled(elec_num,nucl_num,walk_num)
real (c_double ) , intent(in) :: en_distance_rescaled_gl(4, elec_num,nucl_num,walk_num)
real (c_double ) , intent(out) :: forces_jastrow_en_l(3,nucl_num,walk_num)
integer(qmckl_exit_code) :: info
integer*8 :: i, a, k, nw, ii, m,l
double precision :: x, x1, kf, grad_c2
double precision :: denom, invdenom, invdenom2, f, f2, expk, invdist
double precision :: dx(4)
info = QMCKL_SUCCESS
if (context == QMCKL_NULL_CONTEXT) then
info = QMCKL_INVALID_CONTEXT
return
endif
if (walk_num <= 0) then
info = QMCKL_INVALID_ARG_2
return
endif
if (elec_num <= 0) then
info = QMCKL_INVALID_ARG_3
return
endif
if (nucl_num <= 0) then
info = QMCKL_INVALID_ARG_4
return
endif
if (aord_num < 0) then
info = QMCKL_INVALID_ARG_7
return
endif
do nw =1, walk_num
forces_jastrow_en_l(:,:,nw) = 0.0d0
do a = 1, nucl_num
do i = 1, elec_num
expk = dexp(rescale_factor_en(type_nucl_vector(a)+1) * en_distance(a,i,nw))
invdist = 1.d0 / en_distance(a,i,nw)
x = en_distance_rescaled(i,a,nw)
if(abs(x) < 1.d-12) continue
denom = 1.0d0 + a_vector(2, type_nucl_vector(a)+1) * x
invdenom = 1.0d0 / denom
invdenom2 = invdenom*invdenom
f = a_vector(1, type_nucl_vector(a)+1) * invdenom2
do m = 1, 4
dx(m) = en_distance_rescaled_gl(m,i,a,nw)
end do
grad_c2 = dx(1)*dx(1) + dx(2)*dx(2) + dx(3)*dx(3)
do m = 1, 3
forces_jastrow_en_l(m,a,nw) = forces_jastrow_en_l(m,a,nw) + f * dx(m) * (rescale_factor_en(type_nucl_vector(a)+1) * (2 *invdist - rescale_factor_en(type_nucl_vector(a)+1)) + 2*invdist*invdist)
forces_jastrow_en_l(m,a,nw) = forces_jastrow_en_l(m,a,nw) + 2.d0 * f * invdenom * a_vector(2, type_nucl_vector(a)+1) * dx(m) * dx(4)
forces_jastrow_en_l(m,a,nw) = forces_jastrow_en_l(m,a,nw) - 4.d0 * f * invdenom * a_vector(2, type_nucl_vector(a)+1) * rescale_factor_en(type_nucl_vector(a)+1) * dx(m)/expk
forces_jastrow_en_l(m,a,nw) = forces_jastrow_en_l(m,a,nw) - 6.d0 * f * invdenom * invdenom * a_vector(2, type_nucl_vector(a)+1) * a_vector(2, type_nucl_vector(a)+1) * grad_c2 * dx(m)
end do
kf = 2.d0
x1 = x
x = 1.d0
do k=2, aord_num
f = a_vector(k+1,type_nucl_vector(a)+1) * kf * x
do m = 1, 3
forces_jastrow_en_l(m,a,nw) = forces_jastrow_en_l(m,a,nw) &
- f * dx(m) * dx(4) * (kf-1.d0) &
- f / x1 * (kf-1.d0) * (kf-2.d0) * dx(m) /expk /expk &
+ f * x1 * rescale_factor_en(type_nucl_vector(a)+1) * dx(m) * dx(4) * expk &
+ f * x1 * 2 * dx(m) * invdist * invdist &
+ 2 * f * (kf-1.d0) * dx(m) * rescale_factor_en(type_nucl_vector(a)+1) / expk
end do
x = x*x1
kf = kf + 1.d0
end do
end do
end do
end do
end function qmckl_compute_forces_jastrow_en_l_docForce of single electron-nucleus Jastrow value
Calculate the force of the single-electron contribution ot the electron-nucleus Jastrow value. \[ \delta\partial_{\alpha,m} J_{en} = -\left( \frac{a_1 \partial_{i,m} \widetilde{R}_{i\alpha}^{\text{new}}}{(1+a_2 \widetilde{R}_{i\alpha}^{\text{new}} )^2} + \sum_{k=2}^{N_\text{aord}} a_k k {\widetilde{R}_{i\alpha}^{\text{new}}}^{k-1} \partial_{i,m} \widetilde{R}_{i\alpha}^{\text{new}} \right) + \left( \frac{a_1 \partial_{i,m} \widetilde{R}_{i\alpha}^{\text{old}}}{(1+a_2 \widetilde{R}_{i\alpha}^{\text{old}} )^2} + \sum_{k=2}^{N_\text{aord}} a_k k {\widetilde{R}_{i\alpha}^{\text{old}}}^{k-1} \partial_{i,m} \widetilde{R}_{i\alpha}^{\text{old}} \right) \]
Get
qmckl_exit_code
qmckl_get_forces_jastrow_single_en(qmckl_context context,
double* const forces_jastrow_single_en,
const int64_t size_max);Compute
| Variable | Type | In/Out | Description |
|---|---|---|---|
context |
qmckl_context |
in | Global state |
num |
int64_t |
in | Index of single electron |
walk_num |
int64_t |
in | Number of walkers |
elec_num |
int64_t |
in | Number of electrons |
nucl_num |
int64_t |
in | Number of nuclei |
type_nucl_num |
int64_t |
in | Number of unique nuclei |
type_nucl_vector |
int64_t[nucl_num] |
in | IDs of unique nuclei |
aord_num |
int64_t |
in | Number of coefficients |
a_vector |
double[type_nucl_num][aord_num+1] |
in | List of coefficients |
en_distance_rescaled |
double[walk_num][nucl_num][elec_num] |
in | Electron-nucleus rescaled distances |
en_distance_rescaled_gl |
double[walk_num][nucl_num][elec_num][4] |
in | Electron-nucleus rescaled distance derivatives |
en_rescaled_single |
double[walk_num][nucl_num] |
in | Electron-nucleus rescaled single distances |
en_rescaled_single_gl |
double[walk_num][nucl_num][4] |
in | Electron-nucleus rescaled single distance derivatives |
forces_jastrow_single_en |
double[walk_num][nucl_num][3] |
out | Single electron-nucleus forces |
function qmckl_compute_forces_jastrow_single_en_doc( &
context, num_in, walk_num, elec_num, nucl_num, type_nucl_num, &
type_nucl_vector, aord_num, a_vector, &
en_distance_rescaled, en_distance_rescaled_gl, en_rescaled_single, en_rescaled_single_gl, forces_jastrow_single_en) &
bind(C) result(info)
use qmckl
implicit none
integer (qmckl_context), intent(in), value :: context
integer (c_int64_t) , intent(in) , value :: num_in
integer (c_int64_t) , intent(in) , value :: walk_num
integer (c_int64_t) , intent(in) , value :: elec_num
integer (c_int64_t) , intent(in) , value :: nucl_num
integer (c_int64_t) , intent(in) , value :: type_nucl_num
integer (c_int64_t) , intent(in) :: type_nucl_vector(nucl_num)
integer (c_int64_t) , intent(in) , value :: aord_num
real (c_double ) , intent(in) :: a_vector(aord_num+1,type_nucl_num)
real (c_double ) , intent(in) :: en_distance_rescaled(elec_num,nucl_num,walk_num)
real (c_double ) , intent(in) :: en_distance_rescaled_gl(4, elec_num,nucl_num,walk_num)
real (c_double ) , intent(in) :: en_rescaled_single(nucl_num,walk_num)
real (c_double ) , intent(in) :: en_rescaled_single_gl(4, nucl_num,walk_num)
real (c_double ) , intent(out) :: forces_jastrow_single_en(3,nucl_num,walk_num)
integer(qmckl_exit_code) :: info
integer*8 :: i, a, k, nw, ii, num
double precision :: x, x1, kf, x_old, x1_old
double precision :: denom, invdenom, invdenom2, f
double precision :: denom_old, invdenom_old, invdenom2_old, f_old
double precision :: dx(3), dx_old(3)
num = num_in + 1
info = QMCKL_SUCCESS
if (context == QMCKL_NULL_CONTEXT) then
info = QMCKL_INVALID_CONTEXT
return
endif
if (walk_num <= 0) then
info = QMCKL_INVALID_ARG_3
return
endif
if (elec_num <= 0) then
info = QMCKL_INVALID_ARG_4
return
endif
if (nucl_num <= 0) then
info = QMCKL_INVALID_ARG_5
return
endif
if (aord_num < 0) then
info = QMCKL_INVALID_ARG_8
return
endif
do nw =1, walk_num
forces_jastrow_single_en(:,:,nw) = 0.0d0
do a = 1, nucl_num
x_old = en_distance_rescaled(num,a,nw)
x = en_rescaled_single(a,nw)
denom = 1.0d0 + a_vector(2, type_nucl_vector(a)+1) * x
invdenom = 1.0d0 / denom
invdenom2 = invdenom*invdenom
denom_old = 1.0d0 + a_vector(2, type_nucl_vector(a)+1) * x_old
invdenom_old = 1.0d0 / denom_old
invdenom2_old = invdenom_old*invdenom_old
dx(1) = -en_rescaled_single_gl(1,a,nw)
dx(2) = -en_rescaled_single_gl(2,a,nw)
dx(3) = -en_rescaled_single_gl(3,a,nw)
dx_old(1) = -en_distance_rescaled_gl(1,num,a,nw)
dx_old(2) = -en_distance_rescaled_gl(2,num,a,nw)
dx_old(3) = -en_distance_rescaled_gl(3,num,a,nw)
f = a_vector(1, type_nucl_vector(a)+1) * invdenom2
f_old = a_vector(1, type_nucl_vector(a)+1) * invdenom2_old
forces_jastrow_single_en(1,a,nw) = forces_jastrow_single_en(1,a,nw) + f * dx(1) - f_old * dx_old(1)
forces_jastrow_single_en(2,a,nw) = forces_jastrow_single_en(2,a,nw) + f * dx(2) - f_old * dx_old(2)
forces_jastrow_single_en(3,a,nw) = forces_jastrow_single_en(3,a,nw) + f * dx(3) - f_old * dx_old(3)
kf = 2.d0
x1 = x
x = 1.d0
x1_old = x_old
x_old = 1.d0
do k=2, aord_num
f = a_vector(k+1,type_nucl_vector(a)+1) * kf * x
f_old = a_vector(k+1,type_nucl_vector(a)+1) * kf * x_old
forces_jastrow_single_en(1,a,nw) = forces_jastrow_single_en(1,a,nw) + f * x1 * dx(1) - f_old * x1_old * dx_old(1)
forces_jastrow_single_en(2,a,nw) = forces_jastrow_single_en(2,a,nw) + f * x1 * dx(2) - f_old * x1_old * dx_old(2)
forces_jastrow_single_en(3,a,nw) = forces_jastrow_single_en(3,a,nw) + f * x1 * dx(3) - f_old * x1_old * dx_old(3)
x = x*x1
x_old = x_old*x1_old
kf = kf + 1.d0
end do
end do
end do
end function qmckl_compute_forces_jastrow_single_en_docElectron-electron-nucleus Jastrow
Force of tmp_c matrix
Calculates the force of the tmp_c matrix. This is a required component to calculate the force on the 3-body Jastrow. \[ \partial_{\alpha,m} P_{i,\alpha,k,l} = \sum_j \widetilde{r}_{i,j,k} \partial_{\alpha,m}\widetilde{R}_{j,\alpha,l} = -\sum_j \widetilde{r}_{i,j,k} \partial_{j,m}\widetilde{R}_{j,\alpha,l} \]
Get
qmckl_exit_code
qmckl_get_forces_tmp_c(qmckl_context context,
double* const forces_tmp_c,
const int64_t size_max);Compute
| Variable | Type | In/Out | Description |
|---|---|---|---|
context |
qmckl_context |
in | Global state |
walk_num |
int64_t |
in | Number of walkers |
elec_num |
int64_t |
in | Number of electrons |
nucl_num |
int64_t |
in | Number of nuclei |
cord_num |
int64_t |
in | order of polynomials |
een_rescaled_e |
double[walk_num][0:cord_num][elec_num][elec_num] |
in | Electron-nucleus rescaled |
een_rescaled_n_gl |
double[walk_num][0:cord_num][nucl_num][4][elec_num] |
in | Electron-nucleus rescaled derivatives |
forces_tmp_c |
double[walk_num][0:cord_num-1][0:cord_num][nucl_num][4][elec_num] |
out | Force on the tmp_c matrix |
integer(qmckl_exit_code) function qmckl_compute_forces_tmp_c( &
context, walk_num, elec_num, nucl_num, cord_num,&
een_rescaled_e, een_rescaled_n_gl, forces_tmp_c) &
result(info) bind(C)
use, intrinsic :: iso_c_binding
use qmckl
implicit none
integer(qmckl_context), intent(in) :: context
integer (c_int64_t) , intent(in), value :: walk_num, elec_num, cord_num, nucl_num
real (c_double ) , intent(in) :: een_rescaled_e(elec_num, elec_num, 0:cord_num, walk_num)
real (c_double ) , intent(in) :: een_rescaled_n_gl(elec_num, 4, nucl_num, 0:cord_num, walk_num)
real (c_double ) , intent(out) :: forces_tmp_c(elec_num, 4, nucl_num,0:cord_num, 0:cord_num-1, walk_num)
integer*8 :: nw, i
integer*8 :: l, m, k, a,j
info = QMCKL_SUCCESS
if (context == QMCKL_NULL_CONTEXT) info = QMCKL_INVALID_CONTEXT
if (walk_num <= 0) info = QMCKL_INVALID_ARG_2
if (elec_num <= 0) info = QMCKL_INVALID_ARG_3
if (nucl_num <= 0) info = QMCKL_INVALID_ARG_4
if (cord_num < 0) info = QMCKL_INVALID_ARG_5
if (info /= QMCKL_SUCCESS) return
do nw=1, walk_num
do i=0, cord_num-1
info = qmckl_dgemm(context,'N','N',elec_num*1_8,&
nucl_num*(cord_num+1)*4_8, elec_num*1_8, -1.0d0, &
een_rescaled_e(1,1,i,nw),1_8*elec_num, &
een_rescaled_n_gl(1,1,1,0,nw),elec_num*1_8, &
0.0d0, &
forces_tmp_c(1,1,1,0,i,nw),1_8*elec_num)
end do
end do
end function qmckl_compute_forces_tmp_cForce of dtmp_c matrix
Calculates the force of the derivative of the tmp_c matrix: the dtmp_c matrix. \[ \partial_{\alpha,m} \partial_{i,n} P_{i,\alpha,k,l} = \sum_j \partial_{i,n} \widetilde{r}_{i,j,k} \partial_{\alpha,m}\widetilde{R}_{j,\alpha,l} = -\sum_j \partial_{i,n}\widetilde{r}_{i,j,k} \partial_{j,m}\widetilde{R}_{j,\alpha,l} \]
Get
qmckl_exit_code
qmckl_get_forces_dtmp_c(qmckl_context context,
double* const forces_dtmp_c,
const int64_t size_max);Compute
| Variable | Type | In/Out | Description |
|---|---|---|---|
context |
qmckl_context |
in | Global state |
walk_num |
int64_t |
in | Number of walkers |
elec_num |
int64_t |
in | Number of electrons |
nucl_num |
int64_t |
in | Number of nuclei |
cord_num |
int64_t |
in | order of polynomials |
een_rescaled_e_gl |
double[walk_num][0:cord_num][elec_num][4][elec_num] |
in | Electron-nucleus rescaled |
een_rescaled_n_gl |
double[walk_num][0:cord_num][nucl_num][4][elec_num] |
in | Electron-nucleus rescaled derivatives |
forces_dtmp_c |
double[walk_num][0:cord_num-1][0:cord_num][4][nucl_num][4][elec_num] |
out | Force of dtmp_c matrix |
integer(qmckl_exit_code) function qmckl_compute_forces_dtmp_c_doc( &
context, walk_num, elec_num, nucl_num, cord_num,&
een_rescaled_e_gl, een_rescaled_n_gl, forces_dtmp_c) &
result(info) bind(C)
use, intrinsic :: iso_c_binding
use qmckl
implicit none
integer(qmckl_context), intent(in) :: context
integer (c_int64_t) , intent(in), value :: walk_num, elec_num, cord_num, nucl_num
real (c_double ) , intent(in) :: een_rescaled_e_gl(elec_num, 4, elec_num, 0:cord_num, walk_num)
real (c_double ) , intent(in) :: een_rescaled_n_gl(elec_num, 4, nucl_num, 0:cord_num, walk_num)
real (c_double ) , intent(out) :: forces_dtmp_c(elec_num, 4, nucl_num,4,0:cord_num, 0:cord_num-1, walk_num)
integer*8 :: nw, i, k
integer*8 :: l, m, a,j, kk
info = QMCKL_SUCCESS
if (context == QMCKL_NULL_CONTEXT) info = QMCKL_INVALID_CONTEXT
if (walk_num <= 0) info = QMCKL_INVALID_ARG_2
if (elec_num <= 0) info = QMCKL_INVALID_ARG_3
if (nucl_num <= 0) info = QMCKL_INVALID_ARG_4
if (cord_num < 0) info = QMCKL_INVALID_ARG_5
if (info /= QMCKL_SUCCESS) return
do nw = 1, walk_num
do l = 0, cord_num-1
do m = 1, cord_num
do k = 1, 4
do a = 1, nucl_num
do kk = 1, 4
do i = 1, elec_num
forces_dtmp_c(i,kk,a,k,m,l,nw) = 0.d0
do j = 1, elec_num
forces_dtmp_c(i,kk,a,k,m,l,nw) = forces_dtmp_c(i,kk,a,k,m,l,nw) - &
een_rescaled_e_gl(i,kk,j,l,nw) * een_rescaled_n_gl(j,k,a,m,nw)
end do
end do
end do
end do
end do
end do
end do
end do
end function qmckl_compute_forces_dtmp_c_docinteger(qmckl_exit_code) function qmckl_compute_forces_dtmp_c_hpc( &
context, walk_num, elec_num, nucl_num, cord_num,&
een_rescaled_e_gl, een_rescaled_n_gl, forces_dtmp_c) &
result(info) bind(C)
use, intrinsic :: iso_c_binding
use qmckl
implicit none
integer(qmckl_context), intent(in) :: context
integer (c_int64_t) , intent(in), value :: walk_num, elec_num, cord_num, nucl_num
real (c_double ) , intent(in) :: een_rescaled_e_gl(elec_num, 4, elec_num, 0:cord_num, walk_num)
real (c_double ) , intent(in) :: een_rescaled_n_gl(elec_num, 4, nucl_num, 0:cord_num, walk_num)
real (c_double ) , intent(out) :: forces_dtmp_c(elec_num, 4, nucl_num,4,0:cord_num, 0:cord_num-1, walk_num)
integer*8 :: nw, i, k
integer*8 :: l, m, a,j, kk
double precision, allocatable :: tmp(:,:,:,:)
info = QMCKL_SUCCESS
if (context == QMCKL_NULL_CONTEXT) info = QMCKL_INVALID_CONTEXT
if (walk_num <= 0) info = QMCKL_INVALID_ARG_2
if (elec_num <= 0) info = QMCKL_INVALID_ARG_3
if (nucl_num <= 0) info = QMCKL_INVALID_ARG_4
if (cord_num < 0) info = QMCKL_INVALID_ARG_5
if (info /= QMCKL_SUCCESS) return
allocate(tmp(elec_num, 4, 4, nucl_num))
do nw = 1, walk_num
do l = 0, cord_num-1
do m = 1, cord_num
call dgemm('N','N', elec_num*4, 4*nucl_num, elec_num, -1.d0, &
een_rescaled_e_gl(1,1,1,l,nw), elec_num*4, &
een_rescaled_n_gl(1,1,1,m,nw), elec_num, 0.d0, &
tmp, elec_num*4)
do k = 1, 4
do a = 1, nucl_num
forces_dtmp_c(:,:,a,k,m,l,nw) = tmp(:,:,k,a)
end do
end do
end do
end do
end do
deallocate(tmp)
end function qmckl_compute_forces_dtmp_c_hpcForce of electron-electron-nucleus Jastrow value
Calculates the force of the eleectron-electorn-nucleus Jastrow value. \[ \partial_{\alpha,m}J_{een} = \sum_{p=2}^{N_\text{nord}} \sum_{k=0}^{p-1} \sum_{l=0}^{p-k-2\delta_{k,0}} c_{l,k,p,\alpha} \sum_{i=1}^{N_\text{elec}} \left(\widetilde{R}_{i\alpha}^{(p-k+l)/2} \partial_{\alpha,m}P_{i\alpha,k,(p-k-l)/2} + \partial_{\alpha,m}\widetilde{R}_{i\alpha}^{(p-k+l)/2} P_{i\alpha,k,(p-k-l)/2}\right) \]
Get
qmckl_exit_code
qmckl_get_forces_jastrow_een(qmckl_context context,
double* const forces_jastrow_een,
const int64_t size_max);interface
integer(qmckl_exit_code) function qmckl_get_forces_jastrow_een (context, &
forces_jastrow_een, size_max) bind(C)
use, intrinsic :: iso_c_binding
import
implicit none
integer (qmckl_context) , intent(in), value :: context
integer(c_int64_t), intent(in), value :: size_max
real(c_double), intent(out) :: forces_jastrow_een(size_max)
end function qmckl_get_forces_jastrow_een
end interfaceCompute
| Variable | Type | In/Out | Description |
|---|---|---|---|
context |
qmckl_context |
in | Global state |
walk_num |
int64_t |
in | Number of walkers |
elec_num |
int64_t |
in | Number of electrons |
nucl_num |
int64_t |
in | Number of nuclei |
cord_num |
int64_t |
in | order of polynomials |
dim_c_vector |
int64_t |
in | dimension of full coefficient vector |
c_vector_full |
double[dim_c_vector][nucl_num] |
in | full coefficient vector |
lkpm_combined_index |
int64_t[4][dim_c_vector] |
in | combined indices |
een_rescaled_n |
double[walk_num][0:cord_num][nucl_num][elec_num] |
in | Electron-nucleus rescaled |
een_rescaled_n_gl |
double[walk_num][0:cord_num][nucl_num][4][elec_num] |
in | Electron-nucleus rescaled derivatives |
tmp_c |
double[walk_num][0:cord_num-1][0:cord_num][nucl_num][elec_num] |
in | tmp_c matrix |
forces_tmp_c |
double[walk_num][0:cord_num-1][0:cord_num][nucl_num][4][elec_num] |
in | Force of tmp_c matrix |
forces_jastrow_een |
double[walk_num][nucl_num][3] |
out | Force of electron-electron-nucleus Jastrow value |
integer(qmckl_exit_code) function qmckl_compute_forces_jastrow_een( &
context, walk_num, elec_num, nucl_num, cord_num,&
dim_c_vector, c_vector_full, lkpm_combined_index, &
een_rescaled_n, een_rescaled_n_gl, tmp_c, forces_tmp_c,forces_jastrow_een) &
result(info) bind(C)
use, intrinsic :: iso_c_binding
use qmckl
implicit none
integer(qmckl_context), intent(in) :: context
integer (c_int64_t) , intent(in), value :: walk_num, elec_num, cord_num, nucl_num, dim_c_vector
integer (c_int64_t) , intent(in) :: lkpm_combined_index(dim_c_vector,4)
real (c_double ) , intent(in) :: c_vector_full(nucl_num, dim_c_vector)
real (c_double ) , intent(in) :: een_rescaled_n(elec_num, nucl_num, 0:cord_num, walk_num)
real (c_double ) , intent(in) :: een_rescaled_n_gl(elec_num, 4, nucl_num, 0:cord_num, walk_num)
real (c_double ) , intent(in) :: tmp_c(elec_num, nucl_num,0:cord_num, 0:cord_num-1, walk_num)
real (c_double ) , intent(in) :: forces_tmp_c(elec_num,4, nucl_num,0:cord_num, 0:cord_num-1, walk_num)
real (c_double ) , intent(out) :: forces_jastrow_een(3, nucl_num, walk_num)
integer*8 :: i, a, j, l, k, p, m, n, nw, ii
double precision :: accu, accu2, cn
info = QMCKL_SUCCESS
if (context == QMCKL_NULL_CONTEXT) info = QMCKL_INVALID_CONTEXT
if (walk_num <= 0) info = QMCKL_INVALID_ARG_2
if (elec_num <= 0) info = QMCKL_INVALID_ARG_3
if (nucl_num <= 0) info = QMCKL_INVALID_ARG_4
if (cord_num < 0) info = QMCKL_INVALID_ARG_5
if (info /= QMCKL_SUCCESS) return
forces_jastrow_een = 0.d0
do nw =1, walk_num
do n = 1, dim_c_vector
l = lkpm_combined_index(n, 1)
k = lkpm_combined_index(n, 2)
p = lkpm_combined_index(n, 3)
m = lkpm_combined_index(n, 4)
do a = 1, nucl_num
cn = c_vector_full(a, n)
if(cn == 0.d0) cycle
do j = 1, elec_num
do ii = 1, 3
accu = een_rescaled_n(j,a,m,nw) * forces_tmp_c(j,ii,a,m+l,k,nw) &
- een_rescaled_n_gl(j,ii,a,m,nw) * tmp_c(j,a,m+l,k,nw)
forces_jastrow_een(ii, a, nw) = forces_jastrow_een(ii, a, nw) + accu * cn
end do
end do
end do
end do
end do
end function qmckl_compute_forces_jastrow_eenForce of derivatives of electron-nucleus rescaled distance
Calculates the force of the derivatives of the electron-nucleus rescaled distance.
\begin{eqnarray} \partial_{\alpha,m}\partial_{i,n} \widetilde{R}_{i\alpha} =& \partial_{\alpha,m} \left( -\frac{r_{i,n} - R_{\alpha,n}}{R_{i\alpha}} \kappa l e^{-\kappa l R_{i\alpha}}\right)\\ =& - \frac{(r_{i,n} - R_{\alpha,n})(r_{i,m} - R_{\alpha,m})}{R_{i\alpha}^3}l\kappa e^{-\kappa l R_{i\alpha}} - \frac{(r_{i,n} - R_{\alpha,n})(r_{i,m} - R_{\alpha,m})}{R_{i\alpha}^2} \kappa^2 l^2 e^{-\kappa l R_{i\alpha}} + \delta_{n,m} \frac{1}{r}\kappa l e^{-\kappa l R_{i\alpha}}\\ \partial_{\alpha,m}\nabla^2 \widetilde{R}_{i\alpha} =& \partial_{\alpha,m} \left( \kappa l \left( \kappa l - \frac{2}{R_{i\alpha}}\right) e^{-\kappa l R_{i\alpha}}\right)\\ =&-2\kappa l \frac{r_{i,m} - R_{\alpha,m}}{R_{i\alpha}^3}e^{-\kappa l R_{i\alpha}} + \kappa^2 l^2 \left(\kappa l - \frac{2}{R_{i\alpha}} \right) \frac{r_{i,m}-R_{\alpha,m}}{R_{i\alpha}} e^{-\kappa l R_{i\alpha}} \end{eqnarray}Get
qmckl_exit_code
qmckl_get_forces_een_rescaled_n_gl(qmckl_context context,
double* const forces_een_n,
const int64_t size_max);Compute
| Variable | Type | In/Out | Description |
|---|---|---|---|
context |
qmckl_context |
in | Global state |
walk_num |
int64_t |
in | Number of walkers |
elec_num |
int64_t |
in | Number of electrons |
nucl_num |
int64_t |
in | Number of atoms |
type_nucl_num |
int64_t |
in | Number of atom types |
type_nucl_vector |
int64_t[nucl_num] |
in | Types of atoms |
cord_num |
int64_t |
in | Order of polynomials |
rescale_factor_en |
double[nucl_num] |
in | Factor to rescale ee distances |
en_distance |
double[walk_num][elec_num][nucl_num] |
in | Electron-nucleus distances |
een_rescaled_n |
double[walk_num][0:cord_num][nucl_num][elec_num] |
in | Electron-nucleus rescaled distances |
een_rescaled_n_gl |
double[walk_num][0:cord_num][nucl_num][4][elec_num] |
in | Electron-nucleus rescaled distances derivativies |
forces_een_n |
double[walk_num][0:cord_num][3][nucl_num][4][elec_num] |
out | Force of electron-nucleus rescaled distances derivatives |
integer(qmckl_exit_code) function qmckl_compute_forces_een_rescaled_n_gl( &
context, walk_num, elec_num, nucl_num, type_nucl_num, type_nucl_vector, &
cord_num, rescale_factor_en, &
en_distance, een_rescaled_n, een_rescaled_n_gl,forces_een_n) &
result(info) bind(C)
use, intrinsic :: iso_c_binding
use qmckl
implicit none
integer(qmckl_context), intent(in) :: context
integer (c_int64_t) , intent(in),value :: walk_num, elec_num, nucl_num, type_nucl_num, cord_num
integer (c_int64_t) , intent(in) :: type_nucl_vector(nucl_num)
real (c_double ) , intent(in) :: rescale_factor_en(type_nucl_num)
real (c_double ) , intent(in) :: en_distance(nucl_num,elec_num,walk_num)
real (c_double ) , intent(in) :: een_rescaled_n(elec_num,nucl_num,0:cord_num,walk_num)
real (c_double ) , intent(in) :: een_rescaled_n_gl(elec_num,4,nucl_num,0:cord_num,walk_num)
real (c_double ) , intent(out) :: forces_een_n(elec_num,4,nucl_num,3,0:cord_num,walk_num)
double precision :: x, ria_inv, kappa_l, temp
integer*8 :: i, a, k, l, nw, m, n
info = QMCKL_SUCCESS
if (context == QMCKL_NULL_CONTEXT) then
info = QMCKL_INVALID_CONTEXT
return
endif
if (walk_num <= 0) then
info = QMCKL_INVALID_ARG_2
return
endif
if (elec_num <= 0) then
info = QMCKL_INVALID_ARG_3
return
endif
if (nucl_num <= 0) then
info = QMCKL_INVALID_ARG_4
return
endif
if (cord_num < 0) then
info = QMCKL_INVALID_ARG_5
return
endif
!forces_een_n = 0.0d0
!do nw = 1, walk_num
! do l = 0, cord_num
! do a = 1, nucl_num
! kappa_l = dble(l)*rescale_factor_en(type_nucl_vector(a)+1)
! do i = 1, elec_num
! ria_inv = 1.0d0 / en_distance(a,i,nw)
! do n = 1, 3
! do m = 1, 3
! if (m == n) then
! forces_een_n(i,m,a,n,l,nw) = forces_een_n(i,m,a,n,l,nw) + &
! kappa_l*een_rescaled_n(i,a,l,nw) * ria_inv
! end if
! temp = een_rescaled_n_gl(i,m,a,l,nw) * een_rescaled_n_gl(i,n,a,l,nw) / een_rescaled_n(i,a,l,nw)
! forces_een_n(i,m,a,n,l,nw) = forces_een_n(i,m,a,n,l,nw) - &
! temp * ria_inv / kappa_l - temp
! end do
! forces_een_n(i,4,a,n,l,nw) = forces_een_n(i,4,a,n,l,nw) + &
! (2.0d0 * ria_inv * ria_inv &
! - een_rescaled_n_gl(i,4,a,l,nw)/een_rescaled_n(i,a,l,nw)) * &
! een_rescaled_n_gl(i,n,a,l,nw)
! end do
! end do
! end do
! end do
!end do
forces_een_n = 0.0d0
do nw = 1, walk_num
do i = 1, elec_num
do a = 1, nucl_num
do l = 0, cord_num
kappa_l = dble(l)*rescale_factor_en(type_nucl_vector(a)+1)
do m = 1, 4
do n = 1, 3
if (l == 0) then
forces_een_n(i,m,a,n,l,nw) = 0.0d0
else
if (m == n) then
forces_een_n(i,m,a,n,l,nw) = forces_een_n(i,m,a,n,l,nw) + &
kappa_l*een_rescaled_n(i,a,l,nw)/en_distance(a,i,nw)
end if
if (m < 4) then
forces_een_n(i,m,a,n,l,nw) = forces_een_n(i,m,a,n,l,nw) - &
een_rescaled_n_gl(i,m,a,l,nw) * een_rescaled_n_gl(i,n,a,l,nw) / &
(kappa_l*een_rescaled_n(i,a,l,nw)*en_distance(a,i,nw)) - &
een_rescaled_n_gl(i,m,a,l,nw) * &
een_rescaled_n_gl(i,n,a,l,nw)/een_rescaled_n(i,a,l,nw)
else
forces_een_n(i,m,a,n,l,nw) = forces_een_n(i,m,a,n,l,nw) + &
2.0d0 * een_rescaled_n_gl(i,n,a,l,nw) / &
(en_distance(a,i,nw)*en_distance(a,i,nw)) - &
een_rescaled_n_gl(i,m,a,l,nw) * &
een_rescaled_n_gl(i,n,a,l,nw)/een_rescaled_n(i,a,l,nw)
end if
end if
end do
end do
end do
end do
end do
end do
end function qmckl_compute_forces_een_rescaled_n_glForce of electron-electron-nucleus Jastrow gradient
Calculates the force of the electron-electron-nucleus Jastrow gradient (and not the Laplacian).
\begin{eqnarray} \partial_{\alpha,m} \partial_{i,n}J_{een} =& \partial_{\alpha,m} \sum_{p=2}^{N_\text{nord}} \sum_{k=0}^{p-1} \sum_{l=0}^{p-k-2\delta_{k,0}} c_{l,k,p,\alpha} \left(\partial_{i,n}\widetilde{R}_{i\alpha}^{(p-k+l)/2} P_{i\alpha,k,(p-k-l)/2} + \partial_{i,n}\widetilde{R}_{i\alpha}^{(p-k-l)/2} P_{i\alpha,k,(p-k+l)/2} + \widetilde{R}_{i\alpha}^{(p-k+l)/2} \partial_{i,n} P_{i\alpha,k,(p-k-l)/2} + \widetilde{R}_{i\alpha}^{(p-k-l)/2} \partial_{i,n} P_{i\alpha,k,(p-k+l)/2} \right)\\ =& \sum_{p=2}^{N_\text{nord}} \sum_{k=0}^{p-1} \sum_{l=0}^{p-k-2\delta_{k,0}} c_{l,k,p,\alpha} \left(\partial_{\alpha,m}\partial_{i,n}\widetilde{R}_{i\alpha}^{(p-k+l)/2} P_{i\alpha,k,(p-k-l)/2} + \partial_{\alpha,m}\partial_{i,n}\widetilde{R}_{i\alpha}^{(p-k-l)/2} P_{i\alpha,k,(p-k+l)/2} + \partial_{\alpha,m}\widetilde{R}_{i\alpha}^{(p-k+l)/2} \partial_{i,n} P_{i\alpha,k,(p-k-l)/2} + \partial_{\alpha,m}\widetilde{R}_{i\alpha}^{(p-k-l)/2} \partial_{i,n} P_{i\alpha,k,(p-k+l)/2} \right.\\ &+ \left.\partial_{i,n}\widetilde{R}_{i\alpha}^{(p-k+l)/2} \partial_{\alpha,m}P_{i\alpha,k,(p-k-l)/2} + \partial_{i,n}\widetilde{R}_{i\alpha}^{(p-k-l)/2} \partial_{\alpha,m}P_{i\alpha,k,(p-k+l)/2} + \widetilde{R}_{i\alpha}^{(p-k+l)/2} \partial_{\alpha,m}\partial_{i,n} P_{i\alpha,k,(p-k-l)/2} + \widetilde{R}_{i\alpha}^{(p-k-l)/2} \partial_{\alpha,m}\partial_{i,n} P_{i\alpha,k,(p-k+l)/2}\right)\\ =& \sum_{p=2}^{N_\text{nord}} \sum_{k=0}^{p-1} \sum_{l=0}^{p-k-2\delta_{k,0}} c_{l,k,p,\alpha} \left(\partial_{\alpha,m}\partial_{i,n}\widetilde{R}_{i\alpha}^{(p-k+l)/2} P_{i\alpha,k,(p-k-l)/2} + \partial_{\alpha,m}\partial_{i,n}\widetilde{R}_{i\alpha}^{(p-k-l)/2} P_{i\alpha,k,(p-k+l)/2} - \partial_{i,m}\widetilde{R}_{i\alpha}^{(p-k+l)/2} \partial_{i,n} P_{i\alpha,k,(p-k-l)/2} - \partial_{i,m}\widetilde{R}_{i\alpha}^{(p-k-l)/2} \partial_{i,n} P_{i\alpha,k,(p-k+l)/2} \right.\\ &+ \left.\partial_{i,n}\widetilde{R}_{i\alpha}^{(p-k+l)/2} \partial_{\alpha,m}P_{i\alpha,k,(p-k-l)/2} + \partial_{i,n}\widetilde{R}_{i\alpha}^{(p-k-l)/2} \partial_{\alpha,m}P_{i\alpha,k,(p-k+l)/2} + \widetilde{R}_{i\alpha}^{(p-k+l)/2} \partial_{\alpha,m}\partial_{i,n} P_{i\alpha,k,(p-k-l)/2} + \widetilde{R}_{i\alpha}^{(p-k-l)/2} \partial_{\alpha,m}\partial_{i,n} P_{i\alpha,k,(p-k+l)/2}\right)\\ \end{eqnarray}Get
qmckl_exit_code
qmckl_get_forces_jastrow_een_g(qmckl_context context,
double* const forces_jastrow_een_g,
const int64_t size_max);interface
integer(qmckl_exit_code) function qmckl_get_forces_jastrow_een_g (context, &
forces_jastrow_een_g, size_max) bind(C)
use, intrinsic :: iso_c_binding
import
implicit none
integer (qmckl_context) , intent(in), value :: context
integer(c_int64_t), intent(in), value :: size_max
real(c_double), intent(out) :: forces_jastrow_een_g(size_max)
end function qmckl_get_forces_jastrow_een_g
end interface#
Compute
| Variable | Type | In/Out | Description |
|---|---|---|---|
context |
qmckl_context |
in | Global state |
walk_num |
int64_t |
in | Number of walkers |
elec_num |
int64_t |
in | Number of electrons |
nucl_num |
int64_t |
in | Number of nuclei |
cord_num |
int64_t |
in | order of polynomials |
dim_c_vector |
int64_t |
in | dimension of full coefficient vector |
c_vector_full |
double[dim_c_vector][nucl_num] |
in | full coefficient vector |
lkpm_combined_index |
int64_t[4][dim_c_vector] |
in | combined indices |
en_distance |
double[elec_num][nucl_num] |
in | Electron-nucleus distance |
tmp_c |
double[walk_num][0:cord_num-1][0:cord_num][nucl_num][elec_num] |
in | tmp_c matroix |
dtmp_c |
double[walk_num][0:cord_num-1][0:cord_num][nucl_num][4][elec_num] |
in | dtmp_c matrix |
forces_tmp_c |
double[walk_num][0:cord_num-1][0:cord_num][nucl_num][4][elec_num] |
in | Force of tmp_c matrix |
forces_dtmp_c |
double[walk_num][0:cord_num-1][0:cord_num][4][nucl_num][4][elec_num] |
in | Force of dtmp_c matrix |
forces_een_n |
double[walk_num][0:cord_num][3][nucl_num][4][elec_num] |
in | Force of derivatives of electron-nucleus rescaled factor |
een_rescaled_n |
double[walk_num][0:cord_num][nucl_num][elec_num] |
in | Electron-nucleus rescaled factor |
een_rescaled_n_gl |
double[walk_num][0:cord_num][nucl_num][4][elec_num] |
in | Derivative of electron-nucleus rescaled factor |
forces_jastrow_een_g |
double[walk_num][3][nucl_num][3][elec_num] |
out | Force of the electron-electron-nucleus Jastrow gradient |
integer(qmckl_exit_code) function qmckl_compute_forces_jastrow_een_g( &
context, walk_num, elec_num, nucl_num, &
cord_num, dim_c_vector, c_vector_full, lkpm_combined_index, &
en_distance, tmp_c, dtmp_c, forces_tmp_c, forces_dtmp_c, forces_een_n, een_rescaled_n, &
een_rescaled_n_gl, forces_jastrow_een_g)&
result(info) bind(C)
use, intrinsic :: iso_c_binding
use qmckl
implicit none
integer(qmckl_context), intent(in) :: context
integer (c_int64_t) , intent(in),value :: walk_num, elec_num, cord_num, nucl_num, dim_c_vector
integer (c_int64_t) , intent(in) :: lkpm_combined_index(dim_c_vector,4)
real (c_double ) , intent(in) :: c_vector_full(nucl_num, dim_c_vector)
real (c_double ) , intent(in) :: en_distance(nucl_num, elec_num)
real (c_double ) , intent(in) :: tmp_c(elec_num, nucl_num,0:cord_num, 0:cord_num-1, walk_num)
real (c_double ) , intent(in) :: dtmp_c(elec_num, 4, nucl_num,0:cord_num, 0:cord_num-1, walk_num)
real (c_double ) , intent(in) :: forces_tmp_c(elec_num, 4,nucl_num,0:cord_num, 0:cord_num-1, walk_num)
real (c_double ) , intent(in) :: forces_dtmp_c(elec_num, 4, nucl_num,4,0:cord_num, 0:cord_num-1, walk_num)
real (c_double ) , intent(in) :: forces_een_n(elec_num, 4, nucl_num, 3, 0:cord_num, walk_num)
real (c_double ) , intent(in) :: een_rescaled_n(elec_num, nucl_num, 0:cord_num, walk_num)
real (c_double ) , intent(in) :: een_rescaled_n_gl(elec_num, 4, nucl_num, 0:cord_num, walk_num)
real (c_double ) , intent(out) :: forces_jastrow_een_g(elec_num,3,nucl_num,3,walk_num)
integer*8 :: i, a, j, l, k, m, n, nw, ii, jj
double precision :: accu, accu2, cn
info = QMCKL_SUCCESS
if (context == QMCKL_NULL_CONTEXT) info = QMCKL_INVALID_CONTEXT
if (walk_num <= 0) info = QMCKL_INVALID_ARG_2
if (elec_num <= 0) info = QMCKL_INVALID_ARG_3
if (nucl_num <= 0) info = QMCKL_INVALID_ARG_4
if (cord_num < 0) info = QMCKL_INVALID_ARG_5
if (info /= QMCKL_SUCCESS) return
if (cord_num == 0) return
forces_jastrow_een_g = 0.0d0
do nw =1, walk_num
do n = 1, dim_c_vector
l = lkpm_combined_index(n, 1)
k = lkpm_combined_index(n, 2)
m = lkpm_combined_index(n, 4)
do a = 1, nucl_num
cn = c_vector_full(a, n)
if(cn == 0.d0) cycle
do ii = 1, 3
do i = 1, elec_num
do jj = 1, 3
forces_jastrow_een_g(i, ii, a, jj, nw) = forces_jastrow_een_g(i, ii, a, jj, nw) + (&
tmp_c(i,a, m, k,nw) * forces_een_n(i,ii,a,jj ,m+l,nw) &
+ forces_tmp_c(i,jj,a, m, k,nw) * een_rescaled_n_gl(i,ii,a,m+l,nw) &
+ tmp_c(i,a, m+l,k,nw) * forces_een_n(i,ii,a,jj, m, nw) &
+ forces_tmp_c(i,jj,a, m+l,k,nw) * een_rescaled_n_gl(i,ii,a,m, nw) &
- dtmp_c(i,ii,a, m, k,nw) * een_rescaled_n_gl(i,jj,a,m+l,nw) &
+ forces_dtmp_c(i,ii,a,jj,m, k,nw) * een_rescaled_n(i,a, m+l,nw) &
- dtmp_c(i,ii,a, m+l,k,nw) * een_rescaled_n_gl(i,jj,a,m, nw) &
+ forces_dtmp_c(i,ii,a,jj,m+l,k,nw) * een_rescaled_n(i,a, m, nw) &
) * cn
end do
end do
end do
end do
end do
end do
end function qmckl_compute_forces_jastrow_een_gForce of electron-electron-nucleus Jastrow Laplacian
Calculates the force of the electron-electron-nucleus Jastrow Laplacian.
\begin{eqnarray} \partial_{\alpha,m} \nabla^2 J_{een} &=& \partial_{\alpha,m} \sum_{i=1}^{N_\text{elec}}\sum_{p=2}^{N_\text{nord}} \sum_{k=0}^{p-1} \sum_{l=0}^{p-k-2\delta_{k,0}} c_{l,k,p,\alpha} \left(\nabla^2\widetilde{R}_{i\alpha}^{(p-k+l)/2} P_{i\alpha,k,(p-k-l)/2} + \nabla^2\widetilde{R}_{i\alpha}^{(p-k-l)/2} P_{i\alpha,k,(p-k+l)/2} + \widetilde{R}_{i\alpha}^{(p-k+l)/2} \nabla^2 P_{i\alpha,k,(p-k-l)/2} + \widetilde{R}_{i\alpha}^{(p-k-l)/2} \nabla^2 P_{i\alpha,k,(p-k+l)/2} \right.\\ &&+ \left. 2 \nabla \widetilde{R}_{i\alpha}^{(p-k+l)/2} \cdot \nabla P_{i\alpha,k,(p-k-l)/2} + 2 \nabla \widetilde{R}_{i\alpha}^{(p-k-l)/2} \cdot \nabla P_{i\alpha,k,(p-k+l)/2} \right)\\ &=& \sum_{i=1}^{N_\text{elec}}\sum_{p=2}^{N_\text{nord}} \sum_{k=0}^{p-1} \sum_{l=0}^{p-k-2\delta_{k,0}} c_{l,k,p,\alpha} \left( \partial_{\alpha,m} \nabla^2\widetilde{R}_{i\alpha}^{(p-k+l)/2} P_{i\alpha,k,(p-k-l)/2} + \partial_{\alpha,m} \nabla^2\widetilde{R}_{i\alpha}^{(p-k-l)/2} P_{i\alpha,k,(p-k+l)/2} + \partial_{\alpha,m} \widetilde{R}_{i\alpha}^{(p-k+l)/2} \nabla^2 P_{i\alpha,k,(p-k-l)/2} + \partial_{\alpha,m} \widetilde{R}_{i\alpha}^{(p-k-l)/2} \nabla^2 P_{i\alpha,k,(p-k+l)/2} \right.\\ &&+\nabla^2\widetilde{R}_{i\alpha}^{(p-k+l)/2} \partial_{\alpha,m} P_{i\alpha,k,(p-k-l)/2} + \nabla^2\widetilde{R}_{i\alpha}^{(p-k-l)/2} \partial_{\alpha,m} P_{i\alpha,k,(p-k+l)/2} + \widetilde{R}_{i\alpha}^{(p-k+l)/2} \partial_{\alpha,m} \nabla^2 P_{i\alpha,k,(p-k-l)/2} + \widetilde{R}_{i\alpha}^{(p-k-l)/2} \partial_{\alpha,m} \nabla^2 P_{i\alpha,k,(p-k+l)/2} \\ &&+ \left. 2 \partial_{\alpha,m} \nabla \widetilde{R}_{i\alpha}^{(p-k+l)/2} \cdot \nabla P_{i\alpha,k,(p-k-l)/2} + 2 \partial_{\alpha,m} \nabla \widetilde{R}_{i\alpha}^{(p-k-l)/2} \cdot \nabla P_{i\alpha,k,(p-k+l)/2} + 2 \nabla \widetilde{R}_{i\alpha}^{(p-k+l)/2} \cdot \partial_{\alpha,m} \nabla P_{i\alpha,k,(p-k-l)/2} + 2 \nabla \widetilde{R}_{i\alpha}^{(p-k-l)/2} \cdot \partial_{\alpha,m} \nabla P_{i\alpha,k,(p-k+l)/2} \right)\\ &=& \sum_{i=1}^{N_\text{elec}}\sum_{p=2}^{N_\text{nord}} \sum_{k=0}^{p-1} \sum_{l=0}^{p-k-2\delta_{k,0}} c_{l,k,p,\alpha} \left( \partial_{\alpha,m} \nabla^2\widetilde{R}_{i\alpha}^{(p-k+l)/2} P_{i\alpha,k,(p-k-l)/2} + \partial_{\alpha,m} \nabla^2\widetilde{R}_{i\alpha}^{(p-k-l)/2} P_{i\alpha,k,(p-k+l)/2} - \partial_{i,m} \widetilde{R}_{i\alpha}^{(p-k+l)/2} \nabla^2 P_{i\alpha,k,(p-k-l)/2} - \partial_{i,m} \widetilde{R}_{i\alpha}^{(p-k-l)/2} \nabla^2 P_{i\alpha,k,(p-k+l)/2} \right.\\ &&+\nabla^2\widetilde{R}_{i\alpha}^{(p-k+l)/2} \partial_{\alpha,m} P_{i\alpha,k,(p-k-l)/2} + \nabla^2\widetilde{R}_{i\alpha}^{(p-k-l)/2} \partial_{\alpha,m} P_{i\alpha,k,(p-k+l)/2} + \widetilde{R}_{i\alpha}^{(p-k+l)/2} \partial_{\alpha,m} \nabla^2 P_{i\alpha,k,(p-k-l)/2} + \widetilde{R}_{i\alpha}^{(p-k-l)/2} \partial_{\alpha,m} \nabla^2 P_{i\alpha,k,(p-k+l)/2} \\ &&+ \left. 2 \partial_{\alpha,m} \nabla \widetilde{R}_{i\alpha}^{(p-k+l)/2} \cdot \nabla P_{i\alpha,k,(p-k-l)/2} + 2 \partial_{\alpha,m} \nabla \widetilde{R}_{i\alpha}^{(p-k-l)/2} \cdot \nabla P_{i\alpha,k,(p-k+l)/2} + 2 \nabla \widetilde{R}_{i\alpha}^{(p-k+l)/2} \cdot \partial_{\alpha,m} \nabla P_{i\alpha,k,(p-k-l)/2} + 2 \nabla \widetilde{R}_{i\alpha}^{(p-k-l)/2} \cdot \partial_{\alpha,m} \nabla P_{i\alpha,k,(p-k+l)/2} \right) \end{eqnarray}Get
qmckl_exit_code
qmckl_get_forces_jastrow_een_l(qmckl_context context,
double* const forces_jastrow_een_l,
const int64_t size_max);interface
integer(qmckl_exit_code) function qmckl_get_forces_jastrow_een_l (context, &
forces_jastrow_een_l, size_max) bind(C)
use, intrinsic :: iso_c_binding
import
implicit none
integer (qmckl_context) , intent(in), value :: context
integer(c_int64_t), intent(in), value :: size_max
real(c_double), intent(out) :: forces_jastrow_een_l(size_max)
end function qmckl_get_forces_jastrow_een_l
end interface#
Compute
| Variable | Type | In/Out | Description |
|---|---|---|---|
context |
qmckl_context |
in | Global state |
walk_num |
int64_t |
in | Number of walkers |
elec_num |
int64_t |
in | Number of electrons |
nucl_num |
int64_t |
in | Number of nuclei |
cord_num |
int64_t |
in | order of polynomials |
dim_c_vector |
int64_t |
in | dimension of full coefficient vector |
c_vector_full |
double[dim_c_vector][nucl_num] |
in | full coefficient vector |
lkpm_combined_index |
int64_t[4][dim_c_vector] |
in | combined indices |
en_distance |
double[elec_num][nucl_num] |
in | Electron-nucleus distance |
tmp_c |
double[walk_num][0:cord_num-1][0:cord_num][nucl_num][elec_num] |
in | tmpc_matrix |
dtmp_c |
double[walk_num][0:cord_num-1][0:cord_num][nucl_num][4][elec_num] |
in | dtmp_c matrix |
forces_tmp_c |
double[walk_num][0:cord_num-1][0:cord_num][nucl_num][4][elec_num] |
in | Force of tmp_c matrix |
forces_dtmp_c |
double[walk_num][0:cord_num-1][0:cord_num][4][nucl_num][4][elec_num] |
in | Force of dtmp_c matrix |
forces_een_n |
double[walk_num][0:cord_num][3][nucl_num][4][elec_num] |
in | Force of derivative of electron-nucleus rescaled factor |
een_rescaled_n |
double[walk_num][0:cord_num][nucl_num][elec_num] |
in | Electron-nucleus rescaled factor |
een_rescaled_n_gl |
double[walk_num][0:cord_num][nucl_num][4][elec_num] |
in | Derivative of electron-nucleus rescaled factor |
forces_jastrow_een_l |
double[walk_num][3][nucl_num] |
out | Force of electron-electron-nucleus Jastrow Laplacian |
integer(qmckl_exit_code) function qmckl_compute_forces_jastrow_een_l( &
context, walk_num, elec_num, nucl_num, &
cord_num, dim_c_vector, c_vector_full, lkpm_combined_index, &
en_distance, tmp_c, dtmp_c, forces_tmp_c, forces_dtmp_c, forces_een_n, een_rescaled_n, &
een_rescaled_n_gl, forces_jastrow_een_l)&
result(info) bind(C)
use, intrinsic :: iso_c_binding
use qmckl
implicit none
integer(qmckl_context), intent(in) :: context
integer (c_int64_t) , intent(in),value :: walk_num, elec_num, cord_num, nucl_num, dim_c_vector
integer (c_int64_t) , intent(in) :: lkpm_combined_index(dim_c_vector,4)
real (c_double ) , intent(in) :: c_vector_full(nucl_num, dim_c_vector)
real (c_double ) , intent(in) :: en_distance(nucl_num, elec_num)
real (c_double ) , intent(in) :: tmp_c(elec_num, nucl_num,0:cord_num, 0:cord_num-1, walk_num)
real (c_double ) , intent(in) :: dtmp_c(elec_num, 4, nucl_num,0:cord_num, 0:cord_num-1, walk_num)
real (c_double ) , intent(in) :: forces_tmp_c(elec_num, 4,nucl_num,0:cord_num, 0:cord_num-1, walk_num)
real (c_double ) , intent(in) :: forces_dtmp_c(elec_num, 4, nucl_num,4,0:cord_num, 0:cord_num-1, walk_num)
real (c_double ) , intent(in) :: forces_een_n(elec_num, 4, nucl_num, 3, 0:cord_num, walk_num)
real (c_double ) , intent(in) :: een_rescaled_n(elec_num, nucl_num, 0:cord_num, walk_num)
real (c_double ) , intent(in) :: een_rescaled_n_gl(elec_num, 4, nucl_num, 0:cord_num, walk_num)
real (c_double ) , intent(out) :: forces_jastrow_een_l(nucl_num,3,walk_num)
integer*8 :: i, a, j, l, k, m, n, nw, ii, jj
double precision :: accu, accu2, cn
info = QMCKL_SUCCESS
if (context == QMCKL_NULL_CONTEXT) info = QMCKL_INVALID_CONTEXT
if (walk_num <= 0) info = QMCKL_INVALID_ARG_2
if (elec_num <= 0) info = QMCKL_INVALID_ARG_3
if (nucl_num <= 0) info = QMCKL_INVALID_ARG_4
if (cord_num < 0) info = QMCKL_INVALID_ARG_5
if (info /= QMCKL_SUCCESS) return
if (cord_num == 0) return
forces_jastrow_een_l = 0.0d0
do nw =1, walk_num
do n = 1, dim_c_vector
l = lkpm_combined_index(n, 1)
k = lkpm_combined_index(n, 2)
m = lkpm_combined_index(n, 4)
do a = 1, nucl_num
cn = c_vector_full(a, n)
if(cn == 0.d0) cycle
do ii = 1, 3
do i = 1, elec_num
forces_jastrow_een_l(a, ii, nw) = forces_jastrow_een_l(a, ii, nw) + (&
tmp_c(i,a, m, k,nw) * forces_een_n(i,4,a,ii ,m+l,nw) &
+ forces_tmp_c(i,ii,a, m, k,nw) * een_rescaled_n_gl(i,4,a,m+l,nw) &
+ tmp_c(i,a, m+l,k,nw) * forces_een_n(i,4,a,ii, m, nw) &
+ forces_tmp_c(i,ii,a, m+l,k,nw) * een_rescaled_n_gl(i,4,a,m, nw) &
- dtmp_c(i,4,a, m, k,nw) * een_rescaled_n_gl(i,ii,a,m+l,nw) &
+ forces_dtmp_c(i,4,a,ii,m, k,nw) * een_rescaled_n(i,a, m+l,nw) &
- dtmp_c(i,4,a, m+l,k,nw) * een_rescaled_n_gl(i,ii,a,m, nw) &
+ forces_dtmp_c(i,4,a,ii,m+l,k,nw) * een_rescaled_n(i,a, m, nw) &
) * cn
end do
end do
cn = cn + cn
do ii = 1, 3
do i = 1, elec_num
do jj = 1, 3
forces_jastrow_een_l(a, ii, nw) = forces_jastrow_een_l(a, ii, nw) + (&
dtmp_c(i,jj,a,m, k,nw) * forces_een_n(i,jj,a,ii ,m+l,nw) + &
dtmp_c(i,jj,a,m+l, k,nw) * forces_een_n(i,jj,a,ii ,m,nw) + &
forces_dtmp_c(i,jj,a,ii,m, k,nw) * een_rescaled_n_gl(i,jj,a,m+l,nw) + &
forces_dtmp_c(i,jj,a,ii,m+l, k,nw) * een_rescaled_n_gl(i,jj,a,m,nw) &
) * cn
end do
end do
end do
end do
end do
end do
end function qmckl_compute_forces_jastrow_een_lForce of delta_p matrix
Calculates the force of the delta_p matrix, required for force in a single-electron move. Here, the $r^\text{new}$ and $R^\text{new}$ are the new electron and nucleus positions of the electron that is being moved.
\begin{eqnarray*} \partial_{\alpha,m}\delta P_{i,\alpha,k,l} &=& \partial_{\alpha,m} \left(\sum_{j=1}^{N_\text{elec}} \left( \delta \widetilde{r}_{ij}^k \widetilde{R}_{j\alpha}^l \delta_{i,\text{num}} \right) + \widetilde{r}_{i,\text{num}}^k \delta \widetilde{R}_{\text{num},\alpha}^l + \delta \widetilde{r}_{i,\text{num}}^k \left( \widetilde{R}_{\text{num},\alpha}^l + \delta \widetilde{R}_{\text{num},\alpha}^l \right)\right) \\ &=& \partial_{\alpha,m} \left(\sum_{j=1}^{N_\text{elec}} \left( \delta \widetilde{r}_{ij}^k \widetilde{R}_{j\alpha}^l \delta_{i,\text{num}} \right) + \widetilde{r}_{i,\text{num}}^k \widetilde{R}_{\text{num},\alpha}^l + {\widetilde{r}_{i,\text{num}}^{\text{new}}}^k {\widetilde{R}_{\text{num},\alpha}^{\text{new}}}^l \right) \\ &=& \left(\sum_{j=1}^{N_\text{elec}} \left( \delta \widetilde{r}_{ij}^k \partial_{\alpha,m} \widetilde{R}_{j\alpha}^l \delta_{i,\text{num}} \right) + \widetilde{r}_{i,\text{num}}^k \partial_{\alpha,m}\widetilde{R}_{\text{num},\alpha}^l + {\widetilde{r}_{i,\text{num}}^{\text{new}}}^k \partial_{\alpha,m}{\widetilde{R}_{\text{num},\alpha}^{\text{new}}}^l \right) \\ &=& \left(\sum_{j=1}^{N_\text{elec}} \left( -\delta \widetilde{r}_{ij}^k \partial_{i,m} \widetilde{R}_{j\alpha}^l \delta_{i,\text{num}} \right) - \widetilde{r}_{i,\text{num}}^k \partial_{i,m}\widetilde{R}_{\text{num},\alpha}^l - {\widetilde{r}_{i,\text{num}}^{\text{new}}}^k \partial_{i,m}{\widetilde{R}_{\text{num},\alpha}^{\text{new}}}^l \right) \\ \end{eqnarray*}Get
qmckl_exit_code
qmckl_get_forces_jastrow_delta_p(qmckl_context context,
double* const forces_delta_p,
const int64_t size_max);Compute
| Variable | Type | In/Out | Description |
|---|---|---|---|
context |
qmckl_context |
in | Global state |
num |
int64_t |
in | Index of single electron |
walk_num |
int64_t |
in | Number of walkers |
elec_num |
int64_t |
in | Number of electrons |
nucl_num |
int64_t |
in | Number of nuclei |
cord_num |
int64_t |
in | order of polynomials |
een_rescaled_n |
double[walk_num][0:cord_num][nucl_num][elec_num] |
in | Electron-nucleus rescaled distances |
een_rescaled_e |
double[walk_num][0:cord_num][elec_num][elec_num] |
in | Electron-electron rescaled distances |
een_rescaled_single_n |
double[walk_num][0:cord_num][nucl_num] |
in | Electron-nucleus single rescaled distances |
een_rescaled_single_e |
double[walk_num][0:cord_num][elec_num] |
in | Electron-electron single rescaled distances |
een_rescaled_n_gl |
double[walk_num][0:cord_num][nucl_num][4][elec_num] |
in | Electron-nucleus rescaled distances derivatives |
een_rescaled_single_n_gl |
double[walk_num][0:cord_num][nucl_num][4] |
in | Electron-nucleus single rescaled distances derivatives |
forces_delta_p |
double[walk_num][0:cord_num-1][0:cord_num][nucl_num][3][elec_num] |
out | Force of delta_p matrix |
integer(qmckl_exit_code) function qmckl_compute_forces_jastrow_delta_p_doc( &
context, num_in, walk_num, elec_num, nucl_num, cord_num, &
een_rescaled_n, een_rescaled_e, een_rescaled_single_n, een_rescaled_single_e, &
een_rescaled_n_gl, een_rescaled_single_n_gl, forces_delta_p) &
result(info) bind(C)
use, intrinsic :: iso_c_binding
use qmckl
implicit none
integer(qmckl_context), intent(in) :: context
integer(c_int64_t) , intent(in), value :: num_in, walk_num, elec_num, cord_num, nucl_num
real(c_double) , intent(in) :: een_rescaled_n(elec_num, nucl_num, 0:cord_num, walk_num)
real(c_double) , intent(in) :: een_rescaled_e(elec_num, elec_num, 0:cord_num, walk_num)
real(c_double) , intent(in) :: een_rescaled_single_n(nucl_num, 0:cord_num, walk_num)
real(c_double) , intent(in) :: een_rescaled_single_e(elec_num, 0:cord_num, walk_num)
real(c_double) , intent(in) :: een_rescaled_n_gl(elec_num, 4, nucl_num, 0:cord_num, walk_num)
real(c_double) , intent(in) :: een_rescaled_single_n_gl(4, nucl_num, 0:cord_num, walk_num)
real(c_double) , intent(out) :: forces_delta_p(elec_num,3,nucl_num,0:cord_num, 0:cord_num-1, walk_num)
double precision :: tmp1, tmp2
double precision :: delta_e(elec_num)
integer*8 :: i, a, j, l, k, p, m, n, nw, num
double precision :: tmp, accu
integer*8 :: LDA, LDB, LDC
num = num_in + 1_8
info = QMCKL_SUCCESS
if (context == QMCKL_NULL_CONTEXT) info = QMCKL_INVALID_CONTEXT
if (walk_num <= 0) info = QMCKL_INVALID_ARG_3
if (elec_num <= 0) info = QMCKL_INVALID_ARG_4
if (nucl_num <= 0) info = QMCKL_INVALID_ARG_5
if (cord_num < 0) info = QMCKL_INVALID_ARG_6
if (info /= QMCKL_SUCCESS) return
if (cord_num == 0) then
forces_delta_p = 0.d0
return
endif
do nw=1, walk_num
do m=0, cord_num-1
do j = 1, elec_num
delta_e(j) = een_rescaled_e(j,num,m,nw) - een_rescaled_single_e(j,m,nw)
end do
do l=1, cord_num
do a = 1, nucl_num
do k = 1, 3
tmp1 = een_rescaled_n_gl(num, k, a, l, nw)
tmp2 = een_rescaled_single_n_gl(k,a,l,nw)
accu = 0.d0
do j = 1, elec_num
forces_delta_p(j,k,a,l,m,nw) = een_rescaled_e(j,num,m,nw) * tmp1 - &
een_rescaled_single_e(j,m,nw) * tmp2
accu = accu + delta_e(j) * een_rescaled_n_gl(j,k,a,l,nw)
end do
forces_delta_p(num,k,a,l,m,nw) = forces_delta_p(num,k,a,l,m,nw) + accu
end do
end do
end do
end do
end do
end function qmckl_compute_forces_jastrow_delta_p_docqmckl_exit_code
qmckl_compute_forces_jastrow_delta_p_hpc (const qmckl_context context,
const int64_t num,
const int64_t walk_num,
const int64_t elec_num,
const int64_t nucl_num,
const int64_t cord_num,
const double* een_rescaled_n,
const double* een_rescaled_e,
const double* een_rescaled_single_n,
const double* een_rescaled_single_e,
const double* een_rescaled_n_gl,
const double* een_rescaled_single_n_gl,
double* const forces_delta_p )
{
if (context == QMCKL_NULL_CONTEXT) return QMCKL_INVALID_CONTEXT;
if (num < 0) return QMCKL_INVALID_ARG_2;
if (walk_num <= 0) return QMCKL_INVALID_ARG_3;
if (elec_num <= 0) return QMCKL_INVALID_ARG_4;
if (nucl_num <= 0) return QMCKL_INVALID_ARG_5;
if (cord_num < 0) return QMCKL_INVALID_ARG_6;
if (een_rescaled_n == NULL) return QMCKL_INVALID_ARG_7;
if (een_rescaled_e == NULL) return QMCKL_INVALID_ARG_8;
if (een_rescaled_single_n == NULL) return QMCKL_INVALID_ARG_9;
if (een_rescaled_single_e == NULL) return QMCKL_INVALID_ARG_10;
if (een_rescaled_n_gl == NULL) return QMCKL_INVALID_ARG_11;
if (een_rescaled_single_n_gl == NULL) return QMCKL_INVALID_ARG_12;
if (cord_num == 0) {
const size_t dim = elec_num*3*nucl_num*(cord_num+1)*cord_num;
#pragma omp parallel for
for (int64_t nw = 0; nw < walk_num; ++nw) {
memset(&forces_delta_p[dim*nw],0,dim*sizeof(double));
}
return QMCKL_SUCCESS;
}
#pragma omp parallel for
for (int64_t nw = 0; nw < walk_num; ++nw) {
for (int64_t m = 0; m <= cord_num-1; ++m) {
double delta_e[elec_num];
const double* een_rescaled_e_ = &een_rescaled_e[elec_num*(num+elec_num*(m+(cord_num+1)*nw))];
const double* een_rescaled_single_e_ = &een_rescaled_single_e[elec_num*(m+(cord_num+1)*nw)];
for (int64_t j = 0; j < elec_num; ++j) {
delta_e[j] = een_rescaled_e_[j] - een_rescaled_single_e_[j];
}
for (int64_t l = 1; l <= cord_num; ++l) {
for (int64_t a = 0; a < nucl_num; ++a) {
for (int64_t k = 0; k < 3; ++k) {
const double* een_rescaled_n_gl_ = &een_rescaled_n_gl[elec_num*(k+4*(a+nucl_num*(l+(cord_num+1)*nw)))];
const double tmp1 = een_rescaled_n_gl_[num];
const double tmp2 = een_rescaled_single_n_gl[k+4*(a+nucl_num*(l+(cord_num+1)*nw))];
double* forces_delta_p_ = &forces_delta_p[elec_num*(k+3*(a+nucl_num*(l+(cord_num+1)*(m+cord_num*nw))))];
double accu = 0.0;
#pragma omp simd reduction(+:accu)
for (int64_t j = 0; j < elec_num; ++j) {
forces_delta_p_[j] = een_rescaled_e_[j] * tmp1 - een_rescaled_single_e_[j] * tmp2;
accu += delta_e[j] * een_rescaled_n_gl_[j];
}
forces_delta_p_[num] += accu;
}
}
}
}
}
return QMCKL_SUCCESS;
}Force of single electron-electron-nucleus Jastrow value
Computes the single-electron contribution to the electron-electron-nucleus Jastrow value force.
\begin{eqnarray*} \partial_{\alpha,m} \delta J_{een} &=& \partial_{\alpha,m} \sum_{p=2}^{N_\text{nord}} \sum_{k=0}^{p-1} \sum_{l=0}^{p-k-2\delta_{k,0}} c_{l,k,p,\alpha} \left( \sum_{i=1}^{N_\text{elec}} \left( \widetilde{R}_{i,\alpha,(p-k-l)/2} \delta P_{i,\alpha,k,(p-k+l)/2} \right) + \delta \widetilde{R}_{\text{num},\alpha,(p-k-l)/2} \left(P_{\text{num},\alpha,k,(p-k+l)/2} + \delta P_{\text{num},\alpha,k,(p-k+l)/2} \right)\right)\\ &=& \sum_{p=2}^{N_\text{nord}} \sum_{k=0}^{p-1} \sum_{l=0}^{p-k-2\delta_{k,0}} c_{l,k,p,\alpha} \left( \sum_{i=1}^{N_\text{elec}} \left( \partial_{\alpha,m}\widetilde{R}_{i,\alpha,(p-k-l)/2} \delta P_{i,\alpha,k,(p-k+l)/2} + \widetilde{R}_{i,\alpha,(p-k-l)/2} \partial_{\alpha,m}\delta P_{i,\alpha,k,(p-k+l)/2} \right) \right.\\ &&\left. + \partial_{\alpha,m}\delta \widetilde{R}_{\text{num},\alpha,(p-k-l)/2} \left(P_{\text{num},\alpha,k,(p-k+l)/2} + \delta P_{\text{num},\alpha,k,(p-k+l)/2} \right) + \delta \widetilde{R}_{\text{num},\alpha,(p-k-l)/2} \left(\partial_{\alpha,m}P_{\text{num},\alpha,k,(p-k+l)/2} + \partial_{\alpha,m}\delta P_{\text{num},\alpha,k,(p-k+l)/2} \right)\right)\\ &=& \sum_{p=2}^{N_\text{nord}} \sum_{k=0}^{p-1} \sum_{l=0}^{p-k-2\delta_{k,0}} c_{l,k,p,\alpha} \left( \sum_{i=1}^{N_\text{elec}} \left( -\partial_{i,m}\widetilde{R}_{i,\alpha,(p-k-l)/2} \delta P_{i,\alpha,k,(p-k+l)/2} + \widetilde{R}_{i,\alpha,(p-k-l)/2} \partial_{\alpha,m}\delta P_{i,\alpha,k,(p-k+l)/2} \right) \right.\\ &&\left. - \partial_{i,m}\delta \widetilde{R}_{\text{num},\alpha,(p-k-l)/2} \left(P_{\text{num},\alpha,k,(p-k+l)/2} + \delta P_{\text{num},\alpha,k,(p-k+l)/2} \right) + \delta \widetilde{R}_{\text{num},\alpha,(p-k-l)/2} \left(\partial_{\alpha,m}P_{\text{num},\alpha,k,(p-k+l)/2} + \partial_{\alpha,m}\delta P_{\text{num},\alpha,k,(p-k+l)/2} \right)\right)\\ \end{eqnarray*}Get
qmckl_exit_code
qmckl_get_forces_jastrow_single_een(qmckl_context context,
double* const forces_jastrow_single_een,
const int64_t size_max);Compute
| Variable | Type | In/Out | Description |
|---|---|---|---|
context |
qmckl_context |
in | Global state |
num |
int64_t |
in | Index of single electron |
walk_num |
int64_t |
in | Number of walkers |
elec_num |
int64_t |
in | Number of electrons |
nucl_num |
int64_t |
in | Number of nuclei |
cord_num |
int64_t |
in | order of polynomials |
dim_c_vector |
int64_t |
in | dimension of full coefficient vector |
c_vector_full |
double[dim_c_vector][nucl_num] |
in | full coefficient vector |
lkpm_combined_index |
int64_t[4][dim_c_vector] |
in | combined indices |
delta_p |
double[walk_num][0:cord_num-1][0:cord_num][nucl_num][elec_num] |
in | Single electron P matrix |
forces_delta_p |
double[walk_num][0:cord_num-1][0:cord_num][nucl_num][3][elec_num] |
in | Force of single electron P matrix |
tmp_c |
double[walk_num][0:cord_num-1][0:cord_num][nucl_num][elec_num] |
in | P matrix |
forces_tmp_c |
double[walk_num][0:cord_num-1][0:cord_num][nucl_num][4][elec_num] |
in | Force of P matrix |
een_rescaled_n |
double[walk_num][0:cord_num][nucl_num][elec_num] |
in | Electron-nucleus rescaled distances |
een_rescaled_single_n |
double[walk_num][0:cord_num][nucl_num] |
in | Electron-nucleus single rescaled distances |
een_rescaled_n_gl |
double[walk_num][0:cord_num][nucl_num][4][elec_num] |
in | Electron-nucleus rescaled distances derivatives |
een_rescaled_single_n_gl |
double[walk_num][0:cord_num][nucl_num][4] |
in | Electron-nucleus single rescaled distances derivatives |
forces_jastrow_single_een |
double[walk_num][nucl_num][3] |
out | Single electron–electron-nucleus Jastrow forces |
function qmckl_compute_forces_jastrow_single_een_doc( &
context, num_in, walk_num, elec_num, nucl_num, cord_num, &
dim_c_vector, c_vector_full, lkpm_combined_index, &
delta_p, forces_delta_p, tmp_c, forces_tmp_c, &
een_rescaled_n, een_rescaled_single_n, een_rescaled_n_gl, een_rescaled_single_n_gl, forces_jastrow_single_een) &
bind(C) result(info)
use qmckl
implicit none
integer (qmckl_context), intent(in), value :: context
integer (c_int64_t) , intent(in) , value :: num_in
integer (c_int64_t) , intent(in) , value :: walk_num
integer (c_int64_t) , intent(in) , value :: elec_num
integer (c_int64_t) , intent(in) , value :: nucl_num
integer (c_int64_t) , intent(in) , value :: dim_c_vector
integer (c_int64_t) , intent(in) , value :: cord_num
integer(c_int64_t) , intent(in) :: lkpm_combined_index(dim_c_vector,4)
real(c_double) , intent(in) :: c_vector_full(nucl_num, dim_c_vector)
real (c_double ) , intent(in) :: delta_p(elec_num, nucl_num,0:cord_num, 0:cord_num-1, walk_num)
real (c_double ) , intent(in) :: forces_delta_p(elec_num, 3, nucl_num,0:cord_num, 0:cord_num-1, walk_num)
real (c_double ) , intent(in) :: tmp_c(elec_num, nucl_num,0:cord_num, 0:cord_num-1, walk_num)
real (c_double ) , intent(in) :: forces_tmp_c(elec_num, 4, nucl_num,0:cord_num, 0:cord_num-1, walk_num)
real (c_double ) , intent(in) :: een_rescaled_n(elec_num, nucl_num, 0:cord_num, walk_num)
real (c_double ) , intent(in) :: een_rescaled_single_n(nucl_num, 0:cord_num, walk_num)
real (c_double ) , intent(in) :: een_rescaled_n_gl(elec_num, 4, nucl_num, 0:cord_num, walk_num)
real (c_double ) , intent(in) :: een_rescaled_single_n_gl(4, nucl_num, 0:cord_num, walk_num)
real (c_double ) , intent(out) :: forces_jastrow_single_een(3,nucl_num,walk_num)
integer(qmckl_exit_code) :: info
double precision :: een_rescaled_delta_n(nucl_num, 0:cord_num), een_rescaled_delta_n_gl(3,nucl_num, 0:cord_num)
integer*8 :: i, a, j, l, k, p, m, n, nw, num, kk
double precision :: accu, accu2, cn
integer*8 :: LDA, LDB, LDC
num = num_in + 1
info = QMCKL_SUCCESS
if (context == QMCKL_NULL_CONTEXT) info = QMCKL_INVALID_CONTEXT
if (walk_num <= 0) info = QMCKL_INVALID_ARG_3
if (elec_num <= 0) info = QMCKL_INVALID_ARG_4
if (nucl_num <= 0) info = QMCKL_INVALID_ARG_5
if (cord_num < 0) info = QMCKL_INVALID_ARG_6
if (info /= QMCKL_SUCCESS) return
forces_jastrow_single_een = 0.0d0
if (cord_num == 0) return
do nw =1, walk_num
een_rescaled_delta_n(:,:) = een_rescaled_single_n(:,:,nw) - een_rescaled_n(num,:,:,nw)
do kk = 1,3
een_rescaled_delta_n_gl(kk,:,:) = een_rescaled_single_n_gl(kk,:,:,nw) - een_rescaled_n_gl(num,kk,:,:,nw)
end do
do n = 1, dim_c_vector
l = lkpm_combined_index(n, 1)
k = lkpm_combined_index(n, 2)
p = lkpm_combined_index(n, 3)
m = lkpm_combined_index(n, 4)
do a = 1, nucl_num
cn = c_vector_full(a, n)
if(cn == 0.d0) cycle
do kk = 1, 3
accu = 0.0d0
do j = 1, elec_num
accu = accu - een_rescaled_n_gl(j,kk,a,m,nw) * delta_p(j,a,m+l,k,nw) + &
een_rescaled_n(j,a,m,nw) * forces_delta_p(j,kk,a,m+l,k,nw)
end do
accu = accu - een_rescaled_delta_n_gl(kk,a,m) * (tmp_c(num,a,m+l,k,nw) + delta_p(num,a,m+l,k,nw)) + &
een_rescaled_delta_n(a,m) * (forces_tmp_c(num,kk,a,m+l,k,nw) + forces_delta_p(num,kk,a,m+l,k,nw))
forces_jastrow_single_een(kk,a,nw) = forces_jastrow_single_een(kk,a,nw) + accu * cn
end do
end do
end do
end do
end function qmckl_compute_forces_jastrow_single_een_docfunction qmckl_compute_forces_jastrow_single_een_hpc( &
context, num_in, walk_num, elec_num, nucl_num, cord_num, &
dim_c_vector, c_vector_full, lkpm_combined_index, &
delta_p, forces_delta_p, tmp_c, forces_tmp_c, &
een_rescaled_n, een_rescaled_single_n, een_rescaled_n_gl, een_rescaled_single_n_gl, forces_jastrow_single_een) &
bind(C) result(info)
use qmckl
implicit none
integer (qmckl_context), intent(in), value :: context
integer (c_int64_t) , intent(in) , value :: num_in
integer (c_int64_t) , intent(in) , value :: walk_num
integer (c_int64_t) , intent(in) , value :: elec_num
integer (c_int64_t) , intent(in) , value :: nucl_num
integer (c_int64_t) , intent(in) , value :: dim_c_vector
integer (c_int64_t) , intent(in) , value :: cord_num
integer(c_int64_t) , intent(in) :: lkpm_combined_index(dim_c_vector,4)
real(c_double) , intent(in) :: c_vector_full(nucl_num, dim_c_vector)
real (c_double ) , intent(in) :: delta_p(elec_num, nucl_num,0:cord_num, 0:cord_num-1, walk_num)
real (c_double ) , intent(in) :: forces_delta_p(elec_num, 3, nucl_num,0:cord_num, 0:cord_num-1, walk_num)
real (c_double ) , intent(in) :: tmp_c(elec_num, nucl_num,0:cord_num, 0:cord_num-1, walk_num)
real (c_double ) , intent(in) :: forces_tmp_c(elec_num, 4, nucl_num,0:cord_num, 0:cord_num-1, walk_num)
real (c_double ) , intent(in) :: een_rescaled_n(elec_num, nucl_num, 0:cord_num, walk_num)
real (c_double ) , intent(in) :: een_rescaled_single_n(nucl_num, 0:cord_num, walk_num)
real (c_double ) , intent(in) :: een_rescaled_n_gl(elec_num, 4, nucl_num, 0:cord_num, walk_num)
real (c_double ) , intent(in) :: een_rescaled_single_n_gl(4, nucl_num, 0:cord_num, walk_num)
real (c_double ) , intent(out) :: forces_jastrow_single_een(3,nucl_num,walk_num)
integer(qmckl_exit_code) :: info
double precision, allocatable :: een_rescaled_delta_n(:, :), een_rescaled_delta_n_gl(:,:,:)
integer*8 :: i, a, j, l, k, p, m, n, nw, num, kk
double precision :: accu2, cn
double precision, allocatable :: accu(:,:), tmp(:)
double precision, external :: ddot
integer :: elec_num4
num = num_in + 1
info = QMCKL_SUCCESS
if (context == QMCKL_NULL_CONTEXT) info = QMCKL_INVALID_CONTEXT
if (walk_num <= 0) info = QMCKL_INVALID_ARG_3
if (elec_num <= 0) info = QMCKL_INVALID_ARG_4
if (nucl_num <= 0) info = QMCKL_INVALID_ARG_5
if (cord_num < 0) info = QMCKL_INVALID_ARG_6
if (info /= QMCKL_SUCCESS) return
forces_jastrow_single_een = 0.0d0
if (cord_num == 0) return
allocate(een_rescaled_delta_n(nucl_num, 0:cord_num), een_rescaled_delta_n_gl(3,nucl_num, 0:cord_num), &
accu(3,nucl_num), tmp(nucl_num))
elec_num4 = elec_num
do nw =1, walk_num
een_rescaled_delta_n(:,:) = een_rescaled_single_n(:,:,nw) - een_rescaled_n(num,:,:,nw)
een_rescaled_delta_n_gl(1:3,:,:) = een_rescaled_single_n_gl(1:3,:,:,nw) - een_rescaled_n_gl(num,1:3,:,:,nw)
do n = 1, dim_c_vector
l = lkpm_combined_index(n, 1)
k = lkpm_combined_index(n, 2)
p = lkpm_combined_index(n, 3)
m = lkpm_combined_index(n, 4)
do a = 1, nucl_num
cn = c_vector_full(a, n)
accu(1:3,a) = 0.0d0
if(cn == 0.d0) cycle
tmp(a) = tmp_c(num,a,m+l,k,nw) + delta_p(num,a,m+l,k,nw)
call dgemv('T', elec_num4, 3, -1.d0, een_rescaled_n_gl(1,1,a,m,nw), elec_num4, &
delta_p(1,a,m+l,k,nw), 1, 0.d0, accu(1,a), 1)
call dgemv('T', elec_num4, 3, 1.d0, forces_delta_p(1,1,a,m+l,k,nw), elec_num4, &
een_rescaled_n(1,a,m,nw), 1, 1.d0, accu(1,a), 1)
enddo
accu(1,:) = accu(1,:) - een_rescaled_delta_n_gl(1,:,m)*tmp(:)
accu(2,:) = accu(2,:) - een_rescaled_delta_n_gl(2,:,m)*tmp(:)
accu(3,:) = accu(3,:) - een_rescaled_delta_n_gl(3,:,m)*tmp(:)
accu(1,:) = accu(1,:) + een_rescaled_delta_n(:,m)*forces_tmp_c(num,1,:,m+l,k,nw)
accu(2,:) = accu(2,:) + een_rescaled_delta_n(:,m)*forces_tmp_c(num,2,:,m+l,k,nw)
accu(3,:) = accu(3,:) + een_rescaled_delta_n(:,m)*forces_tmp_c(num,3,:,m+l,k,nw)
accu(1,:) = accu(1,:) + een_rescaled_delta_n(:,m)*forces_delta_p(num,1,:,m+l,k,nw)
accu(2,:) = accu(2,:) + een_rescaled_delta_n(:,m)*forces_delta_p(num,2,:,m+l,k,nw)
accu(3,:) = accu(3,:) + een_rescaled_delta_n(:,m)*forces_delta_p(num,3,:,m+l,k,nw)
forces_jastrow_single_een(1,:,nw) = forces_jastrow_single_een(1,:,nw) + accu(1,:) * c_vector_full(:,n)
forces_jastrow_single_een(2,:,nw) = forces_jastrow_single_een(2,:,nw) + accu(2,:) * c_vector_full(:,n)
forces_jastrow_single_een(3,:,nw) = forces_jastrow_single_een(3,:,nw) + accu(3,:) * c_vector_full(:,n)
end do
end do
end function qmckl_compute_forces_jastrow_single_een_hpcForces of the orbitals
Force of AO value
Computes the forces on the values of the atomic orbitals (AO). These are equal to the gradients of the AOs multiplied with a minus sign, and summed over different indices.
Get
qmckl_exit_code
qmckl_get_forces_ao_value(qmckl_context context,
double* const forces_ao_value,
const int64_t size_max);Compute
| Variable | Type | In/Out | Description |
|---|---|---|---|
context |
qmckl_context |
in | Global state |
ao_num |
int64_t |
in | Number of AOs |
shell_num |
int64_t |
in | Number of shells |
point_num |
int64_t |
in | Number of points |
nucl_num |
int64_t |
in | Number of nuclei |
nucleus_index |
int64_t[nucl_num] |
in | Index of the 1st shell of each nucleus |
nucleus_shell_num |
int64_t[nucl_num] |
in | Number of shells per nucleus |
shell_ang_mom |
int32_t[shell_num] |
in | Angular momentum of each shell |
ao_factor |
double[ao_num] |
in | Normalization factor of the AOs |
ao_vgl |
double[point_num][5][shell_num] |
in | Value, gradients and Laplacian of the shells |
forces_ao_value |
double[nucl_num][3][point_num][ao_num] |
out | Forces of the AOs |
function qmckl_compute_forces_ao_value_doc(context, &
ao_num, shell_num, point_num, nucl_num, &
nucleus_index, nucleus_shell_num, &
shell_ang_mom, ao_factor, ao_vgl, forces_ao_value) &
bind(C) result(info)
use qmckl_constants
use qmckl, only : qmckl_ao_polynomial_vgl, qmckl_get_numprec_precision
implicit none
integer (qmckl_context), intent(in) , value :: context
integer (c_int64_t) , intent(in) , value :: ao_num
integer (c_int64_t) , intent(in) , value :: shell_num
integer (c_int64_t) , intent(in) , value :: point_num
integer (c_int64_t) , intent(in) , value :: nucl_num
integer (c_int64_t) , intent(in) :: nucleus_index(nucl_num)
integer (c_int64_t) , intent(in) :: nucleus_shell_num(nucl_num)
integer (c_int32_t) , intent(in) :: shell_ang_mom(shell_num)
real (c_double ) , intent(in) :: ao_factor(ao_num)
real (c_double ) , intent(in) :: ao_vgl(ao_num,5,point_num)
real (c_double ) , intent(out) :: forces_ao_value(ao_num,point_num,3,nucl_num)
integer(qmckl_exit_code) :: info
integer :: l, il, k
integer*8 :: ipoint, inucl, ishell
integer*8 :: ishell_start, ishell_end
integer :: lstart(0:20)
double precision :: x, y, z, r2
double precision :: cutoff
integer , allocatable :: ao_index(:)
allocate(ao_index(ao_num))
!forces_ao_value = 0.d0
! Pre-computed data
do l=0,20
lstart(l) = l*(l+1)*(l+2)/6 +1
end do
k=1
do inucl=1,nucl_num
ishell_start = nucleus_index(inucl) + 1
ishell_end = nucleus_index(inucl) + nucleus_shell_num(inucl)
do ishell = ishell_start, ishell_end
l = shell_ang_mom(ishell)
ao_index(ishell) = k
k = k + lstart(l+1) - lstart(l)
end do
end do
info = QMCKL_SUCCESS
do ipoint = 1, point_num
do inucl=1,nucl_num
! Loop over shells
ishell_start = nucleus_index(inucl) + 1
ishell_end = nucleus_index(inucl) + nucleus_shell_num(inucl)
do ishell = ishell_start, ishell_end
k = ao_index(ishell)
l = shell_ang_mom(ishell)
do il = lstart(l), lstart(l+1)-1
forces_ao_value(k,ipoint,1,inucl) = -ao_vgl(k,2,ipoint)
forces_ao_value(k,ipoint,2,inucl) = -ao_vgl(k,3,ipoint)
forces_ao_value(k,ipoint,3,inucl) = -ao_vgl(k,4,ipoint)
k = k+1
end do
end do
end do
end do
deallocate(ao_index)
end function qmckl_compute_forces_ao_value_docForce of MO value
Calculates the force on the molecular orbitals (MO) values. These are calculated by taking a linear combination of AOs.
Get
qmckl_exit_code
qmckl_get_forces_mo_value(qmckl_context context,
double* const forces_mo_value,
const int64_t size_max);qmckl_exit_code
qmckl_get_forces_mo_value_inplace (qmckl_context context,
double* const forces_mo_value,
const int64_t size_max);Compute
| Variable | Type | In/Out | Description |
|---|---|---|---|
context |
qmckl_context |
in | Global state |
nucl_num |
int64_t |
in | Number of AOs |
ao_num |
int64_t |
in | Number of AOs |
mo_num |
int64_t |
in | Number of MOs |
point_num |
int64_t |
in | Number of points |
shell_num |
int64_t |
in | Number of shells |
nucleus_index |
int64_t[nucl_num] |
in | Index of the 1st shell of each nucleus |
nucleus_shell_num |
int64_t[nucl_num] |
in | Number of shells per nucleus |
shell_ang_mom |
int32_t[shell_num] |
in | Angular momentum of each shell |
coefficient_t |
double[mo_num][ao_num] |
in | Transpose of the AO to MO transformation matrix |
forces_ao_value |
double[nucl_num][3][point_num][ao_num] |
in | Forces of AOs |
forces_mo_value |
double[nucl_num][3][point_num][mo_num] |
out | Forces of MOs |
integer(qmckl_exit_code) function qmckl_compute_forces_mo_value_doc(context, &
nucl_num,ao_num, mo_num, point_num, shell_num, nucleus_index, nucleus_shell_num, &
shell_ang_mom, coefficient_t, forces_ao_value, forces_mo_value) &
result(info) bind(C)
use, intrinsic :: iso_c_binding
use qmckl
implicit none
integer(qmckl_context), intent(in) :: context
integer(c_int64_t) , intent(in), value ::nucl_num, ao_num, mo_num, point_num, shell_num
real(c_double) , intent(in) :: forces_ao_value(ao_num,point_num,3,nucl_num)
real(c_double) , intent(in) :: coefficient_t(mo_num,ao_num)
integer (c_int64_t) , intent(in) :: nucleus_index(nucl_num)
integer (c_int64_t) , intent(in) :: nucleus_shell_num(nucl_num)
integer (c_int32_t) , intent(in) :: shell_ang_mom(shell_num)
real(c_double) , intent(out) :: forces_mo_value(mo_num,point_num,3,nucl_num)
integer*8 :: i,j,k,a, m, ishell_start, ishell_end, il, ishell, l
double precision :: c1, c2, c3
integer, allocatable :: ao_index(:)
integer :: lstart(0:20)
allocate(ao_index(ao_num))
do l=0,20
lstart(l) = l*(l+1)*(l+2)/6 +1
end do
k=1
do a=1,nucl_num
ishell_start = nucleus_index(a) + 1
ishell_end = nucleus_index(a) + nucleus_shell_num(a)
do ishell = ishell_start, ishell_end
l = shell_ang_mom(ishell)
ao_index(ishell) = k
k = k + lstart(l+1) - lstart(l)
end do
end do
info = QMCKL_SUCCESS
forces_mo_value = 0.0d0
do a=1,nucl_num
ishell_start = nucleus_index(a) + 1
ishell_end = nucleus_index(a) + nucleus_shell_num(a)
do j=1,point_num
do ishell = ishell_start, ishell_end
k = ao_index(ishell)
l = shell_ang_mom(ishell)
do il = lstart(l), lstart(l+1)-1
c1 = forces_ao_value(k,j,1,a)
c2 = forces_ao_value(k,j,2,a)
c3 = forces_ao_value(k,j,3,a)
if (c1 == 0.d0 .and. c2 == 0.d0 .and. c3 == 0.d0) cycle
do i=1,mo_num
forces_mo_value(i,j,1,a) = forces_mo_value(i,j,1,a) + coefficient_t(i,k) * c1
forces_mo_value(i,j,2,a) = forces_mo_value(i,j,2,a) + coefficient_t(i,k) * c2
forces_mo_value(i,j,3,a) = forces_mo_value(i,j,3,a) + coefficient_t(i,k) * c3
end do
k = k + 1
end do
end do
end do
end do
deallocate(ao_index)
end function qmckl_compute_forces_mo_value_docqmckl_exit_code qmckl_compute_forces_mo_value_doc (
const qmckl_context context,
const int64_t nucl_num,
const int64_t ao_num,
const int64_t mo_num,
const int64_t point_num,
const int64_t shell_num,
const int64_t* nucleus_index,
const int64_t* nucleus_shell_num,
const int32_t* shell_ang_mom,
const double* coefficient_t,
const double* forces_ao_value,
double* const forces_mo_value );Force of MO gradient
Calculates the forces of the gradients of the MOs. These are calculated by taking a linear combination of the required components of the Hessian of the AOs.
Get
qmckl_exit_code
qmckl_get_forces_mo_g(qmckl_context context,
double* const forces_mo_g,
const int64_t size_max);Compute
| Variable | Type | In/Out | Description |
|---|---|---|---|
context |
qmckl_context |
in | Global state |
ao_num |
int64_t |
in | Number of AOs |
mo_num |
int64_t |
in | Number of MOs |
point_num |
int64_t |
in | Number of points |
nucl_num |
int64_t |
in | Number of nuclei |
shell_num |
int64_t |
in | Number of shells |
nucleus_index |
int64_t[nucl_num] |
in | Index of the 1st shell of each nucleus |
nucleus_shell_num |
int64_t[nucl_num] |
in | Number of shells per nucleus |
shell_ang_mom |
int32_t[shell_num] |
in | Angular momentum of each shell |
coefficient_t |
double[mo_num][ao_num] |
in | Transpose of the AO to MO transformation matrix |
ao_hessian |
double[nucl_num][3][point_num][4][ao_num] |
in | Hessian of AOs |
forces_mo_g |
double[nucl_num][3][point_num][3][mo_num] |
out | Forces on gradients of MOs |
integer function qmckl_compute_forces_mo_g_doc(context, &
ao_num, mo_num, point_num, nucl_num, &
shell_num, nucleus_index, nucleus_shell_num, shell_ang_mom, &
coefficient_t, ao_hessian, forces_mo_g) &
bind(C) result(info)
use qmckl
implicit none
integer(qmckl_context), intent(in), value :: context
integer (c_int64_t) , intent(in), value :: nucl_num, ao_num, mo_num, point_num, shell_num
integer (c_int64_t) , intent(in) :: nucleus_index(nucl_num)
integer (c_int64_t) , intent(in) :: nucleus_shell_num(nucl_num)
integer (c_int32_t) , intent(in) :: shell_ang_mom(shell_num)
real (c_double ) , intent(in) :: coefficient_t(mo_num,ao_num)
real (c_double ) , intent(in) :: ao_hessian(ao_num,4,point_num,3,nucl_num)
real (c_double ) , intent(out) :: forces_mo_g(mo_num,3,point_num,3,nucl_num)
integer*8 :: i,j,k, m, n,a
double precision :: c1
integer :: l, il, ishell
integer*8 :: ishell_start, ishell_end
integer :: lstart(0:20)
integer , allocatable :: ao_index(:)
allocate(ao_index(ao_num))
do l=0,20
lstart(l) = l*(l+1)*(l+2)/6 +1
end do
k=1
do a=1,nucl_num
ishell_start = nucleus_index(a) + 1
ishell_end = nucleus_index(a) + nucleus_shell_num(a)
do ishell = ishell_start, ishell_end
l = shell_ang_mom(ishell)
ao_index(ishell) = k
k = k + lstart(l+1) - lstart(l)
end do
end do
info = QMCKL_SUCCESS
forces_mo_g = 0.d0
do a=1,nucl_num
ishell_start = nucleus_index(a) + 1
ishell_end = nucleus_index(a) + nucleus_shell_num(a)
do n = 1, 3
do j=1,point_num
do m = 1, 3
do ishell = ishell_start, ishell_end
k = ao_index(ishell)
l = shell_ang_mom(ishell)
do il = lstart(l), lstart(l+1)-1
c1 = ao_hessian(k, m, j, n, a)
if (c1 == 0.d0) then
k = k + 1
cycle
end if
do i=1,mo_num
forces_mo_g(i, m, j, n, a) = forces_mo_g(i, m, j, n, a) - coefficient_t(i,k) * c1
end do
k = k+1
end do
end do
end do
end do
end do
end do
deallocate(ao_index)
!do a=1,nucl_num
! do n = 1,3
! do m = 1, 3
! info = qmckl_dgemm(context,'N', 'N', mo_num, point_num, ao_num, &
! -1.d0, coefficient_t, mo_num, &
! ao_hessian(:, m, :, n, a), ao_num, &
! 1.d0, forces_mo_g(:, m, :, n, a), mo_num)
! end do
! end do
!end do
end function qmckl_compute_forces_mo_g_docqmckl_exit_code qmckl_compute_forces_mo_g_doc (
const qmckl_context context,
const int64_t ao_num,
const int64_t mo_num,
const int64_t point_num,
const int64_t nucl_num,
const int64_t shell_num,
const int64_t* nucleus_index,
const int64_t* nucleus_shell_num,
const int32_t* shell_ang_mom,
const double* coefficient_t,
const double* ao_hessian,
double* const forces_mo_g );Force of MO Laplacian
Computes the forces on the Laplacian of the MOs. They are calculated by taking a linear combination of the ao_hessian[:,:,:,3,:] components of the AO Hessian. These store the derivatives of the Laplacian of the AO.
Get
qmckl_exit_code
qmckl_get_forces_mo_l(qmckl_context context,
double* const forces_mo_l,
const int64_t size_max);Compute
| Variable | Type | In/Out | Description |
|---|---|---|---|
context |
qmckl_context |
in | Global state |
ao_num |
int64_t |
in | Number of AOs |
mo_num |
int64_t |
in | Number of MOs |
point_num |
int64_t |
in | Number of points |
nucl_num |
int64_t |
in | Number of nuclei |
shell_num |
int64_t |
in | Number of shells |
nucleus_index |
int64_t[nucl_num] |
in | Index of the 1st shell of each nucleus |
nucleus_shell_num |
int64_t[nucl_num] |
in | Number of shells per nucleus |
shell_ang_mom |
int32_t[shell_num] |
in | Angular momentum of each shell |
coefficient_t |
double[mo_num][ao_num] |
in | Transpose of the AO to MO transformation matrix |
ao_hessian |
double[nucl_num][3][point_num][4][ao_num] |
in | Hessian of AOs |
forces_mo_l |
double[nucl_num][3][point_num][mo_num] |
out | Forces on MO Laplacian |
integer function qmckl_compute_forces_mo_l_doc(context, &
ao_num, mo_num, point_num, nucl_num, &
shell_num, nucleus_index, nucleus_shell_num, shell_ang_mom, &
coefficient_t, ao_hessian, forces_mo_l) &
bind(C) result(info)
use qmckl
implicit none
integer(qmckl_context), intent(in), value :: context
integer (c_int64_t) , intent(in), value :: nucl_num, ao_num, mo_num, point_num, shell_num
integer (c_int64_t) , intent(in) :: nucleus_index(nucl_num)
integer (c_int64_t) , intent(in) :: nucleus_shell_num(nucl_num)
integer (c_int32_t) , intent(in) :: shell_ang_mom(shell_num)
real (c_double ) , intent(in) :: coefficient_t(mo_num,ao_num)
real (c_double ) , intent(in) :: ao_hessian(ao_num,4,point_num,3,nucl_num)
real (c_double ) , intent(out) :: forces_mo_l(mo_num,point_num,3,nucl_num)
integer*8 :: i,j,k, m, n,a, l, il, ishell, ishell_start, ishell_end
integer :: lstart(0:20)
double precision :: c1
integer , allocatable :: ao_index(:)
allocate(ao_index(ao_num))
do l=0,20
lstart(l) = l*(l+1)*(l+2)/6 +1
end do
k=1
do a=1,nucl_num
ishell_start = nucleus_index(a) + 1
ishell_end = nucleus_index(a) + nucleus_shell_num(a)
do ishell = ishell_start, ishell_end
l = shell_ang_mom(ishell)
ao_index(ishell) = k
k = k + lstart(l+1) - lstart(l)
end do
end do
forces_mo_l = 0.d0
info = QMCKL_SUCCESS
do a=1, nucl_num
ishell_start = nucleus_index(a) + 1
ishell_end = nucleus_index(a) + nucleus_shell_num(a)
do j=1,point_num
do n = 1, 3
do ishell = ishell_start, ishell_end
k = ao_index(ishell)
l = shell_ang_mom(ishell)
do il = lstart(l), lstart(l+1)-1
c1 = ao_hessian(k, 4, j, n, a)
if (c1 == 0.d0) then
k = k + 1
cycle
end if
do i=1,mo_num
forces_mo_l(i, j, n, a) = forces_mo_l(i, j, n, a) - coefficient_t(i,k) * c1
end do
k = k+1
end do
end do
end do
end do
end do
deallocate(ao_index)
!do a=1,nucl_num
! do m = 1, 3
! info = qmckl_dgemm(context,'N', 'N', mo_num, point_num, ao_num, &
! -1.d0, coefficient_t, mo_num, &
! ao_hessian(:, 4, :, m, a), ao_num, &
! 1.d0, forces_mo_l(:, :, m, a), mo_num)
! end do
!end do
end function qmckl_compute_forces_mo_l_docqmckl_exit_code qmckl_compute_forces_mo_l_doc (
const qmckl_context context,
const int64_t ao_num,
const int64_t mo_num,
const int64_t point_num,
const int64_t nucl_num,
const int64_t shell_num,
const int64_t* nucleus_index,
const int64_t* nucleus_shell_num,
const int32_t* shell_ang_mom,
const double* coefficient_t,
const double* ao_hessian,
double* const forces_mo_l );