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mirror of https://github.com/TREX-CoE/qmckl.git synced 2024-12-23 04:44:03 +01:00
qmckl/org/qmckl_electron.org
2022-10-09 00:04:03 +02:00

56 KiB

Electrons

In conventional QMC simulations, up-spin and down-spin electrons are different. The electron data structure contains the number of up-spin and down-spin electrons, and the electron coordinates.

The electrons are stored as points in the following order: for each walker, first up-spin electrons and then down-spin electrons.

If the points are set with the 'N' flag, the order of the components is [ (x,y,z), (x,y,z), ... ] Using the 'T' flage, it is [ (x,x,x,...), (y,y,y,...), (z,z,z,...) ]

Context

The following data stored in the context:

Variable Type Description
uninitialized int32_t Keeps bit set for uninitialized data
num int64_t Total number of electrons
up_num int64_t Number of up-spin electrons
down_num int64_t Number of down-spin electrons
provided bool If true, electron is valid
walker qmckl_point Current set of walkers
walker_old qmckl_point Previous set of walkers

Computed data:

Variable Type Description
ee_distance double[walker.num][num][num] Electron-electron distances
ee_distance_date uint64_t Last modification date of the electron-electron distances
en_distance double[walker.num][nucl_num][num] Electron-nucleus distances
en_distance_date uint64_t Last modification date of the electron-electron distances
ee_potential double[walker.num] Electron-electron potential energy
ee_potential_date uint64_t Last modification date of the electron-electron potential
en_potential double[walker.num] Electron-nucleus potential energy
en_potential_date int64_t Date when the electron-nucleus potential energy was computed

Data structure

typedef struct qmckl_walker_struct {
int64_t num;
qmckl_point_struct point;
} qmckl_walker;

typedef struct qmckl_electron_struct {
int64_t        num;
int64_t        up_num;
int64_t        down_num;
qmckl_walker   walker;
qmckl_walker   walker_old;
uint64_t       ee_distance_date;
uint64_t       en_distance_date;
uint64_t       ee_potential_date;
uint64_t       en_potential_date;
double*        ee_distance;
double*        en_distance;
double*        ee_potential;
double*        en_potential;
int32_t        uninitialized;
bool           provided;
} qmckl_electron_struct;

The uninitialized integer contains one bit set to one for each initialization function which has not been called. It becomes equal to zero after all initialization functions have been called. The struct is then initialized and provided == true. Some values are initialized by default, and are not concerned by this mechanism.

qmckl_exit_code qmckl_init_electron(qmckl_context context);
qmckl_exit_code qmckl_init_electron(qmckl_context context) {

if (qmckl_context_check(context) == QMCKL_NULL_CONTEXT) {
 return false;
}

qmckl_context_struct* const ctx = (qmckl_context_struct*) context;
assert (ctx != NULL);

ctx->electron.uninitialized = (1 << 1) - 1;

return QMCKL_SUCCESS;
}
bool qmckl_electron_provided (const qmckl_context context);

Initialization functions

To set the data relative to the electrons in the context, the following functions need to be called. When the data structure is initialized, the internal coord_new and coord_old arrays are both not allocated.

qmckl_exit_code qmckl_set_electron_num      (qmckl_context context, const int64_t up_num, const int64_t down_num);
qmckl_exit_code qmckl_set_electron_coord    (qmckl_context context, const char transp, const int64_t walk_num, const double* coord, const int64_t size_max);

#+NAME:pre2

#+NAME:post

To set the number of electrons, we give the number of up-spin and down-spin electrons to the context and we set the number of walkers.

interface
integer(c_int32_t) function qmckl_set_electron_num(context, alpha, beta) bind(C)
 use, intrinsic :: iso_c_binding
 import
 implicit none

 integer (c_int64_t) , intent(in)  , value :: context
 integer (c_int64_t) , intent(in)  , value :: alpha
 integer (c_int64_t) , intent(in)  , value :: beta
end function
end interface

The following function sets the electron coordinates of all the walkers. When this is done, the pointers to the old and new sets of coordinates are swapped, and the new coordinates are overwritten. This can be done only when the data relative to electrons have been set.

size_max should be equal equal or geater than elec_num * walker.num * 3, to be symmetric with qmckl_get_electron_coord.

Important: changing the electron coordinates increments the date in the context.

interface
integer(c_int32_t) function qmckl_set_electron_coord(context, transp, walk_num, coord, size_max) bind(C)
 use, intrinsic :: iso_c_binding
 import
 implicit none

 integer (c_int64_t) , intent(in)  , value :: context
 character           , intent(in)  , value :: transp
 integer (c_int64_t) , intent(in)  , value :: walk_num
 double precision    , intent(in)          :: coord(*)
 integer (c_int64_t) , intent(in)  , value :: size_max
end function
end interface

Access functions

Access functions return QMCKL_SUCCESS when the data has been successfully retrieved. It returnes QMCKL_INVALID_CONTEXT when the context is not a valid context, and QMCKL_NOT_PROVIDED when the data has not been provided. If the function returns successfully, the variable pointed by the pointer given in argument contains the requested data. Otherwise, this variable is untouched.

Number of electrons

Number of walkers

A walker is a set of electron coordinates that are arguments of the wave function. walk_num is the number of walkers.

Electron coordinates

Returns the current electron coordinates. The pointer is assumed to point on a memory block of size size_max3 * elec_num * walker.num. The order of the indices is:

Normal Transposed
C [walker.num*elec_num][3] [3][walker.num*elec_num]
Fortran (3,walker.num*elec_num) (walker.num*elec_num, 3)

As the walker attribute is equal to points, returning the current electron coordinates is equivalent to returning the current points.

Test

/* Reference input data */
int64_t walk_num      = chbrclf_walk_num;
int64_t elec_num      = chbrclf_elec_num;
int64_t elec_up_num   = chbrclf_elec_up_num;
int64_t elec_dn_num   = chbrclf_elec_dn_num;
int64_t nucl_num      = chbrclf_nucl_num;
double* charge        = chbrclf_charge;
double* nucl_coord    = &(chbrclf_nucl_coord[0][0]);

double* elec_coord    = &(chbrclf_elec_coord[0][0][0]);


/* --- */

qmckl_exit_code rc;

assert(!qmckl_electron_provided(context));

int64_t n;
rc = qmckl_get_electron_num (context, &n);
assert(rc == QMCKL_NOT_PROVIDED);

rc = qmckl_get_electron_up_num (context, &n);
assert(rc == QMCKL_NOT_PROVIDED);

rc = qmckl_get_electron_down_num (context, &n);
assert(rc == QMCKL_NOT_PROVIDED);


rc = qmckl_set_electron_num (context, elec_up_num, elec_dn_num);
qmckl_check(context, rc);
assert(qmckl_electron_provided(context));

rc = qmckl_get_electron_up_num (context, &n);
qmckl_check(context, rc);
assert(n == elec_up_num);

rc = qmckl_get_electron_down_num (context, &n);
qmckl_check(context, rc);
assert(n == elec_dn_num);

rc = qmckl_get_electron_num (context, &n);
qmckl_check(context, rc);
assert(n == elec_num);


int64_t w = 0;
rc = qmckl_get_electron_walk_num (context, &w);
qmckl_check(context, rc);
assert(w == 0);


assert(qmckl_electron_provided(context));

rc = qmckl_set_electron_coord (context, 'N', walk_num, elec_coord, walk_num*elec_num*3);
qmckl_check(context, rc);

rc = qmckl_get_electron_walk_num (context, &w);
qmckl_check(context, rc);
assert(w == walk_num);

double elec_coord2[walk_num*3*elec_num];

rc = qmckl_get_electron_coord (context, 'N', elec_coord2, walk_num*3*elec_num);
qmckl_check(context, rc);
for (int64_t i=0 ; i<3*elec_num*walk_num ; ++i) {
printf("%f %f\n",  elec_coord[i],  elec_coord2[i]);
assert( elec_coord[i] == elec_coord2[i] );
}

Computation

The computed data is stored in the context so that it can be reused by different kernels. To ensure that the data is valid, for each computed data the date of the context is stored when it is computed. To know if some data needs to be recomputed, we check if the date of the dependencies are more recent than the date of the data to compute. If it is the case, then the data is recomputed and the current date is stored.

Electron-electron distances

Get

qmckl_exit_code qmckl_get_electron_ee_distance(qmckl_context context, double* const distance);

Compute

Variable Type In/Out Description
context qmckl_context in Global state
elec_num int64_t in Number of electrons
walk_num int64_t in Number of walkers
coord double[3][walk_num][elec_num] in Electron coordinates
ee_distance double[walk_num][elec_num][elec_num] out Electron-electron distances
integer function qmckl_compute_ee_distance_f(context, elec_num, walk_num, coord, ee_distance) &
 result(info)
use qmckl
implicit none
integer(qmckl_context), intent(in)  :: context
integer*8             , intent(in)  :: elec_num
integer*8             , intent(in)  :: walk_num
double precision      , intent(in)  :: coord(elec_num,walk_num,3)
double precision      , intent(out) :: ee_distance(elec_num,elec_num,walk_num)

integer*8 :: k, i, j
double precision :: x, y, z

info = QMCKL_SUCCESS

if (context == QMCKL_NULL_CONTEXT) then
 info = QMCKL_INVALID_CONTEXT
 return
endif

if (elec_num <= 0) then
 info = QMCKL_INVALID_ARG_2
 return
endif

if (walk_num <= 0) then
 info = QMCKL_INVALID_ARG_3
 return
endif

do k=1,walk_num
 info = qmckl_distance(context, 'T', 'T', elec_num, elec_num, &
      coord(1,k,1), elec_num * walk_num, &
      coord(1,k,1), elec_num * walk_num, &
      ee_distance(1,1,k), elec_num)
 if (info /= QMCKL_SUCCESS) then
    exit
 endif
end do

end function qmckl_compute_ee_distance_f

Test

assert(qmckl_electron_provided(context));


double ee_distance[walk_num * elec_num * elec_num];
rc = qmckl_get_electron_ee_distance(context, ee_distance);

// (e1,e2,w)
// (0,0,0) == 0.
assert(ee_distance[0] == 0.);

// (1,0,0) == (0,1,0)
assert(ee_distance[1] == ee_distance[elec_num]);

// value of (1,0,0)
assert(fabs(ee_distance[1]-7.152322512964209) < 1.e-12);

// (0,0,1) == 0.
assert(ee_distance[elec_num*elec_num] == 0.);

// (1,0,1) == (0,1,1)
assert(ee_distance[elec_num*elec_num+1] == ee_distance[elec_num*elec_num+elec_num]);

// value of (1,0,1)
assert(fabs(ee_distance[elec_num*elec_num+1]-6.5517646321055665) < 1.e-12);

Electron-electron potential

ee_potential is given by

\[ \mathcal{V}_{ee} = \sum_{i=1}^{N_e}\sum_{j>i}^{N_e}\frac{1}{r_{ij}} \]

where \(\mathcal{V}_{ee}\) is the ee potential and \[r_{ij}\] the ee distance.

Get

qmckl_exit_code qmckl_get_electron_ee_potential(qmckl_context context, double* const ee_potential);

Compute

Variable Type In/Out Description
context qmckl_context in Global state
elec_num int64_t in Number of electrons
walk_num int64_t in Number of walkers
ee_distance double[walk_num][elec_num][elec_num] in Electron-electron distances
ee_potential double[walk_num] out Electron-electron potential
integer function qmckl_compute_ee_potential_f(context, elec_num, walk_num, &
 ee_distance, ee_potential) &
 result(info)
use qmckl
implicit none
integer(qmckl_context), intent(in)  :: context
integer*8             , intent(in)  :: elec_num
integer*8             , intent(in)  :: walk_num
double precision      , intent(in)  :: ee_distance(elec_num,elec_num,walk_num)
double precision      , intent(out) :: ee_potential(walk_num)

integer*8 :: nw, i, j

info = QMCKL_SUCCESS

if (context == QMCKL_NULL_CONTEXT) then
 info = QMCKL_INVALID_CONTEXT
 return
endif

if (elec_num <= 0) then
 info = QMCKL_INVALID_ARG_2
 return
endif

if (walk_num <= 0) then
 info = QMCKL_INVALID_ARG_3
 return
endif

ee_potential = 0.0d0
do nw=1,walk_num
do j=2,elec_num
  do i=1,j-1
    if (dabs(ee_distance(i,j,nw)) > 1e-5) then
      ee_potential(nw) = ee_potential(nw) + 1.0d0/(ee_distance(i,j,nw))
    endif
  end do
end do
end do

end function qmckl_compute_ee_potential_f
qmckl_exit_code qmckl_compute_ee_potential (
const qmckl_context context,
const int64_t elec_num,
const int64_t walk_num,
const double* ee_distance,
double* const ee_potential );

Test

double ee_potential[walk_num];

rc = qmckl_get_electron_ee_potential(context, &(ee_potential[0]));
qmckl_check(context, rc);

Electron-nucleus distances

Get

qmckl_exit_code qmckl_get_electron_en_distance(qmckl_context context, double* distance);

Compute

Variable Type In/Out Description
context qmckl_context in Global state
elec_num int64_t in Number of electrons
nucl_num int64_t in Number of nuclei
walk_num int64_t in Number of walkers
elec_coord double[3][walk_num][elec_num] in Electron coordinates
nucl_coord double[3][elec_num] in Nuclear coordinates
en_distance double[walk_num][nucl_num][elec_num] out Electron-nucleus distances
integer function qmckl_compute_en_distance_f(context, elec_num, nucl_num, walk_num, elec_coord, nucl_coord, en_distance) &
 result(info)
use qmckl
implicit none
integer(qmckl_context), intent(in)  :: context
integer*8             , intent(in)  :: elec_num
integer*8             , intent(in)  :: nucl_num
integer*8             , intent(in)  :: walk_num
double precision      , intent(in)  :: elec_coord(elec_num,walk_num,3)
double precision      , intent(in)  :: nucl_coord(nucl_num,3)
double precision      , intent(out) :: en_distance(elec_num,nucl_num,walk_num)

integer*8 :: k

info = QMCKL_SUCCESS

if (context == QMCKL_NULL_CONTEXT) then
 info = QMCKL_INVALID_CONTEXT
 return
endif

if (elec_num <= 0) then
 info = QMCKL_INVALID_ARG_2
 return
endif

if (nucl_num <= 0) then
 info = QMCKL_INVALID_ARG_3
 return
endif

if (walk_num <= 0) then
 info = QMCKL_INVALID_ARG_4
 return
endif

do k=1,walk_num
 info = qmckl_distance(context, 'T', 'T', elec_num, nucl_num, &
      elec_coord(1,k,1), elec_num * walk_num, &
      nucl_coord, nucl_num, &
      en_distance(1,1,k), elec_num)
 if (info /= QMCKL_SUCCESS) then
    exit
 endif
end do

end function qmckl_compute_en_distance_f

Test

assert(!qmckl_nucleus_provided(context));
assert(qmckl_electron_provided(context));

rc = qmckl_set_nucleus_num (context, nucl_num);
qmckl_check(context, rc);

rc = qmckl_set_nucleus_charge (context, charge, nucl_num);
qmckl_check(context, rc);

rc = qmckl_set_nucleus_coord (context, 'T', nucl_coord, 3*nucl_num);
qmckl_check(context, rc);

assert(qmckl_nucleus_provided(context));

double en_distance[walk_num][nucl_num][elec_num];

rc = qmckl_get_electron_en_distance(context, &(en_distance[0][0][0]));
qmckl_check(context, rc);

// (e,n,w) in Fortran notation
// (1,1,1)
assert(fabs(en_distance[0][0][0] - 7.546738741619978) < 1.e-12);

// (1,2,1)
assert(fabs(en_distance[0][1][0] - 8.77102435246984) < 1.e-12);

// (2,1,1)
assert(fabs(en_distance[0][0][1] - 3.698922010513608) < 1.e-12);

// (1,1,2)
assert(fabs(en_distance[1][0][0] - 5.824059436060509) < 1.e-12);

// (1,2,2)
assert(fabs(en_distance[1][1][0] - 7.080482110317645) < 1.e-12);

// (2,1,2)
assert(fabs(en_distance[1][0][1] - 3.1804527583077356) < 1.e-12);

Electron-nucleus potential

en_potential stores the en potential energy

\[ \mathcal{V}_{en} = -\sum_{i=1}^{N_e}\sum_{A=1}^{N_n}\frac{Z_A}{r_{iA}} \]

where \(\mathcal{V}_{en}\) is the en potential, \[r_{iA}\] the en distance and \[Z_A\] is the nuclear charge.

Get

qmckl_exit_code qmckl_get_electron_en_potential(qmckl_context context, double* const en_potential);

Compute

Variable Type In/Out Description
context qmckl_context in Global state
elec_num int64_t in Number of electrons
nucl_num int64_t in Number of nuclei
walk_num int64_t in Number of walkers
charge double[nucl_num] in charge of nucleus
en_distance double[walk_num][nucl_num][elec_num] in Electron-electron rescaled distances
en_potential double[walk_num] out Electron-electron potential
integer function qmckl_compute_en_potential_f(context, elec_num, nucl_num, walk_num, &
 charge, en_distance, en_potential) &
 result(info)
use qmckl
implicit none
integer(qmckl_context), intent(in)  :: context
integer*8             , intent(in)  :: elec_num
integer*8             , intent(in)  :: nucl_num
integer*8             , intent(in)  :: walk_num
double precision      , intent(in)  :: charge(nucl_num)
double precision      , intent(in)  :: en_distance(elec_num,nucl_num,walk_num)
double precision      , intent(out) :: en_potential(walk_num)

integer*8 :: nw, i, j

info = QMCKL_SUCCESS

if (context == QMCKL_NULL_CONTEXT) then
 info = QMCKL_INVALID_CONTEXT
 return
endif

if (elec_num <= 0) then
 info = QMCKL_INVALID_ARG_2
 return
endif

if (walk_num <= 0) then
 info = QMCKL_INVALID_ARG_3
 return
endif

en_potential = 0.0d0
do nw=1,walk_num
do j=1,nucl_num
  do i=1,elec_num
    if (dabs(en_distance(i,j,nw)) > 1e-5) then
      en_potential(nw) = en_potential(nw) - charge(j)/(en_distance(i,j,nw))
    endif
  end do
end do
end do

end function qmckl_compute_en_potential_f
qmckl_exit_code qmckl_compute_en_potential (
const qmckl_context context,
const int64_t elec_num,
const int64_t nucl_num,
const int64_t walk_num,
const double* charge,
const double* en_distance,
double* const en_potential );

Test

double en_potential[walk_num];

rc = qmckl_get_electron_en_potential(context, &(en_potential[0]));
qmckl_check(context, rc);

Generate initial coordinates