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qs_tddfpt2_properties.F
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1!--------------------------------------------------------------------------------------------------!
2! CP2K: A general program to perform molecular dynamics simulations !
3! Copyright 2000-2026 CP2K developers group <https://cp2k.org> !
4! !
5! SPDX-License-Identifier: GPL-2.0-or-later !
6!--------------------------------------------------------------------------------------------------!
7
8MODULE qs_tddfpt2_properties
9 USE atomic_kind_types, ONLY: atomic_kind_type
10 USE bibliography, ONLY: martin2003,&
11 cite_reference
12 USE bse_print, ONLY: print_exciton_descriptors
13 USE bse_properties, ONLY: exciton_descr_type,&
14 get_exciton_descriptors
15 USE bse_util, ONLY: get_multipoles_mo
16 USE cell_types, ONLY: cell_type
17 USE cp_blacs_env, ONLY: cp_blacs_env_type
18 USE cp_cfm_basic_linalg, ONLY: cp_cfm_solve
19 USE cp_cfm_types, ONLY: cp_cfm_create,&
20 cp_cfm_release,&
21 cp_cfm_set_all,&
22 cp_cfm_to_fm,&
23 cp_cfm_type,&
24 cp_fm_to_cfm
25 USE cp_control_types, ONLY: dft_control_type,&
26 tddfpt2_control_type
27 USE cp_dbcsr_api, ONLY: &
28 dbcsr_copy, dbcsr_get_block_p, dbcsr_get_info, dbcsr_init_p, dbcsr_iterator_blocks_left, &
29 dbcsr_iterator_next_block, dbcsr_iterator_start, dbcsr_iterator_stop, dbcsr_iterator_type, &
30 dbcsr_p_type, dbcsr_set, dbcsr_type
31 USE cp_dbcsr_operations, ONLY: copy_dbcsr_to_fm,&
32 copy_fm_to_dbcsr,&
33 cp_dbcsr_sm_fm_multiply,&
34 dbcsr_allocate_matrix_set,&
35 dbcsr_deallocate_matrix_set
36 USE cp_fm_basic_linalg, ONLY: cp_fm_scale,&
37 cp_fm_scale_and_add,&
38 cp_fm_trace
39 USE cp_fm_diag, ONLY: choose_eigv_solver,&
40 cp_fm_geeig
41 USE cp_fm_struct, ONLY: cp_fm_struct_create,&
42 cp_fm_struct_release,&
43 cp_fm_struct_type
44 USE cp_fm_types, ONLY: cp_fm_create,&
45 cp_fm_get_info,&
46 cp_fm_release,&
47 cp_fm_set_all,&
48 cp_fm_to_fm,&
49 cp_fm_to_fm_submat_general,&
50 cp_fm_type,&
51 cp_fm_vectorsnorm
52 USE cp_log_handling, ONLY: cp_get_default_logger,&
53 cp_logger_get_default_io_unit,&
54 cp_logger_type
55 USE cp_output_handling, ONLY: cp_p_file,&
56 cp_print_key_finished_output,&
57 cp_print_key_should_output,&
58 cp_print_key_unit_nr
59 USE cp_realspace_grid_cube, ONLY: cp_pw_to_cube
60 USE input_constants, ONLY: no_sf_tddfpt,&
61 tddfpt_dipole_berry,&
62 tddfpt_dipole_length,&
63 tddfpt_dipole_scf_moment,&
64 tddfpt_dipole_velocity,&
65 tddfpt_dipole_velocity_old
66 USE input_section_types, ONLY: section_vals_get_subs_vals,&
67 section_vals_type,&
68 section_vals_val_get
69 USE kinds, ONLY: default_path_length,&
70 dp,&
71 int_8
72 USE mathconstants, ONLY: twopi,&
73 z_one,&
74 z_zero
75 USE message_passing, ONLY: mp_comm_type,&
76 mp_para_env_type,&
77 mp_request_type
78 USE molden_utils, ONLY: write_mos_molden
79 USE moments_utils, ONLY: get_reference_point
80 USE parallel_gemm_api, ONLY: parallel_gemm
81 USE particle_list_types, ONLY: particle_list_type
82 USE particle_types, ONLY: particle_type
83 USE physcon, ONLY: evolt
84 USE pw_env_types, ONLY: pw_env_get,&
85 pw_env_type
86 USE pw_poisson_types, ONLY: pw_poisson_type
87 USE pw_pool_types, ONLY: pw_pool_p_type,&
88 pw_pool_type
89 USE pw_types, ONLY: pw_c1d_gs_type,&
90 pw_r3d_rs_type
91 USE qs_collocate_density, ONLY: calculate_wavefunction
92 USE qs_environment_types, ONLY: get_qs_env,&
93 qs_environment_type
94 USE qs_kind_types, ONLY: qs_kind_type
95 USE qs_ks_types, ONLY: qs_ks_env_type
96 USE qs_mo_types, ONLY: allocate_mo_set,&
97 deallocate_mo_set,&
98 get_mo_set,&
99 init_mo_set,&
100 mo_set_type,&
101 set_mo_set
102 USE qs_moments, ONLY: build_berry_moment_matrix
103 USE qs_neighbor_list_types, ONLY: neighbor_list_set_p_type
104 USE qs_operators_ao, ONLY: rrc_xyz_ao
105 USE qs_overlap, ONLY: build_overlap_matrix
106 USE qs_subsys_types, ONLY: qs_subsys_get,&
107 qs_subsys_type
108 USE qs_tddfpt2_types, ONLY: tddfpt_ground_state_mos
109 USE string_utilities, ONLY: integer_to_string
110 USE util, ONLY: sort
111#include "./base/base_uses.f90"
112
113 IMPLICIT NONE
114
115 PRIVATE
116
117 CHARACTER(len=*), PARAMETER, PRIVATE :: moduleN = 'qs_tddfpt2_properties'
118
119 ! number of first derivative components (3: d/dx, d/dy, d/dz)
120 INTEGER, PARAMETER, PRIVATE :: nderivs = 3
121 INTEGER, PARAMETER, PRIVATE :: maxspins = 2
122
123 PUBLIC :: tddfpt_dipole_operator, tddfpt_print_summary, tddfpt_print_excitation_analysis, &
124 tddfpt_print_nto_analysis, tddfpt_print_exciton_descriptors
125
126! **************************************************************************************************
127
128CONTAINS
129
130! **************************************************************************************************
131!> \brief Compute the action of the dipole operator on the ground state wave function.
132!> \param dipole_op_mos_occ 2-D array [x,y,z ; spin] of matrices where to put the computed quantity
133!> (allocated and initialised on exit)
134!> \param tddfpt_control TDDFPT control parameters
135!> \param gs_mos molecular orbitals optimised for the ground state
136!> \param qs_env Quickstep environment
137!> \par History
138!> * 05.2016 created as 'tddfpt_print_summary' [Sergey Chulkov]
139!> * 06.2018 dipole operator based on the Berry-phase formula [Sergey Chulkov]
140!> * 08.2018 splited of from 'tddfpt_print_summary' and merged with code from 'tddfpt'
141!> [Sergey Chulkov]
142!> \note \parblock
143!> Adapted version of the subroutine find_contributions() which was originally created
144!> by Thomas Chassaing on 02.2005.
145!>
146!> The relation between dipole integrals in velocity and length forms are the following:
147!> \f[<\psi_i|\nabla|\psi_a> = <\psi_i|\vec{r}|\hat{H}\psi_a> - <\hat{H}\psi_i|\vec{r}|\psi_a>
148!> = (\epsilon_a - \epsilon_i) <\psi_i|\vec{r}|\psi_a> .\f],
149!> due to the commutation identity:
150!> \f[\vec{r}\hat{H} - \hat{H}\vec{r} = [\vec{r},\hat{H}] = [\vec{r},-1/2 \nabla^2] = \nabla\f] .
151!> \endparblock
152! **************************************************************************************************
153 SUBROUTINE tddfpt_dipole_operator(dipole_op_mos_occ, tddfpt_control, gs_mos, qs_env)
154 TYPE(cp_fm_type), ALLOCATABLE, DIMENSION(:, :), &
155 INTENT(inout) :: dipole_op_mos_occ
156 TYPE(tddfpt2_control_type), POINTER :: tddfpt_control
157 TYPE(tddfpt_ground_state_mos), DIMENSION(:), &
158 INTENT(in) :: gs_mos
159 TYPE(qs_environment_type), POINTER :: qs_env
160
161 CHARACTER(LEN=*), PARAMETER :: routinen = 'tddfpt_dipole_operator'
162
163 INTEGER :: handle, i_cos_sin, icol, ideriv, irow, &
164 ispin, jderiv, nao, ncols_local, &
165 ndim_periodic, nrows_local, nspins
166 INTEGER, DIMENSION(:), POINTER :: col_indices, row_indices
167 INTEGER, DIMENSION(maxspins) :: nmo_occ, nmo_virt
168 REAL(kind=dp) :: eval_occ
169 REAL(kind=dp), CONTIGUOUS, DIMENSION(:, :), &
170 POINTER :: local_data_ediff, local_data_wfm
171 REAL(kind=dp), DIMENSION(3) :: kvec, reference_point
172 TYPE(cell_type), POINTER :: cell
173 TYPE(cp_blacs_env_type), POINTER :: blacs_env
174 TYPE(cp_cfm_type), ALLOCATABLE, DIMENSION(:) :: gamma_00, gamma_inv_00
175 TYPE(cp_fm_struct_type), POINTER :: fm_struct
176 TYPE(cp_fm_type) :: ediff_inv, wfm_ao_ao, wfm_mo_virt_mo_occ
177 TYPE(cp_fm_type), ALLOCATABLE, DIMENSION(:) :: s_mos_virt
178 TYPE(cp_fm_type), ALLOCATABLE, DIMENSION(:, :) :: dberry_mos_occ, gamma_real_imag, opvec
179 TYPE(dbcsr_p_type), DIMENSION(:), POINTER :: berry_cossin_xyz, matrix_s, rrc_xyz, scrm
180 TYPE(dft_control_type), POINTER :: dft_control
181 TYPE(neighbor_list_set_p_type), DIMENSION(:), &
182 POINTER :: sab_orb
183 TYPE(pw_env_type), POINTER :: pw_env
184 TYPE(pw_poisson_type), POINTER :: poisson_env
185 TYPE(qs_ks_env_type), POINTER :: ks_env
186
187 CALL timeset(routinen, handle)
188
189 NULLIFY (blacs_env, cell, matrix_s, pw_env)
190 CALL get_qs_env(qs_env, blacs_env=blacs_env, cell=cell, matrix_s=matrix_s, pw_env=pw_env)
191
192 nspins = SIZE(gs_mos)
193 CALL dbcsr_get_info(matrix_s(1)%matrix, nfullrows_total=nao)
194 DO ispin = 1, nspins
195 nmo_occ(ispin) = SIZE(gs_mos(ispin)%evals_occ)
196 nmo_virt(ispin) = SIZE(gs_mos(ispin)%evals_virt)
197 END DO
198
199 ! +++ allocate dipole operator matrices (must be deallocated elsewhere)
200 ALLOCATE (dipole_op_mos_occ(nderivs, nspins))
201 DO ispin = 1, nspins
202 CALL cp_fm_get_info(gs_mos(ispin)%mos_occ, matrix_struct=fm_struct)
203
204 DO ideriv = 1, nderivs
205 CALL cp_fm_create(dipole_op_mos_occ(ideriv, ispin), fm_struct)
206 END DO
207 END DO
208
209 ! +++ allocate work matrices
210 ALLOCATE (s_mos_virt(nspins))
211 DO ispin = 1, nspins
212 CALL cp_fm_get_info(gs_mos(ispin)%mos_virt, matrix_struct=fm_struct)
213 CALL cp_fm_create(s_mos_virt(ispin), fm_struct)
214 CALL cp_dbcsr_sm_fm_multiply(matrix_s(1)%matrix, &
215 gs_mos(ispin)%mos_virt, &
216 s_mos_virt(ispin), &
217 ncol=nmo_virt(ispin), alpha=1.0_dp, beta=0.0_dp)
218 END DO
219
220 ! check that the chosen dipole operator is consistent with the periodic boundary conditions used
221 CALL pw_env_get(pw_env, poisson_env=poisson_env)
222 ndim_periodic = count(poisson_env%parameters%periodic == 1)
223
224 ! select default for dipole form
225 IF (tddfpt_control%dipole_form == 0) THEN
226 CALL get_qs_env(qs_env, dft_control=dft_control)
227 IF (dft_control%qs_control%xtb) THEN
228 IF (ndim_periodic == 0) THEN
229 tddfpt_control%dipole_form = tddfpt_dipole_length
230 ELSE
231 tddfpt_control%dipole_form = tddfpt_dipole_velocity
232 END IF
233 ELSE
234 tddfpt_control%dipole_form = tddfpt_dipole_velocity
235 END IF
236 END IF
237
238 SELECT CASE (tddfpt_control%dipole_form)
239 CASE (tddfpt_dipole_berry)
240 IF (ndim_periodic /= 3) THEN
241 CALL cp_warn(__location__, &
242 "Fully periodic Poisson solver (PERIODIC xyz) "// &
243 "or a large supercell in non-periodic directions is needed "// &
244 "for oscillator strengths based on the Berry phase formula")
245 END IF
246
247 NULLIFY (berry_cossin_xyz)
248 ! index: 1 = Re[exp(-i * G_t * t)],
249 ! 2 = Im[exp(-i * G_t * t)];
250 ! t = x,y,z
251 CALL dbcsr_allocate_matrix_set(berry_cossin_xyz, 2)
252
253 DO i_cos_sin = 1, 2
254 CALL dbcsr_init_p(berry_cossin_xyz(i_cos_sin)%matrix)
255 CALL dbcsr_copy(berry_cossin_xyz(i_cos_sin)%matrix, matrix_s(1)%matrix)
256 END DO
257
258 ! +++ allocate berry-phase-related work matrices
259 ALLOCATE (gamma_00(nspins), gamma_inv_00(nspins), gamma_real_imag(2, nspins), opvec(2, nspins))
260 ALLOCATE (dberry_mos_occ(nderivs, nspins))
261 DO ispin = 1, nspins
262 NULLIFY (fm_struct)
263 CALL cp_fm_struct_create(fm_struct, nrow_global=nmo_occ(ispin), &
264 ncol_global=nmo_occ(ispin), context=blacs_env)
265
266 CALL cp_cfm_create(gamma_00(ispin), fm_struct)
267 CALL cp_cfm_create(gamma_inv_00(ispin), fm_struct)
268
269 DO i_cos_sin = 1, 2
270 CALL cp_fm_create(gamma_real_imag(i_cos_sin, ispin), fm_struct)
271 END DO
272 CALL cp_fm_struct_release(fm_struct)
273
274 ! G_real C_0, G_imag C_0
275 CALL cp_fm_get_info(gs_mos(ispin)%mos_occ, matrix_struct=fm_struct)
276 DO i_cos_sin = 1, 2
277 CALL cp_fm_create(opvec(i_cos_sin, ispin), fm_struct)
278 END DO
279
280 ! dBerry * C_0
281 DO ideriv = 1, nderivs
282 CALL cp_fm_create(dberry_mos_occ(ideriv, ispin), fm_struct)
283 CALL cp_fm_set_all(dberry_mos_occ(ideriv, ispin), 0.0_dp)
284 END DO
285 END DO
286
287 DO ideriv = 1, nderivs
288 kvec(:) = twopi*cell%h_inv(ideriv, :)
289 DO i_cos_sin = 1, 2
290 CALL dbcsr_set(berry_cossin_xyz(i_cos_sin)%matrix, 0.0_dp)
291 END DO
292 CALL build_berry_moment_matrix(qs_env, berry_cossin_xyz(1)%matrix, &
293 berry_cossin_xyz(2)%matrix, kvec)
294
295 DO ispin = 1, nspins
296 ! i_cos_sin = 1: cos (real) component; opvec(1) = gamma_real C_0
297 ! i_cos_sin = 2: sin (imaginary) component; opvec(2) = gamma_imag C_0
298 DO i_cos_sin = 1, 2
299 CALL cp_dbcsr_sm_fm_multiply(berry_cossin_xyz(i_cos_sin)%matrix, &
300 gs_mos(ispin)%mos_occ, &
301 opvec(i_cos_sin, ispin), &
302 ncol=nmo_occ(ispin), alpha=1.0_dp, beta=0.0_dp)
303 END DO
304
305 CALL parallel_gemm('T', 'N', nmo_occ(ispin), nmo_occ(ispin), nao, &
306 1.0_dp, gs_mos(ispin)%mos_occ, opvec(1, ispin), &
307 0.0_dp, gamma_real_imag(1, ispin))
308
309 CALL parallel_gemm('T', 'N', nmo_occ(ispin), nmo_occ(ispin), nao, &
310 -1.0_dp, gs_mos(ispin)%mos_occ, opvec(2, ispin), &
311 0.0_dp, gamma_real_imag(2, ispin))
312
313 CALL cp_fm_to_cfm(msourcer=gamma_real_imag(1, ispin), &
314 msourcei=gamma_real_imag(2, ispin), &
315 mtarget=gamma_00(ispin))
316
317 ! gamma_inv_00 = Q = [C_0^T (gamma_real - i gamma_imag) C_0] ^ {-1}
318 CALL cp_cfm_set_all(gamma_inv_00(ispin), z_zero, z_one)
319 CALL cp_cfm_solve(gamma_00(ispin), gamma_inv_00(ispin))
320
321 CALL cp_cfm_to_fm(msource=gamma_inv_00(ispin), &
322 mtargetr=gamma_real_imag(1, ispin), &
323 mtargeti=gamma_real_imag(2, ispin))
324
325 ! dBerry_mos_occ is identical to dBerry_psi0 from qs_linres_op % polar_operators()
326 CALL parallel_gemm("N", "N", nao, nmo_occ(ispin), nmo_occ(ispin), &
327 1.0_dp, opvec(1, ispin), gamma_real_imag(2, ispin), &
328 0.0_dp, dipole_op_mos_occ(1, ispin))
329 CALL parallel_gemm("N", "N", nao, nmo_occ(ispin), nmo_occ(ispin), &
330 -1.0_dp, opvec(2, ispin), gamma_real_imag(1, ispin), &
331 1.0_dp, dipole_op_mos_occ(1, ispin))
332
333 DO jderiv = 1, nderivs
334 CALL cp_fm_scale_and_add(1.0_dp, dberry_mos_occ(jderiv, ispin), &
335 cell%hmat(jderiv, ideriv), dipole_op_mos_occ(1, ispin))
336 END DO
337 END DO
338 END DO
339
340 ! --- release berry-phase-related work matrices
341 CALL cp_fm_release(opvec)
342 CALL cp_fm_release(gamma_real_imag)
343 DO ispin = nspins, 1, -1
344 CALL cp_cfm_release(gamma_inv_00(ispin))
345 CALL cp_cfm_release(gamma_00(ispin))
346 END DO
347 DEALLOCATE (gamma_00, gamma_inv_00)
348 CALL dbcsr_deallocate_matrix_set(berry_cossin_xyz)
349
350 ! trans_dipole = 2|e|/|G_mu| * Tr Imag(evects^T * (gamma_real - i gamma_imag) * C_0 * gamma_inv_00) +
351 ! 2|e|/|G_mu| * Tr Imag(C_0^T * (gamma_real - i gamma_imag) * evects * gamma_inv_00) ,
352 !
353 ! Taking into account the symmetry of the matrices 'gamma_real' and 'gamma_imag' and the fact
354 ! that the response wave-function is a real-valued function, the above expression can be simplified as
355 ! trans_dipole = 4|e|/|G_mu| * Tr Imag(evects^T * (gamma_real - i gamma_imag) * C_0 * gamma_inv_00)
356 !
357 ! 1/|G_mu| = |lattice_vector_mu| / (2*pi) .
358 DO ispin = 1, nspins
359
360 DO ideriv = 1, nderivs
361 CALL cp_fm_to_fm(dberry_mos_occ(ideriv, ispin), dipole_op_mos_occ(ideriv, ispin))
362 END DO
363 END DO
364
365 CALL cp_fm_release(wfm_ao_ao)
366 CALL cp_fm_release(dberry_mos_occ)
367
368 CASE (tddfpt_dipole_length)
369 IF (ndim_periodic /= 0) THEN
370 CALL cp_warn(__location__, &
371 "Non-periodic Poisson solver (PERIODIC none) "// &
372 "or a large supercell approach is needed "// &
373 "for oscillator strengths based on the length operator")
374 END IF
375
376 ! compute components of the dipole operator in the length form
377 NULLIFY (rrc_xyz)
378 CALL dbcsr_allocate_matrix_set(rrc_xyz, nderivs)
379
380 DO ideriv = 1, nderivs
381 CALL dbcsr_init_p(rrc_xyz(ideriv)%matrix)
382 CALL dbcsr_copy(rrc_xyz(ideriv)%matrix, matrix_s(1)%matrix)
383 END DO
384
385 CALL get_reference_point(reference_point, qs_env=qs_env, &
386 reference=tddfpt_control%dipole_reference, &
387 ref_point=tddfpt_control%dipole_ref_point)
388
389 CALL rrc_xyz_ao(op=rrc_xyz, qs_env=qs_env, rc=reference_point, order=1, &
390 minimum_image=.false., soft=.false.)
391
392 DO ispin = 1, nspins
393
394 DO ideriv = 1, nderivs
395 CALL cp_dbcsr_sm_fm_multiply(rrc_xyz(ideriv)%matrix, &
396 gs_mos(ispin)%mos_occ, &
397 dipole_op_mos_occ(ideriv, ispin), &
398 ncol=nmo_occ(ispin), alpha=1.0_dp, beta=0.0_dp)
399 END DO
400
401 END DO
402
403 CALL dbcsr_deallocate_matrix_set(rrc_xyz)
404
405 CASE (tddfpt_dipole_velocity)
406 ! generate overlap derivatives
407 CALL get_qs_env(qs_env, ks_env=ks_env, sab_orb=sab_orb)
408 NULLIFY (scrm)
409 CALL build_overlap_matrix(ks_env, matrix_s=scrm, nderivative=1, &
410 basis_type_a="ORB", basis_type_b="ORB", &
411 sab_nl=sab_orb)
412
413 DO ispin = 1, nspins
414 DO ideriv = 1, nderivs
415 CALL cp_dbcsr_sm_fm_multiply(scrm(ideriv + 1)%matrix, &
416 gs_mos(ispin)%mos_occ, &
417 dipole_op_mos_occ(ideriv, ispin), &
418 ncol=nmo_occ(ispin), alpha=1.0_dp, beta=0.0_dp)
419 END DO
420
421 CALL cp_fm_release(wfm_mo_virt_mo_occ)
422 END DO
423 CALL dbcsr_deallocate_matrix_set(scrm)
424
425 CASE (tddfpt_dipole_velocity_old)
426 ! generate overlap derivatives
427 CALL get_qs_env(qs_env, ks_env=ks_env, sab_orb=sab_orb)
428 NULLIFY (scrm)
429 CALL build_overlap_matrix(ks_env, matrix_s=scrm, nderivative=1, &
430 basis_type_a="ORB", basis_type_b="ORB", &
431 sab_nl=sab_orb)
432
433 DO ispin = 1, nspins
434 NULLIFY (fm_struct)
435 CALL cp_fm_struct_create(fm_struct, nrow_global=nmo_virt(ispin), &
436 ncol_global=nmo_occ(ispin), context=blacs_env)
437 CALL cp_fm_create(ediff_inv, fm_struct)
438 CALL cp_fm_create(wfm_mo_virt_mo_occ, fm_struct)
439 CALL cp_fm_struct_release(fm_struct)
440
441 CALL cp_fm_get_info(ediff_inv, nrow_local=nrows_local, ncol_local=ncols_local, &
442 row_indices=row_indices, col_indices=col_indices, local_data=local_data_ediff)
443 CALL cp_fm_get_info(wfm_mo_virt_mo_occ, local_data=local_data_wfm)
444
445!$OMP PARALLEL DO DEFAULT(NONE), &
446!$OMP PRIVATE(eval_occ, icol, irow), &
447!$OMP SHARED(col_indices, gs_mos, ispin, local_data_ediff, ncols_local, nrows_local, row_indices)
448 DO icol = 1, ncols_local
449 ! E_occ_i ; imo_occ = col_indices(icol)
450 eval_occ = gs_mos(ispin)%evals_occ(col_indices(icol))
451
452 DO irow = 1, nrows_local
453 ! ediff_inv_weights(a, i) = 1.0 / (E_virt_a - E_occ_i)
454 ! imo_virt = row_indices(irow)
455 local_data_ediff(irow, icol) = 1.0_dp/(gs_mos(ispin)%evals_virt(row_indices(irow)) - eval_occ)
456 END DO
457 END DO
458!$OMP END PARALLEL DO
459
460 DO ideriv = 1, nderivs
461 CALL cp_dbcsr_sm_fm_multiply(scrm(ideriv + 1)%matrix, &
462 gs_mos(ispin)%mos_occ, &
463 dipole_op_mos_occ(ideriv, ispin), &
464 ncol=nmo_occ(ispin), alpha=1.0_dp, beta=0.0_dp)
465
466 CALL parallel_gemm('T', 'N', nmo_virt(ispin), nmo_occ(ispin), nao, &
467 1.0_dp, gs_mos(ispin)%mos_virt, dipole_op_mos_occ(ideriv, ispin), &
468 0.0_dp, wfm_mo_virt_mo_occ)
469
470 ! in-place element-wise (Schur) product;
471 ! avoid allocation of a temporary [nmo_virt x nmo_occ] matrix which is needed
472 ! for cp_fm_schur_product() subroutine call
473
474!$OMP PARALLEL DO DEFAULT(NONE), &
475!$OMP PRIVATE(icol, irow), &
476!$OMP SHARED(ispin, local_data_ediff, local_data_wfm, ncols_local, nrows_local)
477 DO icol = 1, ncols_local
478 DO irow = 1, nrows_local
479 local_data_wfm(irow, icol) = local_data_wfm(irow, icol)*local_data_ediff(irow, icol)
480 END DO
481 END DO
482!$OMP END PARALLEL DO
483
484 CALL parallel_gemm('N', 'N', nao, nmo_occ(ispin), nmo_virt(ispin), &
485 1.0_dp, s_mos_virt(ispin), wfm_mo_virt_mo_occ, &
486 0.0_dp, dipole_op_mos_occ(ideriv, ispin))
487 END DO
488
489 CALL cp_fm_release(wfm_mo_virt_mo_occ)
490 CALL cp_fm_release(ediff_inv)
491 END DO
492 CALL dbcsr_deallocate_matrix_set(scrm)
493
494 CASE DEFAULT
495 cpabort("Unimplemented form of the dipole operator")
496 END SELECT
497
498 ! --- release work matrices
499 CALL cp_fm_release(s_mos_virt)
500
501 CALL timestop(handle)
502 END SUBROUTINE tddfpt_dipole_operator
503
504! **************************************************************************************************
505!> \brief Print final TDDFPT excitation energies and oscillator strengths.
506!> \param log_unit output unit
507!> \param evects TDDFPT trial vectors (SIZE(evects,1) -- number of spins;
508!> SIZE(evects,2) -- number of excited states to print)
509!> \param evals TDDFPT eigenvalues
510!> \param gs_mos ...
511!> \param ostrength TDDFPT oscillator strength
512!> \param mult multiplicity
513!> \param dipole_op_mos_occ action of the dipole operator on the ground state wave function
514!> [x,y,z ; spin]
515!> \param dipole_form ...
516!> \par History
517!> * 05.2016 created [Sergey Chulkov]
518!> * 06.2016 transition dipole moments and oscillator strengths [Sergey Chulkov]
519!> * 07.2016 spin-unpolarised electron density [Sergey Chulkov]
520!> * 08.2018 compute 'dipole_op_mos_occ' in a separate subroutine [Sergey Chulkov]
521!> \note \parblock
522!> Adapted version of the subroutine find_contributions() which was originally created
523!> by Thomas Chassaing on 02.2005.
524!>
525!> Transition dipole moment along direction 'd' is computed as following:
526!> \f[ t_d(spin) = Tr[evects^T dipole\_op\_mos\_occ(d, spin)] .\f]
527!> \endparblock
528! **************************************************************************************************
529 SUBROUTINE tddfpt_print_summary(log_unit, evects, evals, gs_mos, ostrength, mult, &
530 dipole_op_mos_occ, dipole_form)
531 INTEGER, INTENT(in) :: log_unit
532 TYPE(cp_fm_type), DIMENSION(:, :), INTENT(in) :: evects
533 REAL(kind=dp), DIMENSION(:), INTENT(in) :: evals
534 TYPE(tddfpt_ground_state_mos), DIMENSION(:), &
535 POINTER :: gs_mos
536 REAL(kind=dp), DIMENSION(:), INTENT(inout) :: ostrength
537 INTEGER, INTENT(in) :: mult
538 TYPE(cp_fm_type), DIMENSION(:, :), INTENT(in) :: dipole_op_mos_occ
539 INTEGER, INTENT(in) :: dipole_form
540
541 CHARACTER(LEN=*), PARAMETER :: routinen = 'tddfpt_print_summary'
542
543 CHARACTER(len=1) :: lsd_str
544 CHARACTER(len=20) :: mult_str
545 INTEGER :: handle, i, ideriv, ispin, istate, j, &
546 nactive, nao, nocc, nspins, nstates
547 REAL(kind=dp) :: osc_strength
548 REAL(kind=dp), ALLOCATABLE, DIMENSION(:, :, :) :: trans_dipoles
549 TYPE(cp_fm_struct_type), POINTER :: matrix_struct
550 TYPE(cp_fm_type) :: dipact
551
552 CALL timeset(routinen, handle)
553
554 nspins = SIZE(evects, 1)
555 nstates = SIZE(evects, 2)
556
557 IF (nspins > 1) THEN
558 lsd_str = 'U'
559 ELSE
560 lsd_str = 'R'
561 END IF
562
563 ! *** summary header ***
564 IF (log_unit > 0) THEN
565 CALL integer_to_string(mult, mult_str)
566 WRITE (log_unit, '(/,1X,A1,A,1X,A)') lsd_str, "-TDDFPT states of multiplicity", trim(mult_str)
567 SELECT CASE (dipole_form)
568 CASE (tddfpt_dipole_berry)
569 WRITE (log_unit, '(1X,A,/)') "Transition dipoles calculated using Berry operator formulation"
570 CASE (tddfpt_dipole_length)
571 WRITE (log_unit, '(1X,A,/)') "Transition dipoles calculated using length formulation"
572 CASE (tddfpt_dipole_velocity)
573 WRITE (log_unit, '(1X,A,/)') "Transition dipoles calculated using velocity formulation"
574 CASE (tddfpt_dipole_velocity_old)
575 WRITE (log_unit, '(1X,A,/)') "Transition dipoles calculated using old velocity formulation"
576 CASE (tddfpt_dipole_scf_moment)
577 WRITE (log_unit, '(1X,A,/)') "Transition dipoles calculated using SCF-MO moment formulation"
578 CASE DEFAULT
579 cpabort("Unimplemented form of the dipole operator")
580 END SELECT
581
582 WRITE (log_unit, '(T10,A,T19,A,T37,A,T69,A)') "State", "Excitation", &
583 "Transition dipole (a.u.)", "Oscillator"
584 WRITE (log_unit, '(T10,A,T19,A,T37,A,T49,A,T61,A,T67,A)') "number", "energy (eV)", &
585 "x", "y", "z", "strength (a.u.)"
586 WRITE (log_unit, '(T10,72("-"))')
587 END IF
588
589 ! transition dipole moment
590 ALLOCATE (trans_dipoles(nstates, nderivs, nspins))
591 trans_dipoles(:, :, :) = 0.0_dp
592
593 ! nspins == 1 .AND. mult == 3 : spin-flip transitions are forbidden due to symmetry reasons
594 IF (nspins > 1 .OR. mult == 1) THEN
595 DO ispin = 1, nspins
596 CALL cp_fm_get_info(dipole_op_mos_occ(1, ispin), nrow_global=nao, ncol_global=nocc)
597 CALL cp_fm_get_info(evects(ispin, 1), ncol_global=nactive)
598 IF (nocc == nactive) THEN
599 DO ideriv = 1, nderivs
600 CALL cp_fm_trace(evects(ispin, :), dipole_op_mos_occ(ideriv, ispin), &
601 trans_dipoles(:, ideriv, ispin))
602 END DO
603 ELSE ! res
604 CALL cp_fm_get_info(evects(ispin, 1), matrix_struct=matrix_struct)
605 CALL cp_fm_create(dipact, matrix_struct)
606 DO ideriv = 1, nderivs
607 DO i = 1, nactive
608 j = gs_mos(ispin)%index_active(i)
609 CALL cp_fm_to_fm(dipole_op_mos_occ(ideriv, ispin), dipact, &
610 ncol=1, source_start=j, target_start=i)
611 END DO
612 CALL cp_fm_trace(evects(ispin, :), dipact, trans_dipoles(:, ideriv, ispin))
613 END DO
614 CALL cp_fm_release(dipact)
615 END IF
616 END DO
617
618 IF (nspins == 1) THEN
619 trans_dipoles(:, :, 1) = sqrt(2.0_dp)*trans_dipoles(:, :, 1)
620 ELSE
621 trans_dipoles(:, :, 1) = trans_dipoles(:, :, 1) + trans_dipoles(:, :, 2)
622 END IF
623 END IF
624
625 ! *** summary information ***
626 DO istate = 1, nstates
627
628 SELECT CASE (dipole_form)
629 CASE (tddfpt_dipole_berry)
630 osc_strength = 2.0_dp/3.0_dp*evals(istate)*sum(trans_dipoles(istate, :, 1)**2)
631 CASE (tddfpt_dipole_length)
632 osc_strength = 2.0_dp/3.0_dp*evals(istate)*sum(trans_dipoles(istate, :, 1)**2)
633 CASE (tddfpt_dipole_velocity)
634 osc_strength = 2.0_dp/3.0_dp/evals(istate)*sum(trans_dipoles(istate, :, 1)**2)
635 CASE (tddfpt_dipole_velocity_old)
636 osc_strength = 2.0_dp/3.0_dp*evals(istate)*sum(trans_dipoles(istate, :, 1)**2)
637 CASE DEFAULT
638 cpabort("Unimplemented form of the dipole operator")
639 END SELECT
640
641 ostrength(istate) = osc_strength
642 IF (log_unit > 0) THEN
643 WRITE (log_unit, '(1X,A,T9,I7,T19,F11.5,T31,3(1X,ES11.4E2),T69,ES12.5E2)') &
644 "TDDFPT|", istate, evals(istate)*evolt, trans_dipoles(istate, 1:nderivs, 1), osc_strength
645 END IF
646 END DO
647
648 ! punch a checksum for the regs
649 IF (log_unit > 0) THEN
650 WRITE (log_unit, '(/,T2,A,E16.8)') 'TDDFPT : CheckSum E = ', sqrt(sum(evals**2))
651 WRITE (log_unit, '(/,T2,A,E16.8)') 'TDDFPT : CheckSum F = ', sqrt(sum(ostrength**2))
652 END IF
653
654 DEALLOCATE (trans_dipoles)
655
656 CALL timestop(handle)
657 END SUBROUTINE tddfpt_print_summary
658
659! **************************************************************************************************
660!> \brief Print excitation analysis.
661!> \param log_unit output unit
662!> \param evects TDDFPT trial vectors (SIZE(evects,1) -- number of spins;
663!> SIZE(evects,2) -- number of excited states to print)
664!> \param evals TDDFPT eigenvalues
665!> \param gs_mos molecular orbitals optimised for the ground state
666!> \param matrix_s overlap matrix
667!> \param spinflip ...
668!> \param min_amplitude the smallest excitation amplitude to print
669!> \par History
670!> * 05.2016 created as 'tddfpt_print_summary' [Sergey Chulkov]
671!> * 08.2018 splited of from 'tddfpt_print_summary' [Sergey Chulkov]
672! **************************************************************************************************
673 SUBROUTINE tddfpt_print_excitation_analysis(log_unit, evects, evals, gs_mos, matrix_s, spinflip, &
674 min_amplitude)
675 INTEGER, INTENT(in) :: log_unit
676 TYPE(cp_fm_type), DIMENSION(:, :), INTENT(in) :: evects
677 REAL(kind=dp), DIMENSION(:), INTENT(in) :: evals
678 TYPE(tddfpt_ground_state_mos), DIMENSION(:), &
679 INTENT(in) :: gs_mos
680 TYPE(dbcsr_type), POINTER :: matrix_s
681 INTEGER :: spinflip
682 REAL(kind=dp), INTENT(in) :: min_amplitude
683
684 CHARACTER(LEN=*), PARAMETER :: routinen = 'tddfpt_print_excitation_analysis'
685
686 CHARACTER(len=5) :: spin_label, spin_label2
687 INTEGER :: handle, icol, iproc, irow, ispin, &
688 istate, nao, ncols_local, nrows_local, &
689 nspins, nstates, spin2, state_spin, &
690 state_spin2
691 INTEGER(kind=int_8) :: iexc, imo_act, imo_occ, imo_virt, ind, &
692 nexcs, nexcs_local, nexcs_max_local, &
693 nmo_virt_occ, nmo_virt_occ_alpha
694 INTEGER(kind=int_8), ALLOCATABLE, DIMENSION(:) :: inds_local, inds_recv, nexcs_recv
695 INTEGER(kind=int_8), DIMENSION(1) :: nexcs_send
696 INTEGER(kind=int_8), DIMENSION(maxspins) :: nactive8, nmo_occ8, nmo_virt8
697 INTEGER, ALLOCATABLE, DIMENSION(:) :: inds
698 INTEGER, DIMENSION(:), POINTER :: col_indices, row_indices
699 INTEGER, DIMENSION(maxspins) :: nactive, nmo_occ, nmo_virt
700 LOGICAL :: do_exc_analysis
701 REAL(kind=dp), ALLOCATABLE, DIMENSION(:) :: weights_local, weights_neg_abs_recv, &
702 weights_recv
703 REAL(kind=dp), CONTIGUOUS, DIMENSION(:, :), &
704 POINTER :: local_data
705 TYPE(cp_blacs_env_type), POINTER :: blacs_env
706 TYPE(cp_fm_struct_type), POINTER :: fm_struct
707 TYPE(cp_fm_type), ALLOCATABLE, DIMENSION(:) :: s_mos_virt, weights_fm
708 TYPE(mp_para_env_type), POINTER :: para_env
709 TYPE(mp_request_type) :: send_handler, send_handler2
710 TYPE(mp_request_type), ALLOCATABLE, DIMENSION(:) :: recv_handlers, recv_handlers2
711
712 CALL timeset(routinen, handle)
713
714 nspins = SIZE(gs_mos, 1)
715 nstates = SIZE(evects, 2)
716 do_exc_analysis = min_amplitude < 1.0_dp
717
718 CALL cp_fm_get_info(gs_mos(1)%mos_occ, context=blacs_env, para_env=para_env)
719 CALL dbcsr_get_info(matrix_s, nfullrows_total=nao)
720
721 DO ispin = 1, nspins
722 nactive(ispin) = gs_mos(ispin)%nmo_active
723 nactive8(ispin) = int(nactive(ispin), kind=int_8)
724 nmo_occ(ispin) = SIZE(gs_mos(ispin)%evals_occ)
725 nmo_virt(ispin) = SIZE(gs_mos(ispin)%evals_virt)
726 nmo_occ8(ispin) = SIZE(gs_mos(ispin)%evals_occ, kind=int_8)
727 nmo_virt8(ispin) = SIZE(gs_mos(ispin)%evals_virt, kind=int_8)
728 END DO
729
730 ! *** excitation analysis ***
731 IF (do_exc_analysis) THEN
732 cpassert(log_unit <= 0 .OR. para_env%is_source())
733 nmo_virt_occ_alpha = int(nmo_virt(1), int_8)*int(nmo_occ(1), int_8)
734
735 IF (log_unit > 0) THEN
736 WRITE (log_unit, "(1X,A)") "", &
737 "-------------------------------------------------------------------------------", &
738 "- Excitation analysis -", &
739 "-------------------------------------------------------------------------------"
740 WRITE (log_unit, '(8X,A,T27,A,T49,A,T69,A)') "State", "Occupied", "Virtual", "Excitation"
741 WRITE (log_unit, '(8X,A,T28,A,T49,A,T69,A)') "number", "orbital", "orbital", "amplitude"
742 WRITE (log_unit, '(1X,79("-"))')
743
744 IF (nspins == 1) THEN
745 state_spin = 1
746 state_spin2 = 2
747 spin_label = ' '
748 spin_label2 = ' '
749 ELSE IF (spinflip /= no_sf_tddfpt) THEN
750 state_spin = 1
751 state_spin2 = 2
752 spin_label = '(alp)'
753 spin_label2 = '(bet)'
754 END IF
755 END IF
756
757 ALLOCATE (s_mos_virt(SIZE(evects, 1)), weights_fm(SIZE(evects, 1)))
758 DO ispin = 1, SIZE(evects, 1)
759 IF (spinflip == no_sf_tddfpt) THEN
760 spin2 = ispin
761 ELSE
762 spin2 = 2
763 END IF
764 CALL cp_fm_get_info(gs_mos(spin2)%mos_virt, matrix_struct=fm_struct)
765 CALL cp_fm_create(s_mos_virt(ispin), fm_struct)
766 CALL cp_dbcsr_sm_fm_multiply(matrix_s, &
767 gs_mos(spin2)%mos_virt, &
768 s_mos_virt(ispin), &
769 ncol=nmo_virt(spin2), alpha=1.0_dp, beta=0.0_dp)
770
771 NULLIFY (fm_struct)
772 CALL cp_fm_struct_create(fm_struct, nrow_global=nmo_virt(spin2), ncol_global=nactive(ispin), &
773 context=blacs_env)
774 CALL cp_fm_create(weights_fm(ispin), fm_struct)
775 CALL cp_fm_set_all(weights_fm(ispin), 0.0_dp)
776 CALL cp_fm_struct_release(fm_struct)
777 END DO
778
779 nexcs_max_local = 0
780 DO ispin = 1, SIZE(evects, 1)
781 CALL cp_fm_get_info(weights_fm(ispin), nrow_local=nrows_local, ncol_local=ncols_local)
782 nexcs_max_local = nexcs_max_local + int(nrows_local, int_8)*int(ncols_local, int_8)
783 END DO
784
785 ALLOCATE (weights_local(nexcs_max_local), inds_local(nexcs_max_local))
786
787 DO istate = 1, nstates
788 nexcs_local = 0
789 nmo_virt_occ = 0
790
791 ! analyse matrix elements locally and transfer only significant
792 ! excitations to the master node for subsequent ordering
793 DO ispin = 1, SIZE(evects, 1)
794 IF (spinflip == no_sf_tddfpt) THEN
795 spin2 = ispin
796 ELSE
797 spin2 = 2
798 END IF
799 ! compute excitation amplitudes
800 CALL parallel_gemm('T', 'N', nmo_virt(spin2), nactive(ispin), nao, 1.0_dp, s_mos_virt(ispin), &
801 evects(ispin, istate), 0.0_dp, weights_fm(ispin))
802
803 CALL cp_fm_get_info(weights_fm(ispin), nrow_local=nrows_local, ncol_local=ncols_local, &
804 row_indices=row_indices, col_indices=col_indices, local_data=local_data)
805
806 ! locate single excitations with significant amplitudes (>= min_amplitude)
807 DO icol = 1, ncols_local
808 DO irow = 1, nrows_local
809 IF (abs(local_data(irow, icol)) >= min_amplitude) THEN
810 ! number of non-negligible excitations
811 nexcs_local = nexcs_local + 1
812 ! excitation amplitude
813 weights_local(nexcs_local) = local_data(irow, icol)
814 ! index of single excitation (ivirt, iocc, ispin) in compressed form
815 inds_local(nexcs_local) = nmo_virt_occ + int(row_indices(irow), int_8) + &
816 int(col_indices(icol) - 1, int_8)*nmo_virt8(spin2)
817 END IF
818 END DO
819 END DO
820
821 nmo_virt_occ = nmo_virt_occ + nmo_virt8(spin2)*nmo_occ8(ispin)
822 END DO
823
824 IF (para_env%is_source()) THEN
825 ! master node
826 ALLOCATE (nexcs_recv(para_env%num_pe), recv_handlers(para_env%num_pe), recv_handlers2(para_env%num_pe))
827
828 ! collect number of non-negligible excitations from other nodes
829 DO iproc = 1, para_env%num_pe
830 IF (iproc - 1 /= para_env%mepos) THEN
831 CALL para_env%irecv(nexcs_recv(iproc:iproc), iproc - 1, recv_handlers(iproc), 0)
832 ELSE
833 nexcs_recv(iproc) = nexcs_local
834 END IF
835 END DO
836
837 DO iproc = 1, para_env%num_pe
838 IF (iproc - 1 /= para_env%mepos) THEN
839 CALL recv_handlers(iproc)%wait()
840 END IF
841 END DO
842
843 ! compute total number of non-negligible excitations
844 nexcs = 0
845 DO iproc = 1, para_env%num_pe
846 nexcs = nexcs + nexcs_recv(iproc)
847 END DO
848
849 ! receive indices and amplitudes of selected excitations
850 ALLOCATE (weights_recv(nexcs), weights_neg_abs_recv(nexcs))
851 ALLOCATE (inds_recv(nexcs), inds(nexcs))
852
853 nmo_virt_occ = 0
854 DO iproc = 1, para_env%num_pe
855 IF (nexcs_recv(iproc) > 0) THEN
856 IF (iproc - 1 /= para_env%mepos) THEN
857 ! excitation amplitudes
858 CALL para_env%irecv(weights_recv(nmo_virt_occ + 1:nmo_virt_occ + nexcs_recv(iproc)), &
859 iproc - 1, recv_handlers(iproc), 1)
860 ! compressed indices
861 CALL para_env%irecv(inds_recv(nmo_virt_occ + 1:nmo_virt_occ + nexcs_recv(iproc)), &
862 iproc - 1, recv_handlers2(iproc), 2)
863 ELSE
864 ! data on master node
865 weights_recv(nmo_virt_occ + 1:nmo_virt_occ + nexcs_recv(iproc)) = weights_local(1:nexcs_recv(iproc))
866 inds_recv(nmo_virt_occ + 1:nmo_virt_occ + nexcs_recv(iproc)) = inds_local(1:nexcs_recv(iproc))
867 END IF
868
869 nmo_virt_occ = nmo_virt_occ + nexcs_recv(iproc)
870 END IF
871 END DO
872
873 DO iproc = 1, para_env%num_pe
874 IF (iproc - 1 /= para_env%mepos .AND. nexcs_recv(iproc) > 0) THEN
875 CALL recv_handlers(iproc)%wait()
876 CALL recv_handlers2(iproc)%wait()
877 END IF
878 END DO
879
880 DEALLOCATE (nexcs_recv, recv_handlers, recv_handlers2)
881 ELSE
882 ! working node: send the number of selected excited states to the master node
883 nexcs_send(1) = nexcs_local
884 CALL para_env%isend(nexcs_send, para_env%source, send_handler, 0)
885 CALL send_handler%wait()
886
887 IF (nexcs_local > 0) THEN
888 ! send excitation amplitudes
889 CALL para_env%isend(weights_local(1:nexcs_local), para_env%source, send_handler, 1)
890 ! send compressed indices
891 CALL para_env%isend(inds_local(1:nexcs_local), para_env%source, send_handler2, 2)
892
893 CALL send_handler%wait()
894 CALL send_handler2%wait()
895 END IF
896 END IF
897
898 ! sort non-negligible excitations on the master node according to their amplitudes,
899 ! uncompress indices and print summary information
900 IF (para_env%is_source() .AND. log_unit > 0) THEN
901 weights_neg_abs_recv(:) = -abs(weights_recv)
902 CALL sort(weights_neg_abs_recv, int(nexcs), inds)
903
904 WRITE (log_unit, '(T7,I8,F10.5,A)') istate, evals(istate)*evolt, " eV"
905
906 ! This reinitialization is needed to prevent the intel fortran compiler from introduce
907 ! a bug when using optimization level 3 flag
908 state_spin = 1
909 state_spin2 = 1
910 IF (spinflip /= no_sf_tddfpt) THEN
911 state_spin = 1
912 state_spin2 = 2
913 END IF
914 DO iexc = 1, nexcs
915 ind = inds_recv(inds(iexc)) - 1
916 IF ((nspins > 1) .AND. (spinflip == no_sf_tddfpt)) THEN
917 IF (ind < nmo_virt_occ_alpha) THEN
918 state_spin = 1
919 state_spin2 = 1
920 spin_label = '(alp)'
921 spin_label2 = '(alp)'
922 ELSE
923 state_spin = 2
924 state_spin2 = 2
925 ind = ind - nmo_virt_occ_alpha
926 spin_label = '(bet)'
927 spin_label2 = '(bet)'
928 END IF
929 END IF
930 imo_act = ind/nmo_virt8(state_spin2) + 1
931 imo_occ = gs_mos(state_spin)%index_active(imo_act)
932 imo_virt = mod(ind, nmo_virt8(state_spin2)) + 1
933
934 WRITE (log_unit, '(T27,I8,1X,A5,T48,I8,1X,A5,T70,F9.6)') imo_occ, spin_label, &
935 nmo_occ8(state_spin2) + imo_virt, spin_label2, weights_recv(inds(iexc))
936 END DO
937 END IF
938
939 ! deallocate temporary arrays
940 IF (para_env%is_source()) THEN
941 DEALLOCATE (weights_recv, weights_neg_abs_recv, inds_recv, inds)
942 END IF
943 END DO
944
945 DEALLOCATE (weights_local, inds_local)
946 IF (log_unit > 0) THEN
947 WRITE (log_unit, "(1X,A)") &
948 "-------------------------------------------------------------------------------"
949 END IF
950 END IF
951
952 CALL cp_fm_release(weights_fm)
953 CALL cp_fm_release(s_mos_virt)
954
955 CALL timestop(handle)
956
957 END SUBROUTINE tddfpt_print_excitation_analysis
958
959! **************************************************************************************************
960!> \brief Print natural transition orbital analysis.
961!> \param qs_env Information on Kinds and Particles
962!> \param evects TDDFPT trial vectors (SIZE(evects,1) -- number of spins;
963!> SIZE(evects,2) -- number of excited states to print)
964!> \param evals TDDFPT eigenvalues
965!> \param ostrength ...
966!> \param gs_mos molecular orbitals optimised for the ground state
967!> \param matrix_s overlap matrix
968!> \param print_section ...
969!> \par History
970!> * 06.2019 created [JGH]
971! **************************************************************************************************
972 SUBROUTINE tddfpt_print_nto_analysis(qs_env, evects, evals, ostrength, gs_mos, matrix_s, print_section)
973 TYPE(qs_environment_type), POINTER :: qs_env
974 TYPE(cp_fm_type), DIMENSION(:, :), INTENT(in) :: evects
975 REAL(kind=dp), DIMENSION(:), INTENT(in) :: evals, ostrength
976 TYPE(tddfpt_ground_state_mos), DIMENSION(:), &
977 INTENT(in) :: gs_mos
978 TYPE(dbcsr_type), POINTER :: matrix_s
979 TYPE(section_vals_type), POINTER :: print_section
980
981 CHARACTER(LEN=*), PARAMETER :: routinen = 'tddfpt_print_nto_analysis'
982 INTEGER, PARAMETER :: ntomax = 10
983
984 CHARACTER(LEN=20), DIMENSION(2) :: nto_name
985 INTEGER :: handle, i, ia, icg, iounit, ispin, &
986 istate, j, nao, nlist, nmax, nmo, &
987 nnto, nspins, nstates
988 INTEGER, DIMENSION(2) :: iv
989 INTEGER, DIMENSION(2, ntomax) :: ia_index
990 INTEGER, DIMENSION(:), POINTER :: slist, stride
991 LOGICAL :: append_cube, cube_file, explicit
992 REAL(kind=dp) :: os_threshold, sume, threshold
993 REAL(kind=dp), ALLOCATABLE, DIMENSION(:) :: eigvals
994 REAL(kind=dp), ALLOCATABLE, DIMENSION(:, :) :: eigenvalues
995 REAL(kind=dp), DIMENSION(ntomax) :: ia_eval
996 TYPE(cell_type), POINTER :: cell
997 TYPE(cp_fm_struct_type), POINTER :: fm_mo_struct, fm_struct
998 TYPE(cp_fm_type) :: sev, smat, tmat, wmat, work, wvec
999 TYPE(cp_fm_type), ALLOCATABLE, DIMENSION(:) :: teig
1000 TYPE(cp_logger_type), POINTER :: logger
1001 TYPE(mo_set_type), ALLOCATABLE, DIMENSION(:) :: nto_set
1002 TYPE(particle_type), DIMENSION(:), POINTER :: particle_set
1003 TYPE(qs_kind_type), DIMENSION(:), POINTER :: qs_kind_set
1004 TYPE(section_vals_type), POINTER :: molden_section, nto_section
1005
1006 CALL timeset(routinen, handle)
1007
1008 logger => cp_get_default_logger()
1009 iounit = cp_logger_get_default_io_unit(logger)
1010
1011 IF (btest(cp_print_key_should_output(logger%iter_info, print_section, &
1012 "NTO_ANALYSIS"), cp_p_file)) THEN
1013
1014 CALL cite_reference(martin2003)
1015
1016 CALL section_vals_val_get(print_section, "NTO_ANALYSIS%THRESHOLD", r_val=threshold)
1017 CALL section_vals_val_get(print_section, "NTO_ANALYSIS%INTENSITY_THRESHOLD", r_val=os_threshold)
1018 CALL section_vals_val_get(print_section, "NTO_ANALYSIS%STATE_LIST", explicit=explicit)
1019
1020 IF (explicit) THEN
1021 CALL section_vals_val_get(print_section, "NTO_ANALYSIS%STATE_LIST", i_vals=slist)
1022 nlist = SIZE(slist)
1023 ELSE
1024 nlist = 0
1025 END IF
1026
1027 IF (iounit > 0) THEN
1028 WRITE (iounit, "(1X,A)") "", &
1029 "-------------------------------------------------------------------------------", &
1030 "- Natural Orbital analysis -", &
1031 "-------------------------------------------------------------------------------"
1032 END IF
1033
1034 nspins = SIZE(evects, 1)
1035 nstates = SIZE(evects, 2)
1036 CALL dbcsr_get_info(matrix_s, nfullrows_total=nao)
1037
1038 DO istate = 1, nstates
1039 IF (os_threshold > ostrength(istate)) THEN
1040 IF (iounit > 0) THEN
1041 WRITE (iounit, "(1X,A,I6)") " Skipping state ", istate
1042 END IF
1043 cycle
1044 END IF
1045 IF (nlist > 0) THEN
1046 IF (.NOT. any(slist == istate)) THEN
1047 IF (iounit > 0) THEN
1048 WRITE (iounit, "(1X,A,I6)") " Skipping state ", istate
1049 END IF
1050 cycle
1051 END IF
1052 END IF
1053 IF (iounit > 0) THEN
1054 WRITE (iounit, "(1X,A,I6,T30,F10.5,A)") " STATE NR. ", istate, evals(istate)*evolt, " eV"
1055 END IF
1056 nmax = 0
1057 DO ispin = 1, nspins
1058 CALL cp_fm_get_info(evects(ispin, istate), matrix_struct=fm_struct, ncol_global=nmo)
1059 nmax = max(nmax, nmo)
1060 END DO
1061 ALLOCATE (eigenvalues(nmax, nspins))
1062 eigenvalues = 0.0_dp
1063 ! SET 1: Hole states
1064 ! SET 2: Particle states
1065 nto_name(1) = 'Hole_states'
1066 nto_name(2) = 'Particle_states'
1067 ALLOCATE (nto_set(2))
1068 DO i = 1, 2
1069 CALL allocate_mo_set(nto_set(i), nao, ntomax, 0, 0.0_dp, 1.0_dp, 0.0_dp)
1070 CALL cp_fm_get_info(evects(1, istate), matrix_struct=fm_struct)
1071 CALL cp_fm_struct_create(fmstruct=fm_mo_struct, template_fmstruct=fm_struct, &
1072 ncol_global=ntomax)
1073 CALL cp_fm_create(tmat, fm_mo_struct)
1074 CALL init_mo_set(nto_set(i), fm_ref=tmat, name=nto_name(i))
1075 CALL cp_fm_release(tmat)
1076 CALL cp_fm_struct_release(fm_mo_struct)
1077 END DO
1078 !
1079 ALLOCATE (teig(nspins))
1080 ! hole states
1081 ! Diagonalize X(T)*S*X
1082 DO ispin = 1, nspins
1083 associate(ev => evects(ispin, istate))
1084 CALL cp_fm_get_info(ev, matrix_struct=fm_struct, ncol_global=nmo)
1085 CALL cp_fm_create(sev, fm_struct)
1086 CALL cp_fm_struct_create(fmstruct=fm_mo_struct, template_fmstruct=fm_struct, &
1087 nrow_global=nmo, ncol_global=nmo)
1088 CALL cp_fm_create(tmat, fm_mo_struct)
1089 CALL cp_fm_create(teig(ispin), fm_mo_struct)
1090 CALL cp_dbcsr_sm_fm_multiply(matrix_s, ev, sev, ncol=nmo, alpha=1.0_dp, beta=0.0_dp)
1091 CALL parallel_gemm('T', 'N', nmo, nmo, nao, 1.0_dp, ev, sev, 0.0_dp, tmat)
1092 END associate
1093
1094 CALL choose_eigv_solver(tmat, teig(ispin), eigenvalues(1:nmo, ispin))
1095
1096 CALL cp_fm_struct_release(fm_mo_struct)
1097 CALL cp_fm_release(tmat)
1098 CALL cp_fm_release(sev)
1099 END DO
1100 ! find major determinants i->a
1101 ia_index = 0
1102 sume = 0.0_dp
1103 nnto = 0
1104 DO i = 1, ntomax
1105 iv = maxloc(eigenvalues)
1106 ia_eval(i) = eigenvalues(iv(1), iv(2))
1107 ia_index(1:2, i) = iv(1:2)
1108 sume = sume + ia_eval(i)
1109 eigenvalues(iv(1), iv(2)) = 0.0_dp
1110 nnto = nnto + 1
1111 IF (sume > threshold) EXIT
1112 END DO
1113 ! store hole states
1114 CALL set_mo_set(nto_set(1), nmo=nnto)
1115 DO i = 1, nnto
1116 ia = ia_index(1, i)
1117 ispin = ia_index(2, i)
1118 CALL cp_fm_get_info(gs_mos(ispin)%mos_occ, ncol_global=nmo)
1119 CALL cp_fm_get_info(teig(ispin), matrix_struct=fm_struct)
1120 CALL cp_fm_struct_create(fmstruct=fm_mo_struct, template_fmstruct=fm_struct, &
1121 nrow_global=nmo, ncol_global=1)
1122 CALL cp_fm_create(tmat, fm_mo_struct)
1123 CALL cp_fm_struct_release(fm_mo_struct)
1124 CALL cp_fm_get_info(gs_mos(1)%mos_occ, matrix_struct=fm_struct)
1125 CALL cp_fm_struct_create(fmstruct=fm_mo_struct, template_fmstruct=fm_struct, &
1126 ncol_global=1)
1127 CALL cp_fm_create(wvec, fm_mo_struct)
1128 CALL cp_fm_struct_release(fm_mo_struct)
1129 CALL cp_fm_to_fm(teig(ispin), tmat, 1, ia, 1)
1130 CALL parallel_gemm('N', 'N', nao, 1, nmo, 1.0_dp, gs_mos(ispin)%mos_occ, &
1131 tmat, 0.0_dp, wvec)
1132 CALL cp_fm_to_fm(wvec, nto_set(1)%mo_coeff, 1, 1, i)
1133 CALL cp_fm_release(wvec)
1134 CALL cp_fm_release(tmat)
1135 END DO
1136 ! particle states
1137 ! Solve generalized eigenvalue equation: (S*X)*(S*X)(T)*v = lambda*S*v
1138 CALL set_mo_set(nto_set(2), nmo=nnto)
1139 DO ispin = 1, nspins
1140 associate(ev => evects(ispin, istate))
1141 CALL cp_fm_get_info(ev, matrix_struct=fm_struct, nrow_global=nao, ncol_global=nmo)
1142 ALLOCATE (eigvals(nao))
1143 eigvals = 0.0_dp
1144 CALL cp_fm_create(sev, fm_struct)
1145 CALL cp_dbcsr_sm_fm_multiply(matrix_s, ev, sev, ncol=nmo, alpha=1.0_dp, beta=0.0_dp)
1146 END associate
1147 CALL cp_fm_struct_create(fmstruct=fm_mo_struct, template_fmstruct=fm_struct, &
1148 nrow_global=nao, ncol_global=nao)
1149 CALL cp_fm_create(tmat, fm_mo_struct)
1150 CALL cp_fm_create(smat, fm_mo_struct)
1151 CALL cp_fm_create(wmat, fm_mo_struct)
1152 CALL cp_fm_create(work, fm_mo_struct)
1153 CALL cp_fm_struct_release(fm_mo_struct)
1154 CALL copy_dbcsr_to_fm(matrix_s, smat)
1155 CALL parallel_gemm('N', 'T', nao, nao, nmo, 1.0_dp, sev, sev, 0.0_dp, tmat)
1156 CALL cp_fm_geeig(tmat, smat, wmat, eigvals, work)
1157 DO i = 1, nnto
1158 IF (ispin == ia_index(2, i)) THEN
1159 icg = 0
1160 DO j = 1, nao
1161 IF (abs(eigvals(j) - ia_eval(i)) < 1.e-6_dp) THEN
1162 icg = j
1163 EXIT
1164 END IF
1165 END DO
1166 IF (icg == 0) THEN
1167 CALL cp_warn(__location__, &
1168 "Could not locate particle state associated with hole state.")
1169 ELSE
1170 CALL cp_fm_to_fm(wmat, nto_set(2)%mo_coeff, 1, icg, i)
1171 END IF
1172 END IF
1173 END DO
1174 DEALLOCATE (eigvals)
1175 CALL cp_fm_release(sev)
1176 CALL cp_fm_release(tmat)
1177 CALL cp_fm_release(smat)
1178 CALL cp_fm_release(wmat)
1179 CALL cp_fm_release(work)
1180 END DO
1181 ! print
1182 IF (iounit > 0) THEN
1183 sume = 0.0_dp
1184 DO i = 1, nnto
1185 sume = sume + ia_eval(i)
1186 WRITE (iounit, "(T6,A,i2,T30,A,i1,T42,A,F8.5,T63,A,F8.5)") &
1187 "Particle-Hole state:", i, " Spin:", ia_index(2, i), &
1188 "Eigenvalue:", ia_eval(i), " Sum Eigv:", sume
1189 END DO
1190 END IF
1191 ! Cube and Molden files
1192 nto_section => section_vals_get_subs_vals(print_section, "NTO_ANALYSIS")
1193 CALL section_vals_val_get(nto_section, "CUBE_FILES", l_val=cube_file)
1194 CALL section_vals_val_get(nto_section, "STRIDE", i_vals=stride)
1195 CALL section_vals_val_get(nto_section, "APPEND", l_val=append_cube)
1196 IF (cube_file) THEN
1197 CALL print_nto_cubes(qs_env, nto_set, istate, stride, append_cube, nto_section)
1198 END IF
1199 CALL get_qs_env(qs_env, qs_kind_set=qs_kind_set, particle_set=particle_set, cell=cell)
1200 molden_section => section_vals_get_subs_vals(print_section, "MOS_MOLDEN")
1201 CALL write_mos_molden(nto_set, qs_kind_set, particle_set, molden_section, cell=cell, qs_env=qs_env)
1202 !
1203 DEALLOCATE (eigenvalues)
1204 CALL cp_fm_release(teig)
1205 !
1206 DO i = 1, 2
1207 CALL deallocate_mo_set(nto_set(i))
1208 END DO
1209 DEALLOCATE (nto_set)
1210 END DO
1211
1212 IF (iounit > 0) THEN
1213 WRITE (iounit, "(1X,A)") &
1214 "-------------------------------------------------------------------------------"
1215 END IF
1216
1217 END IF
1218
1219 CALL timestop(handle)
1220
1221 END SUBROUTINE tddfpt_print_nto_analysis
1222
1223! **************************************************************************************************
1224!> \brief Print exciton descriptors, cf. Mewes et al., JCTC 14, 710-725 (2018)
1225!> \param log_unit output unit
1226!> \param evects TDDFPT trial vectors (SIZE(evects,1) -- number of spins;
1227!> SIZE(evects,2) -- number of excited states to print)
1228!> \param gs_mos molecular orbitals optimised for the ground state
1229!> \param matrix_s overlap matrix
1230!> \param do_directional_exciton_descriptors flag for computing descriptors for each (cartesian) direction
1231!> \param qs_env Information on particles/geometry
1232!> \par History
1233!> * 12.2024 created as 'tddfpt_print_exciton_descriptors' [Maximilian Graml]
1234! **************************************************************************************************
1235 SUBROUTINE tddfpt_print_exciton_descriptors(log_unit, evects, gs_mos, matrix_s, &
1236 do_directional_exciton_descriptors, qs_env)
1237 INTEGER, INTENT(in) :: log_unit
1238 TYPE(cp_fm_type), DIMENSION(:, :), INTENT(in) :: evects
1239 TYPE(tddfpt_ground_state_mos), DIMENSION(:), &
1240 INTENT(in) :: gs_mos
1241 TYPE(dbcsr_type), POINTER :: matrix_s
1242 LOGICAL, INTENT(IN) :: do_directional_exciton_descriptors
1243 TYPE(qs_environment_type), INTENT(IN), POINTER :: qs_env
1244
1245 CHARACTER(LEN=*), PARAMETER :: routinen = 'tddfpt_print_exciton_descriptors'
1246
1247 CHARACTER(LEN=4) :: prefix_output
1248 INTEGER :: handle, ispin, istate, n_moments_quad, &
1249 nactive, nao, nspins, nstates
1250 INTEGER, DIMENSION(maxspins) :: nmo_occ, nmo_virt
1251 LOGICAL :: print_checkvalue
1252 REAL(kind=dp), ALLOCATABLE, DIMENSION(:) :: ref_point_multipole
1253 TYPE(cp_blacs_env_type), POINTER :: blacs_env
1254 TYPE(cp_fm_struct_type), POINTER :: fm_struct_mo_coeff, &
1255 fm_struct_s_mos_virt, fm_struct_x_ia_n
1256 TYPE(cp_fm_type), ALLOCATABLE, DIMENSION(:) :: eigvec_x_ia_n, fm_multipole_ab, &
1257 fm_multipole_ai, fm_multipole_ij, &
1258 s_mos_virt
1259 TYPE(cp_fm_type), DIMENSION(:), POINTER :: mo_coeff
1260 TYPE(exciton_descr_type), ALLOCATABLE, &
1261 DIMENSION(:) :: exc_descr
1262
1263 CALL timeset(routinen, handle)
1264
1265 nspins = SIZE(evects, 1)
1266 nstates = SIZE(evects, 2)
1267
1268 cpassert(nspins == 1) ! Other spins are not yet implemented for exciton descriptors
1269
1270 CALL cp_fm_get_info(gs_mos(1)%mos_occ, context=blacs_env)
1271 CALL dbcsr_get_info(matrix_s, nfullrows_total=nao)
1272
1273 DO ispin = 1, nspins
1274 nmo_occ(ispin) = SIZE(gs_mos(ispin)%evals_occ)
1275 nmo_virt(ispin) = SIZE(gs_mos(ispin)%evals_virt)
1276 END DO
1277
1278 ! Prepare fm with all MO coefficents, i.e. nao x nao
1279 ALLOCATE (mo_coeff(nspins))
1280 CALL cp_fm_struct_create(fm_struct_mo_coeff, nrow_global=nao, ncol_global=nao, &
1281 context=blacs_env)
1282 DO ispin = 1, nspins
1283 CALL cp_fm_create(mo_coeff(ispin), fm_struct_mo_coeff)
1284 CALL cp_fm_to_fm_submat_general(gs_mos(ispin)%mos_occ, &
1285 mo_coeff(ispin), &
1286 nao, &
1287 nmo_occ(ispin), &
1288 1, &
1289 1, &
1290 1, &
1291 1, &
1292 blacs_env)
1293 CALL cp_fm_to_fm_submat_general(gs_mos(ispin)%mos_virt, &
1294 mo_coeff(ispin), &
1295 nao, &
1296 nmo_virt(ispin), &
1297 1, &
1298 1, &
1299 1, &
1300 nmo_occ(ispin) + 1, &
1301 blacs_env)
1302 END DO
1303 CALL cp_fm_struct_release(fm_struct_mo_coeff)
1304
1305 ! Compute multipole moments
1306 ! fm_multipole_XY have structure inherited by libint, i.e. x, y, z, xx, xy, xz, yy, yz, zz
1307 n_moments_quad = 9
1308 ALLOCATE (ref_point_multipole(3))
1309 ALLOCATE (fm_multipole_ij(n_moments_quad))
1310 ALLOCATE (fm_multipole_ab(n_moments_quad))
1311 ALLOCATE (fm_multipole_ai(n_moments_quad))
1312
1313 CALL get_multipoles_mo(fm_multipole_ai, fm_multipole_ij, fm_multipole_ab, &
1314 qs_env, mo_coeff, ref_point_multipole, 2, &
1315 nmo_occ(1), nmo_virt(1), blacs_env)
1316
1317 CALL cp_fm_release(mo_coeff)
1318
1319 ! Compute eigenvector X of the Casida equation from trial vectors
1320 ALLOCATE (s_mos_virt(nspins), eigvec_x_ia_n(nspins))
1321 DO ispin = 1, nspins
1322 CALL cp_fm_get_info(gs_mos(ispin)%mos_virt, matrix_struct=fm_struct_s_mos_virt)
1323 CALL cp_fm_create(s_mos_virt(ispin), fm_struct_s_mos_virt)
1324 NULLIFY (fm_struct_s_mos_virt)
1325 CALL cp_dbcsr_sm_fm_multiply(matrix_s, &
1326 gs_mos(ispin)%mos_virt, &
1327 s_mos_virt(ispin), &
1328 ncol=nmo_virt(ispin), alpha=1.0_dp, beta=0.0_dp)
1329
1330 CALL cp_fm_struct_create(fm_struct_x_ia_n, nrow_global=nmo_occ(ispin), ncol_global=nmo_virt(ispin), &
1331 context=blacs_env)
1332 CALL cp_fm_create(eigvec_x_ia_n(ispin), fm_struct_x_ia_n)
1333 CALL cp_fm_struct_release(fm_struct_x_ia_n)
1334 END DO
1335 ALLOCATE (exc_descr(nstates))
1336 DO istate = 1, nstates
1337 DO ispin = 1, nspins
1338 CALL cp_fm_set_all(eigvec_x_ia_n(ispin), 0.0_dp)
1339 ! compute eigenvectors X of the TDA equation
1340 ! Reshuffle multiplication from
1341 ! X_ai = S_ma ^T * C_mi
1342 ! to
1343 ! X_ia = C_mi ^T * S_ma
1344 ! for compatibility with the structure needed for get_exciton_descriptors of bse_properties.F
1345 CALL cp_fm_get_info(evects(ispin, istate), ncol_global=nactive)
1346 IF (nactive /= nmo_occ(ispin)) THEN
1347 CALL cp_abort(__location__, &
1348 "Reduced active space excitations not implemented")
1349 END IF
1350 CALL parallel_gemm('T', 'N', nmo_occ(ispin), nmo_virt(ispin), nao, 1.0_dp, &
1351 evects(ispin, istate), s_mos_virt(ispin), 0.0_dp, eigvec_x_ia_n(ispin))
1352
1353 CALL get_exciton_descriptors(exc_descr, eigvec_x_ia_n(ispin), &
1354 fm_multipole_ij, fm_multipole_ab, &
1355 fm_multipole_ai, &
1356 istate, nmo_occ(ispin), nmo_virt(ispin))
1357 END DO
1358 END DO
1359 CALL cp_fm_release(eigvec_x_ia_n)
1360 CALL cp_fm_release(s_mos_virt)
1361 CALL cp_fm_release(fm_multipole_ai)
1362 CALL cp_fm_release(fm_multipole_ij)
1363 CALL cp_fm_release(fm_multipole_ab)
1364
1365 ! Actual printing
1366 print_checkvalue = .true.
1367 prefix_output = ' '
1368 CALL print_exciton_descriptors(exc_descr, ref_point_multipole, log_unit, &
1369 nstates, print_checkvalue, do_directional_exciton_descriptors, &
1370 prefix_output, qs_env)
1371
1372 DEALLOCATE (ref_point_multipole)
1373 DEALLOCATE (exc_descr)
1374
1375 CALL timestop(handle)
1376
1377 END SUBROUTINE tddfpt_print_exciton_descriptors
1378
1379! **************************************************************************************************
1380!> \brief ...
1381!> \param vin ...
1382!> \param vout ...
1383!> \param mos_occ ...
1384!> \param matrix_s ...
1385! **************************************************************************************************
1386 SUBROUTINE project_vector(vin, vout, mos_occ, matrix_s)
1387 TYPE(dbcsr_type) :: vin, vout
1388 TYPE(cp_fm_type), INTENT(IN) :: mos_occ
1389 TYPE(dbcsr_type), POINTER :: matrix_s
1390
1391 CHARACTER(LEN=*), PARAMETER :: routinen = 'project_vector'
1392
1393 INTEGER :: handle, nao, nmo
1394 REAL(kind=dp) :: norm(1)
1395 TYPE(cp_fm_struct_type), POINTER :: fm_struct, fm_vec_struct
1396 TYPE(cp_fm_type) :: csvec, svec, vec
1397
1398 CALL timeset(routinen, handle)
1399
1400 CALL cp_fm_get_info(mos_occ, matrix_struct=fm_struct, nrow_global=nao, ncol_global=nmo)
1401 CALL cp_fm_struct_create(fmstruct=fm_vec_struct, template_fmstruct=fm_struct, &
1402 nrow_global=nao, ncol_global=1)
1403 CALL cp_fm_create(vec, fm_vec_struct)
1404 CALL cp_fm_create(svec, fm_vec_struct)
1405 CALL cp_fm_struct_release(fm_vec_struct)
1406 CALL cp_fm_struct_create(fmstruct=fm_vec_struct, template_fmstruct=fm_struct, &
1407 nrow_global=nmo, ncol_global=1)
1408 CALL cp_fm_create(csvec, fm_vec_struct)
1409 CALL cp_fm_struct_release(fm_vec_struct)
1410
1411 CALL copy_dbcsr_to_fm(vin, vec)
1412 CALL cp_dbcsr_sm_fm_multiply(matrix_s, vec, svec, ncol=1, alpha=1.0_dp, beta=0.0_dp)
1413 CALL parallel_gemm('T', 'N', nmo, 1, nao, 1.0_dp, mos_occ, svec, 0.0_dp, csvec)
1414 CALL parallel_gemm('N', 'N', nao, 1, nmo, -1.0_dp, mos_occ, csvec, 1.0_dp, vec)
1415 CALL cp_fm_vectorsnorm(vec, norm)
1416 cpassert(norm(1) > 1.e-14_dp)
1417 norm(1) = sqrt(1._dp/norm(1))
1418 CALL cp_fm_scale(norm(1), vec)
1419 CALL copy_fm_to_dbcsr(vec, vout, keep_sparsity=.false.)
1420
1421 CALL cp_fm_release(csvec)
1422 CALL cp_fm_release(svec)
1423 CALL cp_fm_release(vec)
1424
1425 CALL timestop(handle)
1426
1427 END SUBROUTINE project_vector
1428
1429! **************************************************************************************************
1430!> \brief ...
1431!> \param va ...
1432!> \param vb ...
1433!> \param res ...
1434! **************************************************************************************************
1435 SUBROUTINE vec_product(va, vb, res)
1436 TYPE(dbcsr_type) :: va, vb
1437 REAL(kind=dp), INTENT(OUT) :: res
1438
1439 CHARACTER(LEN=*), PARAMETER :: routinen = 'vec_product'
1440
1441 INTEGER :: handle, icol, irow
1442 LOGICAL :: found
1443 REAL(kind=dp), DIMENSION(:, :), POINTER :: vba, vbb
1444 TYPE(dbcsr_iterator_type) :: iter
1445 TYPE(mp_comm_type) :: group
1446
1447 CALL timeset(routinen, handle)
1448
1449 res = 0.0_dp
1450
1451 CALL dbcsr_get_info(va, group=group)
1452 CALL dbcsr_iterator_start(iter, va)
1453 DO WHILE (dbcsr_iterator_blocks_left(iter))
1454 CALL dbcsr_iterator_next_block(iter, irow, icol, vba)
1455 CALL dbcsr_get_block_p(vb, row=irow, col=icol, block=vbb, found=found)
1456 res = res + sum(vba*vbb)
1457 cpassert(found)
1458 END DO
1459 CALL dbcsr_iterator_stop(iter)
1460 CALL group%sum(res)
1461
1462 CALL timestop(handle)
1463
1464 END SUBROUTINE vec_product
1465
1466! **************************************************************************************************
1467!> \brief ...
1468!> \param qs_env ...
1469!> \param mos ...
1470!> \param istate ...
1471!> \param stride ...
1472!> \param append_cube ...
1473!> \param print_section ...
1474! **************************************************************************************************
1475 SUBROUTINE print_nto_cubes(qs_env, mos, istate, stride, append_cube, print_section)
1476
1477 TYPE(qs_environment_type), POINTER :: qs_env
1478 TYPE(mo_set_type), DIMENSION(:), INTENT(IN) :: mos
1479 INTEGER, INTENT(IN) :: istate
1480 INTEGER, DIMENSION(:), POINTER :: stride
1481 LOGICAL, INTENT(IN) :: append_cube
1482 TYPE(section_vals_type), POINTER :: print_section
1483
1484 CHARACTER(LEN=default_path_length) :: filename, my_pos_cube, title
1485 INTEGER :: i, iset, nmo, unit_nr
1486 LOGICAL :: mpi_io
1487 TYPE(atomic_kind_type), DIMENSION(:), POINTER :: atomic_kind_set
1488 TYPE(cell_type), POINTER :: cell
1489 TYPE(cp_fm_type), POINTER :: mo_coeff
1490 TYPE(cp_logger_type), POINTER :: logger
1491 TYPE(dft_control_type), POINTER :: dft_control
1492 TYPE(particle_list_type), POINTER :: particles
1493 TYPE(particle_type), DIMENSION(:), POINTER :: particle_set
1494 TYPE(pw_c1d_gs_type) :: wf_g
1495 TYPE(pw_env_type), POINTER :: pw_env
1496 TYPE(pw_pool_p_type), DIMENSION(:), POINTER :: pw_pools
1497 TYPE(pw_pool_type), POINTER :: auxbas_pw_pool
1498 TYPE(pw_r3d_rs_type) :: wf_r
1499 TYPE(qs_kind_type), DIMENSION(:), POINTER :: qs_kind_set
1500 TYPE(qs_subsys_type), POINTER :: subsys
1501
1502 logger => cp_get_default_logger()
1503
1504 CALL get_qs_env(qs_env=qs_env, dft_control=dft_control, pw_env=pw_env)
1505 CALL pw_env_get(pw_env, auxbas_pw_pool=auxbas_pw_pool, pw_pools=pw_pools)
1506 CALL auxbas_pw_pool%create_pw(wf_r)
1507 CALL auxbas_pw_pool%create_pw(wf_g)
1508
1509 CALL get_qs_env(qs_env, subsys=subsys)
1510 CALL qs_subsys_get(subsys, particles=particles)
1511
1512 my_pos_cube = "REWIND"
1513 IF (append_cube) THEN
1514 my_pos_cube = "APPEND"
1515 END IF
1516
1517 CALL get_qs_env(qs_env=qs_env, &
1518 atomic_kind_set=atomic_kind_set, &
1519 qs_kind_set=qs_kind_set, &
1520 cell=cell, &
1521 particle_set=particle_set)
1522
1523 DO iset = 1, 2
1524 CALL get_mo_set(mo_set=mos(iset), mo_coeff=mo_coeff, nmo=nmo)
1525 DO i = 1, nmo
1526 CALL calculate_wavefunction(mo_coeff, i, wf_r, wf_g, atomic_kind_set, qs_kind_set, &
1527 cell, dft_control, particle_set, pw_env)
1528 IF (iset == 1) THEN
1529 WRITE (filename, '(a4,I3.3,I2.2,a11)') "NTO_STATE", istate, i, "_Hole_State"
1530 ELSE IF (iset == 2) THEN
1531 WRITE (filename, '(a4,I3.3,I2.2,a15)') "NTO_STATE", istate, i, "_Particle_State"
1532 END IF
1533 mpi_io = .true.
1534 unit_nr = cp_print_key_unit_nr(logger, print_section, '', extension=".cube", &
1535 middle_name=trim(filename), file_position=my_pos_cube, &
1536 log_filename=.false., ignore_should_output=.true., mpi_io=mpi_io)
1537 IF (iset == 1) THEN
1538 WRITE (title, *) "Natural Transition Orbital Hole State", i
1539 ELSE IF (iset == 2) THEN
1540 WRITE (title, *) "Natural Transition Orbital Particle State", i
1541 END IF
1542 CALL cp_pw_to_cube(wf_r, unit_nr, title, particles=particles, stride=stride, mpi_io=mpi_io)
1543 CALL cp_print_key_finished_output(unit_nr, logger, print_section, '', &
1544 ignore_should_output=.true., mpi_io=mpi_io)
1545 END DO
1546 END DO
1547
1548 CALL auxbas_pw_pool%give_back_pw(wf_g)
1549 CALL auxbas_pw_pool%give_back_pw(wf_r)
1550
1551 END SUBROUTINE print_nto_cubes
1552
1553END MODULE qs_tddfpt2_properties
cp_dbcsr_operations::dbcsr_allocate_matrix_set
Definition cp_dbcsr_operations.F:77
cp_dbcsr_operations::dbcsr_deallocate_matrix_set
Definition cp_dbcsr_operations.F:85
cp_fm_basic_linalg::cp_fm_trace
Definition cp_fm_basic_linalg.F:78
cp_fm_types::cp_fm_release
Definition cp_fm_types.F:88
cp_fm_types::cp_fm_to_fm
Definition cp_fm_types.F:83
parallel_gemm_api::parallel_gemm
Definition parallel_gemm_api.F:39
atomic_kind_types
Define the atomic kind types and their sub types.
Definition atomic_kind_types.F:23
bibliography
collects all references to literature in CP2K as new algorithms / method are included from literature...
Definition bibliography.F:21
bibliography::martin2003
integer, save, public martin2003
Definition bibliography.F:36
bse_print
Routines for printing information in context of the BSE calculation.
Definition bse_print.F:13
bse_print::print_exciton_descriptors
subroutine, public print_exciton_descriptors(exc_descr, ref_point_multipole, unit_nr, num_print_exc_descr, print_checkvalue, print_directional_exc_descr, prefix_output, qs_env)
Prints exciton descriptors, cf. Mewes et al., JCTC 14, 710-725 (2018)
Definition bse_print.F:573
bse_properties
Routines for computing excitonic properties, e.g. exciton diameter, from the BSE.
Definition bse_properties.F:13
bse_properties::get_exciton_descriptors
subroutine, public get_exciton_descriptors(exc_descr, fm_x_ia, fm_multipole_ij_trunc, fm_multipole_ab_trunc, fm_multipole_ai_trunc, i_exc, homo, virtual, fm_y_ia)
...
Definition bse_properties.F:765
bse_util
Auxiliary routines for GW + Bethe-Salpeter for computing electronic excitations.
Definition bse_util.F:13
bse_util::get_multipoles_mo
subroutine, public get_multipoles_mo(fm_multipole_ai_trunc, fm_multipole_ij_trunc, fm_multipole_ab_trunc, qs_env, mo_coeff, rpoint, n_moments, homo_red, virtual_red, context_bse, ispin)
...
Definition bse_util.F:1886
cell_types
Handles all functions related to the CELL.
Definition cell_types.F:15
cp_blacs_env
methods related to the blacs parallel environment
Definition cp_blacs_env.F:15
cp_cfm_basic_linalg
Basic linear algebra operations for complex full matrices.
Definition cp_cfm_basic_linalg.F:16
cp_cfm_basic_linalg::cp_cfm_solve
subroutine, public cp_cfm_solve(matrix_a, general_a, determinant)
Solve the system of linear equations A*b=A_general using LU decomposition. Pay attention that both ma...
Definition cp_cfm_basic_linalg.F:729
cp_cfm_types
Represents a complex full matrix distributed on many processors.
Definition cp_cfm_types.F:12
cp_cfm_types::cp_cfm_release
subroutine, public cp_cfm_release(matrix)
Releases a full matrix.
Definition cp_cfm_types.F:182
cp_cfm_types::cp_fm_to_cfm
subroutine, public cp_fm_to_cfm(msourcer, msourcei, mtarget)
Construct a complex full matrix by taking its real and imaginary parts from two separate real-value f...
Definition cp_cfm_types.F:844
cp_cfm_types::cp_cfm_create
subroutine, public cp_cfm_create(matrix, matrix_struct, name, nrow, ncol, set_zero)
Creates a new full matrix with the given structure.
Definition cp_cfm_types.F:125
cp_cfm_types::cp_cfm_set_all
subroutine, public cp_cfm_set_all(matrix, alpha, beta)
Set all elements of the full matrix to alpha. Besides, set all diagonal matrix elements to beta (if g...
Definition cp_cfm_types.F:202
cp_cfm_types::cp_cfm_to_fm
subroutine, public cp_cfm_to_fm(msource, mtargetr, mtargeti)
Copy real and imaginary parts of a complex full matrix into separate real-value full matrices.
Definition cp_cfm_types.F:792
cp_control_types
Defines control structures, which contain the parameters and the settings for the DFT-based calculati...
Definition cp_control_types.F:12
cp_dbcsr_api
Definition cp_dbcsr_api.F:8
cp_dbcsr_api::dbcsr_iterator_blocks_left
logical function, public dbcsr_iterator_blocks_left(iterator)
...
Definition cp_dbcsr_api.F:944
cp_dbcsr_api::dbcsr_iterator_stop
subroutine, public dbcsr_iterator_stop(iterator)
...
Definition cp_dbcsr_api.F:1050
cp_dbcsr_api::dbcsr_copy
subroutine, public dbcsr_copy(matrix_b, matrix_a, name, keep_sparsity, keep_imaginary)
...
Definition cp_dbcsr_api.F:371
cp_dbcsr_api::dbcsr_get_block_p
subroutine, public dbcsr_get_block_p(matrix, row, col, block, found, row_size, col_size)
...
Definition cp_dbcsr_api.F:693
cp_dbcsr_api::dbcsr_get_info
subroutine, public dbcsr_get_info(matrix, nblkrows_total, nblkcols_total, nfullrows_total, nfullcols_total, nblkrows_local, nblkcols_local, nfullrows_local, nfullcols_local, my_prow, my_pcol, local_rows, local_cols, proc_row_dist, proc_col_dist, row_blk_size, col_blk_size, row_blk_offset, col_blk_offset, distribution, name, matrix_type, group)
...
Definition cp_dbcsr_api.F:808
cp_dbcsr_api::dbcsr_init_p
subroutine, public dbcsr_init_p(matrix)
...
Definition cp_dbcsr_api.F:207
cp_dbcsr_api::dbcsr_iterator_next_block
subroutine, public dbcsr_iterator_next_block(iterator, row, column, block, block_number_argument_has_been_removed, row_size, col_size, row_offset, col_offset, transposed)
...
Definition cp_dbcsr_api.F:971
cp_dbcsr_api::dbcsr_iterator_start
subroutine, public dbcsr_iterator_start(iterator, matrix, shared, dynamic, dynamic_byrows)
...
Definition cp_dbcsr_api.F:1012
cp_dbcsr_api::dbcsr_set
subroutine, public dbcsr_set(matrix, alpha)
...
Definition cp_dbcsr_api.F:1204
cp_dbcsr_operations
DBCSR operations in CP2K.
Definition cp_dbcsr_operations.F:18
cp_dbcsr_operations::cp_dbcsr_sm_fm_multiply
subroutine, public cp_dbcsr_sm_fm_multiply(matrix, fm_in, fm_out, ncol, alpha, beta)
multiply a dbcsr with a fm matrix
Definition cp_dbcsr_operations.F:548
cp_dbcsr_operations::copy_dbcsr_to_fm
subroutine, public copy_dbcsr_to_fm(matrix, fm)
Copy a DBCSR matrix to a BLACS matrix.
Definition cp_dbcsr_operations.F:212
cp_dbcsr_operations::copy_fm_to_dbcsr
subroutine, public copy_fm_to_dbcsr(fm, matrix, keep_sparsity)
Copy a BLACS matrix to a dbcsr matrix.
Definition cp_dbcsr_operations.F:111
cp_fm_basic_linalg
Basic linear algebra operations for full matrices.
Definition cp_fm_basic_linalg.F:14
cp_fm_basic_linalg::cp_fm_scale_and_add
subroutine, public cp_fm_scale_and_add(alpha, matrix_a, beta, matrix_b)
calc A <- alpha*A + beta*B optimized for alpha == 1.0 (just add beta*B) and beta == 0....
Definition cp_fm_basic_linalg.F:170
cp_fm_basic_linalg::cp_fm_scale
subroutine, public cp_fm_scale(alpha, matrix_a)
scales a matrix matrix_a = alpha * matrix_b
Definition cp_fm_basic_linalg.F:1502
cp_fm_diag
used for collecting some of the diagonalization schemes available for cp_fm_type. cp_fm_power also mo...
Definition cp_fm_diag.F:17
cp_fm_diag::cp_fm_geeig
subroutine, public cp_fm_geeig(amatrix, bmatrix, eigenvectors, eigenvalues, work)
General Eigenvalue Problem AX = BXE. Use cuSOLVERMp directly when requested and large enough; otherwi...
Definition cp_fm_diag.F:1486
cp_fm_diag::choose_eigv_solver
subroutine, public choose_eigv_solver(matrix, eigenvectors, eigenvalues, info)
Choose the Eigensolver depending on which library is available ELPA seems to be unstable for small sy...
Definition cp_fm_diag.F:245
cp_fm_struct
represent the structure of a full matrix
Definition cp_fm_struct.F:14
cp_fm_struct::cp_fm_struct_create
subroutine, public cp_fm_struct_create(fmstruct, para_env, context, nrow_global, ncol_global, nrow_block, ncol_block, descriptor, first_p_pos, local_leading_dimension, template_fmstruct, square_blocks, force_block)
allocates and initializes a full matrix structure
Definition cp_fm_struct.F:132
cp_fm_struct::cp_fm_struct_release
subroutine, public cp_fm_struct_release(fmstruct)
releases a full matrix structure
Definition cp_fm_struct.F:355
cp_fm_types
represent a full matrix distributed on many processors
Definition cp_fm_types.F:15
cp_fm_types::cp_fm_get_info
subroutine, public cp_fm_get_info(matrix, name, nrow_global, ncol_global, nrow_block, ncol_block, nrow_local, ncol_local, row_indices, col_indices, local_data, context, nrow_locals, ncol_locals, matrix_struct, para_env)
returns all kind of information about the full matrix
Definition cp_fm_types.F:1038
cp_fm_types::cp_fm_vectorsnorm
subroutine, public cp_fm_vectorsnorm(matrix, norm_array)
find the inorm of each column norm_{j}= sqrt( \sum_{i} A_{ij}*A_{ij} )
Definition cp_fm_types.F:1213
cp_fm_types::cp_fm_to_fm_submat_general
subroutine, public cp_fm_to_fm_submat_general(source, destination, nrows, ncols, s_firstrow, s_firstcol, d_firstrow, d_firstcol, global_context)
General copy of a submatrix of fm matrix to a submatrix of another fm matrix. The two matrices can ha...
Definition cp_fm_types.F:1986
cp_fm_types::cp_fm_set_all
subroutine, public cp_fm_set_all(matrix, alpha, beta)
set all elements of a matrix to the same value, and optionally the diagonal to a different one
Definition cp_fm_types.F:534
cp_fm_types::cp_fm_create
subroutine, public cp_fm_create(matrix, matrix_struct, name, nrow, ncol, set_zero)
creates a new full matrix with the given structure
Definition cp_fm_types.F:165
cp_log_handling
various routines to log and control the output. The idea is that decisions about where to log should ...
Definition cp_log_handling.F:41
cp_log_handling::cp_logger_get_default_io_unit
integer function, public cp_logger_get_default_io_unit(logger)
returns the unit nr for the ionode (-1 on all other processors) skips as well checks if the procs cal...
Definition cp_log_handling.F:523
cp_log_handling::cp_get_default_logger
type(cp_logger_type) function, pointer, public cp_get_default_logger()
returns the default logger
Definition cp_log_handling.F:234
cp_output_handling
routines to handle the output, The idea is to remove the decision of wheter to output and what to out...
Definition cp_output_handling.F:25
cp_output_handling::cp_print_key_unit_nr
integer function, public cp_print_key_unit_nr(logger, basis_section, print_key_path, extension, middle_name, local, log_filename, ignore_should_output, file_form, file_position, file_action, file_status, do_backup, on_file, is_new_file, mpi_io, fout)
...
Definition cp_output_handling.F:853
cp_output_handling::cp_print_key_finished_output
subroutine, public cp_print_key_finished_output(unit_nr, logger, basis_section, print_key_path, local, ignore_should_output, on_file, mpi_io)
should be called after you finish working with a unit obtained with cp_print_key_unit_nr,...
Definition cp_output_handling.F:1073
cp_output_handling::cp_p_file
integer, parameter, public cp_p_file
Definition cp_output_handling.F:103
cp_output_handling::cp_print_key_should_output
integer function, public cp_print_key_should_output(iteration_info, basis_section, print_key_path, used_print_key, first_time)
returns what should be done with the given property if btest(res,cp_p_store) then the property should...
Definition cp_output_handling.F:345
cp_realspace_grid_cube
A wrapper around pw_to_cube() which accepts particle_list_type.
Definition cp_realspace_grid_cube.F:12
cp_realspace_grid_cube::cp_pw_to_cube
subroutine, public cp_pw_to_cube(pw, unit_nr, title, particles, zeff, stride, max_file_size_mb, zero_tails, silent, mpi_io)
...
Definition cp_realspace_grid_cube.F:48
input_constants
collects all constants needed in input so that they can be used without circular dependencies
Definition input_constants.F:18
input_constants::tddfpt_dipole_berry
integer, parameter, public tddfpt_dipole_berry
Definition input_constants.F:726
input_constants::tddfpt_dipole_scf_moment
integer, parameter, public tddfpt_dipole_scf_moment
Definition input_constants.F:726
input_constants::tddfpt_dipole_velocity
integer, parameter, public tddfpt_dipole_velocity
Definition input_constants.F:726
input_constants::tddfpt_dipole_length
integer, parameter, public tddfpt_dipole_length
Definition input_constants.F:726
input_constants::tddfpt_dipole_velocity_old
integer, parameter, public tddfpt_dipole_velocity_old
Definition input_constants.F:726
input_constants::no_sf_tddfpt
integer, parameter, public no_sf_tddfpt
Definition input_constants.F:608
input_section_types
objects that represent the structure of input sections and the data contained in an input section
Definition input_section_types.F:15
input_section_types::section_vals_get_subs_vals
recursive type(section_vals_type) function, pointer, public section_vals_get_subs_vals(section_vals, subsection_name, i_rep_section, can_return_null)
returns the values of the requested subsection
Definition input_section_types.F:735
input_section_types::section_vals_val_get
subroutine, public section_vals_val_get(section_vals, keyword_name, i_rep_section, i_rep_val, n_rep_val, val, l_val, i_val, r_val, c_val, l_vals, i_vals, r_vals, c_vals, explicit)
returns the requested value
Definition input_section_types.F:1052
kinds
Defines the basic variable types.
Definition kinds.F:23
kinds::int_8
integer, parameter, public int_8
Definition kinds.F:54
kinds::dp
integer, parameter, public dp
Definition kinds.F:34
kinds::default_path_length
integer, parameter, public default_path_length
Definition kinds.F:58
mathconstants
Definition of mathematical constants and functions.
Definition mathconstants.F:16
mathconstants::z_one
complex(kind=dp), parameter, public z_one
Definition mathconstants.F:143
mathconstants::twopi
real(kind=dp), parameter, public twopi
Definition mathconstants.F:112
mathconstants::z_zero
complex(kind=dp), parameter, public z_zero
Definition mathconstants.F:143
message_passing
Interface to the message passing library MPI.
Definition message_passing.F:23
molden_utils
Functions handling the MOLDEN format. Split from mode_selective.
Definition molden_utils.F:12
molden_utils::write_mos_molden
subroutine, public write_mos_molden(mos, qs_kind_set, particle_set, print_section, cell, unoccupied_orbs, unoccupied_evals, qs_env, calc_energies)
Write out the MOs in molden format for visualisation.
Definition molden_utils.F:85
moments_utils
Calculates the moment integrals <a|r^m|b>
Definition moments_utils.F:15
moments_utils::get_reference_point
subroutine, public get_reference_point(rpoint, drpoint, qs_env, fist_env, reference, ref_point, ifirst, ilast)
...
Definition moments_utils.F:61
parallel_gemm_api
basic linear algebra operations for full matrixes
Definition parallel_gemm_api.F:14
particle_list_types
represent a simple array based list of the given type
Definition particle_list_types.F:15
particle_types
Define the data structure for the particle information.
Definition particle_types.F:19
physcon
Definition of physical constants:
Definition physcon.F:68
physcon::evolt
real(kind=dp), parameter, public evolt
Definition physcon.F:183
pw_env_types
container for various plainwaves related things
Definition pw_env_types.F:14
pw_env_types::pw_env_get
subroutine, public pw_env_get(pw_env, pw_pools, cube_info, gridlevel_info, auxbas_pw_pool, auxbas_grid, auxbas_rs_desc, auxbas_rs_grid, rs_descs, rs_grids, xc_pw_pool, vdw_pw_pool, poisson_env, interp_section)
returns the various attributes of the pw env
Definition pw_env_types.F:113
pw_poisson_types
functions related to the poisson solver on regular grids
Definition pw_poisson_types.F:22
pw_pool_types
Manages a pool of grids (to be used for example as tmp objects), but can also be used to instantiate ...
Definition pw_pool_types.F:24
pw_types
Definition pw_types.F:24
qs_collocate_density
Calculate the plane wave density by collocating the primitive Gaussian functions (pgf).
Definition qs_collocate_density.F:38
qs_collocate_density::calculate_wavefunction
subroutine, public calculate_wavefunction(mo_vectors, ivector, rho, rho_gspace, atomic_kind_set, qs_kind_set, cell, dft_control, particle_set, pw_env, basis_type)
maps a given wavefunction on the grid
Definition qs_collocate_density.F:2869
qs_environment_types
Definition qs_environment_types.F:14
qs_environment_types::get_qs_env
subroutine, public get_qs_env(qs_env, atomic_kind_set, qs_kind_set, cell, super_cell, cell_ref, use_ref_cell, kpoints, dft_control, mos, sab_orb, sab_all, qmmm, qmmm_periodic, mimic, sac_ae, sac_ppl, sac_lri, sap_ppnl, sab_vdw, sab_scp, sap_oce, sab_lrc, sab_se, sab_xtbe, sab_tbe, sab_core, sab_xb, sab_xtb_pp, sab_xtb_nonbond, sab_almo, sab_kp, sab_kp_nosym, sab_cneo, particle_set, energy, force, matrix_h, matrix_h_im, matrix_ks, matrix_ks_im, matrix_vxc, run_rtp, rtp, matrix_h_kp, matrix_h_im_kp, matrix_ks_kp, matrix_ks_im_kp, matrix_vxc_kp, kinetic_kp, matrix_s_kp, matrix_w_kp, matrix_s_ri_aux_kp, matrix_s, matrix_s_ri_aux, matrix_w, matrix_p_mp2, matrix_p_mp2_admm, matrix_vhxc, rho, rho_xc, pw_env, ewald_env, ewald_pw, active_space, mpools, input, para_env, blacs_env, scf_control, rel_control, kinetic, qs_charges, vppl, xcint_weights, rho_core, rho_nlcc, rho_nlcc_g, ks_env, ks_qmmm_env, wf_history, scf_env, local_particles, local_molecules, distribution_2d, dbcsr_dist, molecule_kind_set, molecule_set, subsys, cp_subsys, oce, local_rho_set, rho_atom_set, task_list, task_list_soft, rho0_atom_set, rho0_mpole, rhoz_set, rhoz_cneo_set, ecoul_1c, rho0_s_rs, rho0_s_gs, rhoz_cneo_s_rs, rhoz_cneo_s_gs, do_kpoints, has_unit_metric, requires_mo_derivs, mo_derivs, mo_loc_history, nkind, natom, nelectron_total, nelectron_spin, efield, neighbor_list_id, linres_control, xas_env, virial, cp_ddapc_env, cp_ddapc_ewald, outer_scf_history, outer_scf_ihistory, x_data, et_coupling, dftb_potential, results, se_taper, se_store_int_env, se_nddo_mpole, se_nonbond_env, admm_env, lri_env, lri_density, exstate_env, ec_env, harris_env, dispersion_env, gcp_env, vee, rho_external, external_vxc, mask, mp2_env, bs_env, kg_env, wanniercentres, atprop, ls_scf_env, do_transport, transport_env, v_hartree_rspace, s_mstruct_changed, rho_changed, potential_changed, forces_up_to_date, mscfg_env, almo_scf_env, gradient_history, variable_history, embed_pot, spin_embed_pot, polar_env, mos_last_converged, eeq, rhs, do_rixs, tb_tblite)
Get the QUICKSTEP environment.
Definition qs_environment_types.F:534
qs_kind_types
Define the quickstep kind type and their sub types.
Definition qs_kind_types.F:23
qs_ks_types
Definition qs_ks_types.F:15
qs_mo_types
Definition and initialisation of the mo data type.
Definition qs_mo_types.F:22
qs_mo_types::set_mo_set
subroutine, public set_mo_set(mo_set, maxocc, homo, lfomo, nao, nelectron, n_el_f, nmo, eigenvalues, occupation_numbers, uniform_occupation, kts, mu, flexible_electron_count)
Set the components of a MO set data structure.
Definition qs_mo_types.F:456
qs_mo_types::init_mo_set
subroutine, public init_mo_set(mo_set, fm_pool, fm_ref, fm_struct, name, counter)
initializes an allocated mo_set. eigenvalues, mo_coeff, occupation_numbers are valid only after this ...
Definition qs_mo_types.F:247
qs_mo_types::allocate_mo_set
subroutine, public allocate_mo_set(mo_set, nao, nmo, nelectron, n_el_f, maxocc, flexible_electron_count)
Allocates a mo set and partially initializes it (nao,nmo,nelectron, and flexible_electron_count are v...
Definition qs_mo_types.F:207
qs_mo_types::deallocate_mo_set
subroutine, public deallocate_mo_set(mo_set)
Deallocate a wavefunction data structure.
Definition qs_mo_types.F:356
qs_mo_types::get_mo_set
subroutine, public get_mo_set(mo_set, maxocc, homo, lfomo, nao, nelectron, n_el_f, nmo, eigenvalues, occupation_numbers, mo_coeff, mo_coeff_b, uniform_occupation, kts, mu, flexible_electron_count)
Get the components of a MO set data structure.
Definition qs_mo_types.F:401
qs_moments
Calculates the moment integrals <a|r^m|b> and <a|r x d/dr|b>
Definition qs_moments.F:14
qs_moments::build_berry_moment_matrix
subroutine, public build_berry_moment_matrix(qs_env, cosmat, sinmat, kvec, sab_orb_external, basis_type)
...
Definition qs_moments.F:1360
qs_neighbor_list_types
Define the neighbor list data types and the corresponding functionality.
Definition qs_neighbor_list_types.F:17
qs_operators_ao
Definition qs_operators_ao.F:13
qs_operators_ao::rrc_xyz_ao
subroutine, public rrc_xyz_ao(op, qs_env, rc, order, minimum_image, soft)
Calculation of the components of the dipole operator in the length form by taking the relative positi...
Definition qs_operators_ao.F:689
qs_overlap
Calculation of overlap matrix, its derivatives and forces.
Definition qs_overlap.F:19
qs_overlap::build_overlap_matrix
subroutine, public build_overlap_matrix(ks_env, matrix_s, matrixkp_s, matrix_name, nderivative, basis_type_a, basis_type_b, sab_nl, calculate_forces, matrix_p, matrixkp_p, ext_kpoints)
Calculation of the overlap matrix over Cartesian Gaussian functions.
Definition qs_overlap.F:121
qs_subsys_types
types that represent a quickstep subsys
Definition qs_subsys_types.F:12
qs_subsys_types::qs_subsys_get
subroutine, public qs_subsys_get(subsys, atomic_kinds, atomic_kind_set, particles, particle_set, local_particles, molecules, molecule_set, molecule_kinds, molecule_kind_set, local_molecules, para_env, colvar_p, shell_particles, core_particles, gci, multipoles, natom, nparticle, ncore, nshell, nkind, atprop, virial, results, cell, cell_ref, use_ref_cell, energy, force, qs_kind_set, cp_subsys, nelectron_total, nelectron_spin)
...
Definition qs_subsys_types.F:137
qs_tddfpt2_properties
Definition qs_tddfpt2_properties.F:8
qs_tddfpt2_properties::tddfpt_dipole_operator
subroutine, public tddfpt_dipole_operator(dipole_op_mos_occ, tddfpt_control, gs_mos, qs_env)
Compute the action of the dipole operator on the ground state wave function.
Definition qs_tddfpt2_properties.F:154
qs_tddfpt2_properties::tddfpt_print_nto_analysis
subroutine, public tddfpt_print_nto_analysis(qs_env, evects, evals, ostrength, gs_mos, matrix_s, print_section)
Print natural transition orbital analysis.
Definition qs_tddfpt2_properties.F:973
qs_tddfpt2_properties::tddfpt_print_excitation_analysis
subroutine, public tddfpt_print_excitation_analysis(log_unit, evects, evals, gs_mos, matrix_s, spinflip, min_amplitude)
Print excitation analysis.
Definition qs_tddfpt2_properties.F:675
qs_tddfpt2_properties::tddfpt_print_exciton_descriptors
subroutine, public tddfpt_print_exciton_descriptors(log_unit, evects, gs_mos, matrix_s, do_directional_exciton_descriptors, qs_env)
Print exciton descriptors, cf. Mewes et al., JCTC 14, 710-725 (2018)
Definition qs_tddfpt2_properties.F:1237
qs_tddfpt2_properties::tddfpt_print_summary
subroutine, public tddfpt_print_summary(log_unit, evects, evals, gs_mos, ostrength, mult, dipole_op_mos_occ, dipole_form)
Print final TDDFPT excitation energies and oscillator strengths.
Definition qs_tddfpt2_properties.F:531
qs_tddfpt2_types
Definition qs_tddfpt2_types.F:8
string_utilities
Utilities for string manipulations.
Definition string_utilities.F:16
string_utilities::integer_to_string
subroutine, public integer_to_string(inumber, string)
Converts an integer number to a string. The WRITE statement will return an error message,...
Definition string_utilities.F:3239
util
All kind of helpful little routines.
Definition util.F:14
atomic_kind_types::atomic_kind_type
Provides all information about an atomic kind.
Definition atomic_kind_types.F:45
bse_properties::exciton_descr_type
Definition bse_properties.F:67
cell_types::cell_type
Type defining parameters related to the simulation cell.
Definition cell_types.F:60
cp_blacs_env::cp_blacs_env_type
represent a blacs multidimensional parallel environment (for the mpi corrispective see cp_paratypes/m...
Definition cp_blacs_env.F:53
cp_cfm_types::cp_cfm_type
Represent a complex full matrix.
Definition cp_cfm_types.F:69
cp_control_types::dft_control_type
Definition cp_control_types.F:757
cp_control_types::tddfpt2_control_type
Definition cp_control_types.F:634
cp_dbcsr_api::dbcsr_iterator_type
Definition cp_dbcsr_api.F:188
cp_dbcsr_api::dbcsr_p_type
Definition cp_dbcsr_api.F:172
cp_dbcsr_api::dbcsr_type
Definition cp_dbcsr_api.F:176
cp_fm_struct::cp_fm_struct_type
keeps the information about the structure of a full matrix
Definition cp_fm_struct.F:82
cp_fm_types::cp_fm_type
represent a full matrix
Definition cp_fm_types.F:114
cp_log_handling::cp_logger_type
type of a logger, at the moment it contains just a print level starting at which level it should be l...
Definition cp_log_handling.F:140
input_section_types::section_vals_type
stores the values of a section
Definition input_section_types.F:127
message_passing::mp_comm_type
Definition message_passing.F:161
message_passing::mp_para_env_type
stores all the informations relevant to an mpi environment
Definition message_passing.F:750
message_passing::mp_request_type
Definition message_passing.F:610
particle_list_types::particle_list_type
represent a list of objects
Definition particle_list_types.F:46
particle_types::particle_type
Definition particle_types.F:35
pw_env_types::pw_env_type
contained for different pw related things
Definition pw_env_types.F:70
pw_poisson_types::pw_poisson_type
environment for the poisson solver
Definition pw_poisson_types.F:123
pw_pool_types::pw_pool_p_type
to create arrays of pools
Definition pw_pool_types.F:135
pw_pool_types::pw_pool_type
Manages a pool of grids (to be used for example as tmp objects), but can also be used to instantiate ...
Definition pw_pool_types.F:83
pw_types::pw_c1d_gs_type
Definition pw_types.F:127
pw_types::pw_r3d_rs_type
Definition pw_types.F:62
qs_environment_types::qs_environment_type
Definition qs_environment_types.F:222
qs_kind_types::qs_kind_type
Provides all information about a quickstep kind.
Definition qs_kind_types.F:190
qs_ks_types::qs_ks_env_type
calculation environment to calculate the ks matrix, holds all the needed vars. assumes that the core ...
Definition qs_ks_types.F:137
qs_mo_types::mo_set_type
Definition qs_mo_types.F:47
qs_neighbor_list_types::neighbor_list_set_p_type
Definition qs_neighbor_list_types.F:67
qs_subsys_types::qs_subsys_type
Definition qs_subsys_types.F:56
qs_tddfpt2_types::tddfpt_ground_state_mos
Ground state molecular orbitals.
Definition qs_tddfpt2_types.F:85