mirror of
https://github.com/LCPQ/quantum_package
synced 2024-12-22 20:35:19 +01:00
Merge branch 'master' of github.com:LCPQ/quantum_package
Conflicts: src/MOGuess/NEEDED_MODULES
This commit is contained in:
commit
985562b645
@ -216,8 +216,9 @@ class H_apply(object):
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self.data["size_max"] = str(1024*128)
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self.data["copy_buffer"] = """
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call copy_h_apply_buffer_to_wf
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selection_criterion_min = selection_criterion_min*0.1d0
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selection_criterion_min = min(selection_criterion_min, maxval(select_max))*0.1d0
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selection_criterion = selection_criterion_min
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call write_double(output_Dets,selection_criterion,'Selection criterion')
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"""
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self.data["keys_work"] = """
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e_2_pert_buffer = 0.d0
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@ -230,16 +231,17 @@ class H_apply(object):
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self.data["omp_parallel"] += """&
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!$OMP REDUCTION (max:select_max_out)"""
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self.data["skip"] = """
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if ((i_generator < size(select_max)).and. &
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(select_max(i_generator) < selection_criterion_min*selection_criterion_factor)) then
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!$ call omp_set_lock(lck)
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do k=1,N_st
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norm_psi(k) = norm_psi(k) + psi_coef(i_generator,k)*psi_coef(i_generator,k)
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delta_pt2(k) = 0.d0
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pt2_old(k) = 0.d0
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enddo
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!$ call omp_unset_lock(lck)
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cycle
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if (i_generator < size_select_max) then
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if (select_max(i_generator) < selection_criterion_min*selection_criterion_factor) then
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!$ call omp_set_lock(lck)
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do k=1,N_st
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norm_psi(k) = norm_psi(k) + psi_coef(i_generator,k)*psi_coef(i_generator,k)
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delta_pt2(k) = 0.d0
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pt2_old(k) = 0.d0
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enddo
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!$ call omp_unset_lock(lck)
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cycle
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endif
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endif
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select_max(i_generator) = 0.d0
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"""
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@ -23,9 +23,9 @@ export QPACKAGE_ROOT=${QPACKAGE_ROOT}
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export PYTHONPATH+=:\${QPACKAGE_ROOT}/scripts
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export PATH+=:\${QPACKAGE_ROOT}/scripts
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export PATH+=:\${QPACKAGE_ROOT}/bin
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export QPACKAGE_CACHE_URL="http://qmcchem.ups-tlse.fr/files/scemama/quantum_package/cache
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export QPACKAGE_CACHE_URL="http://qmcchem.ups-tlse.fr/files/scemama/quantum_package/cache"
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export PATH+=:${QPACKAGE_ROOT}/irpf90/bin/
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"
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source ${QPACKAGE_ROOT}/irpf90/bin/irpman
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EOF
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source quantum_package.rc
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@ -4,5 +4,5 @@
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\int \left(\chi_i({\bf r}) \right)^2 dr = 1
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* The AO coefficients in the EZFIO files are not normalized
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* The AO coefficients in the EZFIO files are not necessarily normalized and are normalized after reading
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* The AO coefficients and exponents are ordered in increasing order of exponents
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@ -54,17 +54,17 @@ Documentation
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Coefficients, exponents and powers of x,y and z
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ao_coef(i,j) = coefficient of the jth primitive on the ith ao
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`ao_coef_transp <http://github.com/LCPQ/quantum_package/tree/master/src/AOs/aos.irp.f#L136>`_
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`ao_coef_transp <http://github.com/LCPQ/quantum_package/tree/master/src/AOs/aos.irp.f#L96>`_
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Transposed ao_coef and ao_expo
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`ao_expo <http://github.com/LCPQ/quantum_package/tree/master/src/AOs/aos.irp.f#L20>`_
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Coefficients, exponents and powers of x,y and z
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ao_coef(i,j) = coefficient of the jth primitive on the ith ao
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`ao_expo_transp <http://github.com/LCPQ/quantum_package/tree/master/src/AOs/aos.irp.f#L137>`_
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`ao_expo_transp <http://github.com/LCPQ/quantum_package/tree/master/src/AOs/aos.irp.f#L97>`_
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Transposed ao_coef and ao_expo
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`ao_nucl <http://github.com/LCPQ/quantum_package/tree/master/src/AOs/aos.irp.f#L186>`_
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`ao_nucl <http://github.com/LCPQ/quantum_package/tree/master/src/AOs/aos.irp.f#L146>`_
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Index of the nuclei on which the ao is centered
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`ao_num <http://github.com/LCPQ/quantum_package/tree/master/src/AOs/aos.irp.f#L1>`_
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@ -73,21 +73,17 @@ Documentation
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`ao_num_align <http://github.com/LCPQ/quantum_package/tree/master/src/AOs/aos.irp.f#L2>`_
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Number of atomic orbitals
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`ao_overlap <http://github.com/LCPQ/quantum_package/tree/master/src/AOs/aos.irp.f#L96>`_
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matrix of the overlap for tha AOs
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S(i,j) = overlap between the ith and the jth atomic basis function
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`ao_power <http://github.com/LCPQ/quantum_package/tree/master/src/AOs/aos.irp.f#L19>`_
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Coefficients, exponents and powers of x,y and z
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ao_coef(i,j) = coefficient of the jth primitive on the ith ao
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`ao_prim_num <http://github.com/LCPQ/quantum_package/tree/master/src/AOs/aos.irp.f#L154>`_
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`ao_prim_num <http://github.com/LCPQ/quantum_package/tree/master/src/AOs/aos.irp.f#L114>`_
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Number of primitives per atomic orbital
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`ao_prim_num_max <http://github.com/LCPQ/quantum_package/tree/master/src/AOs/aos.irp.f#L176>`_
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`ao_prim_num_max <http://github.com/LCPQ/quantum_package/tree/master/src/AOs/aos.irp.f#L136>`_
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Undocumented
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`ao_prim_num_max_align <http://github.com/LCPQ/quantum_package/tree/master/src/AOs/aos.irp.f#L177>`_
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`ao_prim_num_max_align <http://github.com/LCPQ/quantum_package/tree/master/src/AOs/aos.irp.f#L137>`_
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Undocumented
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|
@ -36,58 +36,58 @@ Documentation
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integral of the AO basis <ik|jl> or (ij|kl)
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i(r1) j(r1) 1/r12 k(r2) l(r2)
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`ao_bielec_integral_schwartz <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/ao_bi_integrals.irp.f#L326>`_
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`ao_bielec_integral_schwartz <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/ao_bi_integrals.irp.f#L341>`_
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Needed to compuet Schwartz inequalities
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`ao_bielec_integrals_in_map <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/ao_bi_integrals.irp.f#L189>`_
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`ao_bielec_integrals_in_map <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/ao_bi_integrals.irp.f#L188>`_
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Map of Atomic integrals
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i(r1) j(r2) 1/r12 k(r1) l(r2)
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`compute_ao_bielec_integrals <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/ao_bi_integrals.irp.f#L148>`_
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`compute_ao_bielec_integrals <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/ao_bi_integrals.irp.f#L147>`_
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Compute AO 1/r12 integrals for all i and fixed j,k,l
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`eri <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/ao_bi_integrals.irp.f#L487>`_
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`eri <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/ao_bi_integrals.irp.f#L502>`_
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ATOMIC PRIMTIVE bielectronic integral between the 4 primitives ::
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primitive_1 = x1**(a_x) y1**(a_y) z1**(a_z) exp(-alpha * r1**2)
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primitive_2 = x1**(b_x) y1**(b_y) z1**(b_z) exp(- beta * r1**2)
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primitive_3 = x2**(c_x) y2**(c_y) z2**(c_z) exp(-delta * r2**2)
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primitive_4 = x2**(d_x) y2**(d_y) z2**(d_z) exp(- gama * r2**2)
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`general_primitive_integral <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/ao_bi_integrals.irp.f#L352>`_
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`general_primitive_integral <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/ao_bi_integrals.irp.f#L367>`_
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Computes the integral <pq|rs> where p,q,r,s are Gaussian primitives
|
||||
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`give_polynom_mult_center_x <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/ao_bi_integrals.irp.f#L632>`_
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`give_polynom_mult_center_x <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/ao_bi_integrals.irp.f#L647>`_
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subroutine that returns the explicit polynom in term of the "t"
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variable of the following polynomw :
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I_x1(a_x, d_x,p,q) * I_x1(a_y, d_y,p,q) * I_x1(a_z, d_z,p,q)
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`i_x1_new <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/ao_bi_integrals.irp.f#L576>`_
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`i_x1_new <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/ao_bi_integrals.irp.f#L591>`_
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recursive function involved in the bielectronic integral
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`i_x1_pol_mult <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/ao_bi_integrals.irp.f#L695>`_
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`i_x1_pol_mult <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/ao_bi_integrals.irp.f#L710>`_
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recursive function involved in the bielectronic integral
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`i_x1_pol_mult_a1 <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/ao_bi_integrals.irp.f#L815>`_
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`i_x1_pol_mult_a1 <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/ao_bi_integrals.irp.f#L830>`_
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recursive function involved in the bielectronic integral
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||||
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`i_x1_pol_mult_a2 <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/ao_bi_integrals.irp.f#L869>`_
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`i_x1_pol_mult_a2 <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/ao_bi_integrals.irp.f#L884>`_
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recursive function involved in the bielectronic integral
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`i_x1_pol_mult_recurs <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/ao_bi_integrals.irp.f#L729>`_
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`i_x1_pol_mult_recurs <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/ao_bi_integrals.irp.f#L744>`_
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recursive function involved in the bielectronic integral
|
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`i_x2_new <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/ao_bi_integrals.irp.f#L599>`_
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`i_x2_new <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/ao_bi_integrals.irp.f#L614>`_
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recursive function involved in the bielectronic integral
|
||||
|
||||
`i_x2_pol_mult <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/ao_bi_integrals.irp.f#L931>`_
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`i_x2_pol_mult <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/ao_bi_integrals.irp.f#L946>`_
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recursive function involved in the bielectronic integral
|
||||
|
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`integrale_new <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/ao_bi_integrals.irp.f#L531>`_
|
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`integrale_new <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/ao_bi_integrals.irp.f#L546>`_
|
||||
calculate the integral of the polynom ::
|
||||
I_x1(a_x+b_x, c_x+d_x,p,q) * I_x1(a_y+b_y, c_y+d_y,p,q) * I_x1(a_z+b_z, c_z+d_z,p,q)
|
||||
between ( 0 ; 1)
|
||||
|
||||
`n_pt_sup <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/ao_bi_integrals.irp.f#L618>`_
|
||||
`n_pt_sup <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/ao_bi_integrals.irp.f#L633>`_
|
||||
Returns the upper boundary of the degree of the polynom involved in the
|
||||
bielctronic integral :
|
||||
Ix(a_x,b_x,c_x,d_x) * Iy(a_y,b_y,c_y,d_y) * Iz(a_z,b_z,c_z,d_z)
|
||||
@ -112,7 +112,7 @@ Documentation
|
||||
`clear_ao_map <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/map_integrals.irp.f#L128>`_
|
||||
Frees the memory of the AO map
|
||||
|
||||
`clear_mo_map <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/map_integrals.irp.f#L243>`_
|
||||
`clear_mo_map <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/map_integrals.irp.f#L285>`_
|
||||
Frees the memory of the MO map
|
||||
|
||||
`get_ao_bielec_integral <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/map_integrals.irp.f#L33>`_
|
||||
@ -136,7 +136,11 @@ Documentation
|
||||
Returns multiple integrals <ij|kl> in the MO basis, all
|
||||
i for j,k,l fixed.
|
||||
|
||||
`get_mo_map_size <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/map_integrals.irp.f#L235>`_
|
||||
`get_mo_bielec_integrals_existing_ik <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/map_integrals.irp.f#L235>`_
|
||||
Returns multiple integrals <ij|kl> in the MO basis, all
|
||||
i for j,k,l fixed.
|
||||
|
||||
`get_mo_map_size <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/map_integrals.irp.f#L277>`_
|
||||
Return the number of elements in the MO map
|
||||
|
||||
`insert_into_ao_integrals_map <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/map_integrals.irp.f#L153>`_
|
||||
@ -154,13 +158,13 @@ Documentation
|
||||
`add_integrals_to_map <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/mo_bi_integrals.irp.f#L40>`_
|
||||
Adds integrals to tha MO map according to some bitmask
|
||||
|
||||
`mo_bielec_integral_jj <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/mo_bi_integrals.irp.f#L296>`_
|
||||
`mo_bielec_integral_jj <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/mo_bi_integrals.irp.f#L305>`_
|
||||
Transform Bi-electronic integrals <ij|ij> and <ij|ji>
|
||||
|
||||
`mo_bielec_integral_jj_anti <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/mo_bi_integrals.irp.f#L298>`_
|
||||
`mo_bielec_integral_jj_anti <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/mo_bi_integrals.irp.f#L307>`_
|
||||
Transform Bi-electronic integrals <ij|ij> and <ij|ji>
|
||||
|
||||
`mo_bielec_integral_jj_exchange <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/mo_bi_integrals.irp.f#L297>`_
|
||||
`mo_bielec_integral_jj_exchange <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/mo_bi_integrals.irp.f#L306>`_
|
||||
Transform Bi-electronic integrals <ij|ij> and <ij|ji>
|
||||
|
||||
`mo_bielec_integrals_in_map <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/mo_bi_integrals.irp.f#L21>`_
|
||||
@ -169,22 +173,22 @@ Documentation
|
||||
`mo_bielec_integrals_index <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/mo_bi_integrals.irp.f#L1>`_
|
||||
Computes an unique index for i,j,k,l integrals
|
||||
|
||||
`ao_integrals_threshold <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/options.irp.f#L73>`_
|
||||
`ao_integrals_threshold <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/options.irp.f#L69>`_
|
||||
If <pq|rs> < ao_integrals_threshold, <pq|rs> = 0
|
||||
|
||||
`do_direct_integrals <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/options.irp.f#L111>`_
|
||||
`do_direct_integrals <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/options.irp.f#L105>`_
|
||||
If True, compute integrals on the fly
|
||||
|
||||
`mo_integrals_threshold <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/options.irp.f#L92>`_
|
||||
`mo_integrals_threshold <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/options.irp.f#L87>`_
|
||||
If <ij|kl> < mo_integrals_threshold, <ij|kl> = 0
|
||||
|
||||
`read_ao_integrals <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/options.irp.f#L55>`_
|
||||
`read_ao_integrals <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/options.irp.f#L52>`_
|
||||
If true, read AO integrals in EZFIO
|
||||
|
||||
`read_mo_integrals <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/options.irp.f#L37>`_
|
||||
`read_mo_integrals <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/options.irp.f#L35>`_
|
||||
If true, read MO integrals in EZFIO
|
||||
|
||||
`write_ao_integrals <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/options.irp.f#L19>`_
|
||||
`write_ao_integrals <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/options.irp.f#L18>`_
|
||||
If true, write AO integrals in EZFIO
|
||||
|
||||
`write_mo_integrals <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts/options.irp.f#L1>`_
|
||||
|
@ -57,7 +57,7 @@ Documentation
|
||||
`full_ijkl_bitmask <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks.irp.f#L12>`_
|
||||
Bitmask to include all possible MOs
|
||||
|
||||
`generators_bitmask <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks.irp.f#L91>`_
|
||||
`generators_bitmask <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks.irp.f#L88>`_
|
||||
Bitmasks for generator determinants. (N_int, alpha/beta, hole/particle, generator).
|
||||
3rd index is :
|
||||
* 1 : hole for single exc
|
||||
@ -70,10 +70,10 @@ Documentation
|
||||
`hf_bitmask <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks.irp.f#L32>`_
|
||||
Hartree Fock bit mask
|
||||
|
||||
`i_bitmask_gen <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks.irp.f#L182>`_
|
||||
`i_bitmask_gen <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks.irp.f#L174>`_
|
||||
Current bitmask for the generators
|
||||
|
||||
`i_bitmask_ref <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks.irp.f#L190>`_
|
||||
`i_bitmask_ref <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks.irp.f#L182>`_
|
||||
Current bitmask for the reference
|
||||
|
||||
`n_generators_bitmask <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks.irp.f#L58>`_
|
||||
@ -82,13 +82,13 @@ Documentation
|
||||
`n_int <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks.irp.f#L3>`_
|
||||
Number of 64-bit integers needed to represent determinants as binary strings
|
||||
|
||||
`n_reference_bitmask <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks.irp.f#L126>`_
|
||||
`n_reference_bitmask <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks.irp.f#L122>`_
|
||||
Number of bitmasks for reference
|
||||
|
||||
`ref_bitmask <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks.irp.f#L50>`_
|
||||
Reference bit mask, used in Slater rules, chosen as Hartree-Fock bitmask
|
||||
|
||||
`reference_bitmask <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks.irp.f#L159>`_
|
||||
`reference_bitmask <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks.irp.f#L152>`_
|
||||
Bitmasks for reference determinants. (N_int, alpha/beta, hole/particle, reference)
|
||||
|
||||
`bitstring_to_hexa <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask/bitmasks_routines.irp.f#L95>`_
|
||||
|
@ -28,6 +28,18 @@ BEGIN_PROVIDER [ integer(bit_kind), full_ijkl_bitmask, (N_int,4) ]
|
||||
enddo
|
||||
END_PROVIDER
|
||||
|
||||
|
||||
BEGIN_PROVIDER [ integer(bit_kind), cis_ijkl_bitmask, (N_int,4) ]
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! Bitmask to include all possible single excitations from Hartree-Fock
|
||||
END_DOC
|
||||
|
||||
integer :: i,j,n
|
||||
cis_ijkl_bitmask = full_ijkl_bitmask
|
||||
cis_ijkl_bitmask(:,1) = HF_bitmask(:,1)
|
||||
END_PROVIDER
|
||||
|
||||
|
||||
BEGIN_PROVIDER [ integer(bit_kind), HF_bitmask, (N_int,2)]
|
||||
implicit none
|
||||
|
1
src/CIS/ASSUMPTIONS.rst
Normal file
1
src/CIS/ASSUMPTIONS.rst
Normal file
@ -0,0 +1 @@
|
||||
* The molecular orbitals are assumed orthonormal
|
9
src/CIS/H_apply.irp.f
Normal file
9
src/CIS/H_apply.irp.f
Normal file
@ -0,0 +1,9 @@
|
||||
! Generates subroutine H_apply_cisd
|
||||
! ----------------------------------
|
||||
|
||||
BEGIN_SHELL [ /usr/bin/env python ]
|
||||
from generate_h_apply import H_apply
|
||||
H = H_apply("cis",do_double_exc=False)
|
||||
print H
|
||||
END_SHELL
|
||||
|
8
src/CIS/Makefile
Normal file
8
src/CIS/Makefile
Normal file
@ -0,0 +1,8 @@
|
||||
default: all
|
||||
|
||||
# Define here all new external source files and objects.Don't forget to prefix the
|
||||
# object files with IRPF90_temp/
|
||||
SRC=
|
||||
OBJ=
|
||||
|
||||
include $(QPACKAGE_ROOT)/src/Makefile.common
|
42
src/CIS/README.rst
Normal file
42
src/CIS/README.rst
Normal file
@ -0,0 +1,42 @@
|
||||
==========
|
||||
CIS Module
|
||||
==========
|
||||
|
||||
Assumptions
|
||||
===========
|
||||
|
||||
.. Do not edit this section. It was auto-generated from the
|
||||
.. NEEDED_MODULES file.
|
||||
|
||||
* The molecular orbitals are assumed orthonormal
|
||||
|
||||
|
||||
Documentation
|
||||
=============
|
||||
|
||||
.. Do not edit this section. It was auto-generated from the
|
||||
.. NEEDED_MODULES file.
|
||||
|
||||
|
||||
|
||||
Needed Modules
|
||||
==============
|
||||
|
||||
.. Do not edit this section. It was auto-generated from the
|
||||
.. NEEDED_MODULES file.
|
||||
|
||||
* `AOs <http://github.com/LCPQ/quantum_package/tree/master/src/AOs>`_
|
||||
* `BiInts <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts>`_
|
||||
* `Bitmask <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask>`_
|
||||
* `Dets <http://github.com/LCPQ/quantum_package/tree/master/src/Dets>`_
|
||||
* `Electrons <http://github.com/LCPQ/quantum_package/tree/master/src/Electrons>`_
|
||||
* `Ezfio_files <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files>`_
|
||||
* `Hartree_Fock <http://github.com/LCPQ/quantum_package/tree/master/src/Hartree_Fock>`_
|
||||
* `MonoInts <http://github.com/LCPQ/quantum_package/tree/master/src/MonoInts>`_
|
||||
* `MOs <http://github.com/LCPQ/quantum_package/tree/master/src/MOs>`_
|
||||
* `Nuclei <http://github.com/LCPQ/quantum_package/tree/master/src/Nuclei>`_
|
||||
* `Output <http://github.com/LCPQ/quantum_package/tree/master/src/Output>`_
|
||||
* `SingleRefMethod <http://github.com/LCPQ/quantum_package/tree/master/src/SingleRefMethod>`_
|
||||
* `Utils <http://github.com/LCPQ/quantum_package/tree/master/src/Utils>`_
|
||||
* `Selectors_full <http://github.com/LCPQ/quantum_package/tree/master/src/Selectors_full>`_
|
||||
|
17
src/CIS/cis.irp.f
Normal file
17
src/CIS/cis.irp.f
Normal file
@ -0,0 +1,17 @@
|
||||
program cis
|
||||
implicit none
|
||||
integer :: i
|
||||
|
||||
print *, 'HF = ', HF_energy
|
||||
print *, 'N_states = ', N_states
|
||||
call H_apply_cis
|
||||
print *, 'N_det = ', N_det
|
||||
do i = 1,N_states
|
||||
print *, 'energy = ',CI_energy(i)
|
||||
print *, 'E_corr = ',CI_electronic_energy(i) - ref_bitmask_energy
|
||||
enddo
|
||||
psi_coef = ci_eigenvectors
|
||||
SOFT_TOUCH psi_coef
|
||||
call save_wavefunction
|
||||
|
||||
end
|
61
src/CIS/super_ci.irp.f
Normal file
61
src/CIS/super_ci.irp.f
Normal file
@ -0,0 +1,61 @@
|
||||
program cis
|
||||
implicit none
|
||||
integer :: i
|
||||
|
||||
call super_CI
|
||||
|
||||
end
|
||||
|
||||
subroutine super_CI
|
||||
implicit none
|
||||
double precision :: E, delta_E, delta_D, E_min
|
||||
integer :: k
|
||||
character :: save_char
|
||||
|
||||
call write_time(output_hartree_fock)
|
||||
write(output_hartree_fock,'(A4,X,A16, X, A16, X, A16 )'), &
|
||||
'====','================','================','================'
|
||||
write(output_hartree_fock,'(A4,X,A16, X, A16, X, A16 )'), &
|
||||
' N ', 'Energy ', 'Energy diff ', 'Save '
|
||||
write(output_hartree_fock,'(A4,X,A16, X, A16, X, A16 )'), &
|
||||
'====','================','================','================'
|
||||
|
||||
E = HF_energy + 1.d0
|
||||
delta_D = 0.d0
|
||||
E_min = HF_energy
|
||||
FREE psi_det psi_coef
|
||||
call clear_mo_map
|
||||
N_det = 1
|
||||
SOFT_TOUCH N_det
|
||||
mo_coef = eigenvectors_fock_matrix_mo
|
||||
TOUCH mo_coef
|
||||
do k=1,n_it_scf_max
|
||||
delta_E = HF_energy - E
|
||||
E = HF_energy
|
||||
if (E < E_min) then
|
||||
call save_mos
|
||||
save_char = 'X'
|
||||
else
|
||||
save_char = ' '
|
||||
endif
|
||||
write(output_hartree_fock,'(I4,X,F16.10, X, F16.10, X, A8 )'),&
|
||||
k, E, delta_E, save_char
|
||||
if ( (delta_E < 0.d0).and.(dabs(delta_E) < thresh_scf) ) then
|
||||
exit
|
||||
endif
|
||||
call H_apply_cis
|
||||
call diagonalize_CI
|
||||
call set_natural_mos
|
||||
FREE psi_det psi_coef
|
||||
call clear_mo_map
|
||||
N_det = 1
|
||||
SOFT_TOUCH N_det
|
||||
mo_coef = eigenvectors_fock_matrix_mo
|
||||
TOUCH mo_coef
|
||||
enddo
|
||||
|
||||
write(output_hartree_fock,'(A4,X,A16, X, A16, X, A16 )'), &
|
||||
'====','================','================','================'
|
||||
call write_time(output_hartree_fock)
|
||||
end
|
||||
|
@ -17,12 +17,6 @@ Documentation
|
||||
`iunit_two_body_dm_bb <http://github.com/LCPQ/quantum_package/tree/master/src/DensityMatrix/density_matrix.irp.f#L4>`_
|
||||
Temporary files for 2-body dm calculation
|
||||
|
||||
`one_body_dm_a <http://github.com/LCPQ/quantum_package/tree/master/src/DensityMatrix/density_matrix.irp.f#L213>`_
|
||||
Alpha and beta one-body density matrix
|
||||
|
||||
`one_body_dm_b <http://github.com/LCPQ/quantum_package/tree/master/src/DensityMatrix/density_matrix.irp.f#L214>`_
|
||||
Alpha and beta one-body density matrix
|
||||
|
||||
`two_body_dm_diag_aa <http://github.com/LCPQ/quantum_package/tree/master/src/DensityMatrix/density_matrix.irp.f#L170>`_
|
||||
diagonal part of the two body density matrix
|
||||
|
||||
|
@ -152,6 +152,21 @@ Documentation
|
||||
`davidson_threshold <http://github.com/LCPQ/quantum_package/tree/master/src/Dets/davidson.irp.f#L374>`_
|
||||
Can be : [ energy | residual | both | wall_time | cpu_time | iterations ]
|
||||
|
||||
`one_body_dm_mo <http://github.com/LCPQ/quantum_package/tree/master/src/Dets/density_matrix.irp.f#L73>`_
|
||||
One-body density matrix
|
||||
|
||||
`one_body_dm_mo_alpha <http://github.com/LCPQ/quantum_package/tree/master/src/Dets/density_matrix.irp.f#L1>`_
|
||||
Alpha and beta one-body density matrix for each state
|
||||
|
||||
`one_body_dm_mo_beta <http://github.com/LCPQ/quantum_package/tree/master/src/Dets/density_matrix.irp.f#L2>`_
|
||||
Alpha and beta one-body density matrix for each state
|
||||
|
||||
`save_natural_mos <http://github.com/LCPQ/quantum_package/tree/master/src/Dets/density_matrix.irp.f#L81>`_
|
||||
Save natural orbitals, obtained by diagonalization of the one-body density matrix in the MO basis
|
||||
|
||||
`state_average_weight <http://github.com/LCPQ/quantum_package/tree/master/src/Dets/density_matrix.irp.f#L99>`_
|
||||
Weights in the state-average calculation of the density matrix
|
||||
|
||||
`det_search_key <http://github.com/LCPQ/quantum_package/tree/master/src/Dets/determinants.irp.f#L303>`_
|
||||
Return an integer*8 corresponding to a determinant index for searching
|
||||
|
||||
@ -307,6 +322,9 @@ Documentation
|
||||
`s_z2_sz <http://github.com/LCPQ/quantum_package/tree/master/src/Dets/s2.irp.f#L37>`_
|
||||
Undocumented
|
||||
|
||||
`save_natorb <http://github.com/LCPQ/quantum_package/tree/master/src/Dets/save_natorb.irp.f#L1>`_
|
||||
Undocumented
|
||||
|
||||
`a_operator <http://github.com/LCPQ/quantum_package/tree/master/src/Dets/slater_rules.irp.f#L721>`_
|
||||
Needed for diag_H_mat_elem
|
||||
|
||||
|
@ -78,10 +78,10 @@ BEGIN_PROVIDER [ double precision, one_body_dm_mo, (mo_tot_num_align,mo_tot_num)
|
||||
one_body_dm_mo = one_body_dm_mo_alpha + one_body_dm_mo_beta
|
||||
END_PROVIDER
|
||||
|
||||
subroutine save_natural_mos
|
||||
subroutine set_natural_mos
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! Save natural orbitals, obtained by diagonalization of the one-body density matrix in the MO basis
|
||||
! Set natural orbitals, obtained by diagonalization of the one-body density matrix in the MO basis
|
||||
END_DOC
|
||||
character*(64) :: label
|
||||
double precision, allocatable :: tmp(:,:)
|
||||
@ -92,9 +92,18 @@ subroutine save_natural_mos
|
||||
label = "Natural"
|
||||
call mo_as_eigvectors_of_mo_matrix(tmp,size(tmp,1),size(tmp,2),label)
|
||||
deallocate(tmp)
|
||||
call save_mos
|
||||
|
||||
end
|
||||
subroutine save_natural_mos
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! Save natural orbitals, obtained by diagonalization of the one-body density matrix in the MO basis
|
||||
END_DOC
|
||||
call set_natural_mos
|
||||
call save_mos
|
||||
|
||||
end
|
||||
|
||||
|
||||
BEGIN_PROVIDER [ double precision, state_average_weight, (N_states) ]
|
||||
implicit none
|
||||
|
@ -10,3 +10,7 @@ determinants
|
||||
n_det_max_jacobi integer
|
||||
threshold_generators double precision
|
||||
threshold_selectors double precision
|
||||
det_num integer
|
||||
det_occ integer (electrons_elec_alpha_num,determinants_det_num,2)
|
||||
det_coef double precision (determinants_det_num)
|
||||
|
||||
|
@ -56,7 +56,7 @@ BEGIN_PROVIDER [ integer, N_det_max_jacobi ]
|
||||
if (exists) then
|
||||
call ezfio_get_determinants_n_det_max_jacobi(N_det_max_jacobi)
|
||||
else
|
||||
N_det_max_jacobi = 2000
|
||||
N_det_max_jacobi = 10000
|
||||
endif
|
||||
call write_int(output_dets,N_det_max_jacobi,'Lapack diagonalization up to')
|
||||
ASSERT (N_det_max_jacobi > 0)
|
||||
|
37
src/Dets/save_for_qmcchem.irp.f
Normal file
37
src/Dets/save_for_qmcchem.irp.f
Normal file
@ -0,0 +1,37 @@
|
||||
subroutine save_dets_qmcchem
|
||||
use bitmasks
|
||||
implicit none
|
||||
character :: c(mo_tot_num)
|
||||
integer :: i,k
|
||||
|
||||
integer, allocatable :: occ(:,:,:), occ_tmp(:,:)
|
||||
!DIR$ ATTRIBUTES ALIGN : $IRP_ALIGN :: occ, occ_tmp
|
||||
|
||||
call ezfio_set_determinants_det_num(N_det)
|
||||
call ezfio_set_determinants_det_coef(psi_coef_sorted(1,1))
|
||||
|
||||
allocate (occ(elec_alpha_num,N_det,2))
|
||||
! OMP PARALLEL DEFAULT(NONE) &
|
||||
! OMP PRIVATE(occ_tmp,i,k)&
|
||||
! OMP SHARED(N_det,psi_det_sorted,elec_alpha_num, &
|
||||
! OMP occ,elec_beta_num,N_int)
|
||||
allocate (occ_tmp(N_int*bit_kind_size,2))
|
||||
occ_tmp = 0
|
||||
! OMP DO
|
||||
do i=1,N_det
|
||||
call bitstring_to_list(psi_det_sorted(1,1,i), occ_tmp(1,1), elec_alpha_num, N_int )
|
||||
call bitstring_to_list(psi_det_sorted(1,2,i), occ_tmp(1,2), elec_beta_num, N_int )
|
||||
do k=1,elec_alpha_num
|
||||
occ(k,i,1) = occ_tmp(k,1)
|
||||
occ(k,i,2) = occ_tmp(k,2)
|
||||
enddo
|
||||
enddo
|
||||
! OMP END DO
|
||||
deallocate(occ_tmp)
|
||||
! OMP END PARALLEL
|
||||
call ezfio_set_determinants_det_occ(occ)
|
||||
call write_int(output_dets,N_det,'Determinants saved for QMC')
|
||||
deallocate(occ)
|
||||
end
|
||||
|
||||
|
@ -11,7 +11,7 @@ program cisd
|
||||
|
||||
pt2 = 1.d0
|
||||
diag_algorithm = "Lapack"
|
||||
do while (maxval(abs(pt2(1:N_st))) > 1.d-4)
|
||||
do while (maxval(abs(pt2(1:N_st))) > 1.d-5)
|
||||
call H_apply_FCI(pt2, norm_pert, H_pert_diag, N_st)
|
||||
call diagonalize_CI
|
||||
call save_wavefunction
|
||||
@ -25,14 +25,16 @@ program cisd
|
||||
exit
|
||||
endif
|
||||
enddo
|
||||
! print *, 'Final step'
|
||||
call H_apply_FCI_PT2(pt2, norm_pert, H_pert_diag, N_st)
|
||||
|
||||
print *, 'Final step'
|
||||
! call remove_small_contributions
|
||||
! call diagonalize_CI
|
||||
! print *, 'N_det = ', N_det
|
||||
! print *, 'N_states = ', N_states
|
||||
! print *, 'PT2 = ', pt2
|
||||
! print *, 'E = ', CI_energy
|
||||
! print *, 'E+PT2 = ', CI_energy+pt2
|
||||
! print *, '-----'
|
||||
print *, 'N_det = ', N_det
|
||||
print *, 'N_states = ', N_states
|
||||
print *, 'PT2 = ', pt2
|
||||
print *, 'E = ', CI_energy
|
||||
print *, 'E+PT2 = ', CI_energy+pt2
|
||||
print *, '-----'
|
||||
deallocate(pt2,norm_pert)
|
||||
end
|
||||
|
@ -5,3 +5,45 @@ Generators_full Module
|
||||
All the determinants of the wave function are generators. In this way, the Full CI
|
||||
space is explored.
|
||||
|
||||
Documentation
|
||||
=============
|
||||
|
||||
.. Do not edit this section. It was auto-generated from the
|
||||
.. NEEDED_MODULES file.
|
||||
|
||||
`n_det_generators <http://github.com/LCPQ/quantum_package/tree/master/src/Generators_full/generators.irp.f#L22>`_
|
||||
For Single reference wave functions, the number of generators is 1 : the
|
||||
Hartree-Fock determinant
|
||||
|
||||
`psi_generators <http://github.com/LCPQ/quantum_package/tree/master/src/Generators_full/generators.irp.f#L44>`_
|
||||
For Single reference wave functions, the generator is the
|
||||
Hartree-Fock determinant
|
||||
|
||||
`select_max <http://github.com/LCPQ/quantum_package/tree/master/src/Generators_full/generators.irp.f#L60>`_
|
||||
Memo to skip useless selectors
|
||||
|
||||
`threshold_generators <http://github.com/LCPQ/quantum_package/tree/master/src/Generators_full/generators.irp.f#L3>`_
|
||||
Percentage of the norm of the state-averaged wave function to
|
||||
consider for the generators
|
||||
|
||||
|
||||
|
||||
Needed Modules
|
||||
==============
|
||||
|
||||
.. Do not edit this section. It was auto-generated from the
|
||||
.. NEEDED_MODULES file.
|
||||
|
||||
* `AOs <http://github.com/LCPQ/quantum_package/tree/master/src/AOs>`_
|
||||
* `BiInts <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts>`_
|
||||
* `Bitmask <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask>`_
|
||||
* `Dets <http://github.com/LCPQ/quantum_package/tree/master/src/Dets>`_
|
||||
* `Electrons <http://github.com/LCPQ/quantum_package/tree/master/src/Electrons>`_
|
||||
* `Ezfio_files <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files>`_
|
||||
* `Hartree_Fock <http://github.com/LCPQ/quantum_package/tree/master/src/Hartree_Fock>`_
|
||||
* `MonoInts <http://github.com/LCPQ/quantum_package/tree/master/src/MonoInts>`_
|
||||
* `MOs <http://github.com/LCPQ/quantum_package/tree/master/src/MOs>`_
|
||||
* `Nuclei <http://github.com/LCPQ/quantum_package/tree/master/src/Nuclei>`_
|
||||
* `Output <http://github.com/LCPQ/quantum_package/tree/master/src/Output>`_
|
||||
* `Utils <http://github.com/LCPQ/quantum_package/tree/master/src/Utils>`_
|
||||
|
||||
|
@ -57,7 +57,15 @@ BEGIN_PROVIDER [ integer(bit_kind), psi_generators, (N_int,2,psi_det_size) ]
|
||||
|
||||
END_PROVIDER
|
||||
|
||||
BEGIN_PROVIDER [ double precision, select_max, (3000) ]
|
||||
BEGIN_PROVIDER [ integer, size_select_max]
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! Size of the select_max array
|
||||
END_DOC
|
||||
size_select_max = 10000
|
||||
END_PROVIDER
|
||||
|
||||
BEGIN_PROVIDER [ double precision, select_max, (size_select_max) ]
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! Memo to skip useless selectors
|
||||
|
@ -260,3 +260,36 @@ BEGIN_PROVIDER [ double precision, Fock_matrix_ao, (ao_num_align, ao_num) ]
|
||||
endif
|
||||
END_PROVIDER
|
||||
|
||||
subroutine Fock_mo_to_ao(FMO,LDFMO,FAO,LDFAO)
|
||||
implicit none
|
||||
integer, intent(in) :: LDFMO ! size(FMO,1)
|
||||
integer, intent(in) :: LDFAO ! size(FAO,1)
|
||||
double precision, intent(in) :: FMO(LDFMO,*)
|
||||
double precision, intent(out) :: FAO(LDFAO,*)
|
||||
|
||||
double precision, allocatable :: T(:,:), M(:,:)
|
||||
! F_ao = S C F_mo C^t S
|
||||
allocate (T(mo_tot_num_align,mo_tot_num),M(ao_num_align,mo_tot_num))
|
||||
call dgemm('N','N', ao_num,ao_num,ao_num, 1.d0, &
|
||||
ao_overlap, size(ao_overlap,1), &
|
||||
mo_coef, size(mo_coef,1), &
|
||||
0.d0, &
|
||||
M, size(M,1))
|
||||
call dgemm('N','N', ao_num,mo_tot_num,mo_tot_num, 1.d0, &
|
||||
M, size(M,1), &
|
||||
FMO, size(FMO,1), &
|
||||
0.d0, &
|
||||
T, size(T,1))
|
||||
call dgemm('N','T', mo_tot_num,ao_num,mo_tot_num, 1.d0, &
|
||||
T, size(T,1), &
|
||||
mo_coef, size(mo_coef,1), &
|
||||
0.d0, &
|
||||
M, size(M,1))
|
||||
call dgemm('N','N', ao_num,ao_num,ao_num, 1.d0, &
|
||||
M, size(M,1), &
|
||||
ao_overlap, size(ao_overlap,1), &
|
||||
0.d0, &
|
||||
FAO, size(FAO,1))
|
||||
deallocate(T,M)
|
||||
end
|
||||
|
||||
|
@ -71,6 +71,9 @@ Documentation
|
||||
K = Fb - Fa
|
||||
.br
|
||||
|
||||
`fock_mo_to_ao <http://github.com/LCPQ/quantum_package/tree/master/src/Hartree_Fock/Fock_matrix.irp.f#L263>`_
|
||||
Undocumented
|
||||
|
||||
`hf_energy <http://github.com/LCPQ/quantum_package/tree/master/src/Hartree_Fock/Fock_matrix.irp.f#L211>`_
|
||||
Hartree-Fock energy
|
||||
|
||||
@ -83,25 +86,10 @@ Documentation
|
||||
`hf_density_matrix_ao_beta <http://github.com/LCPQ/quantum_package/tree/master/src/Hartree_Fock/HF_density_matrix_ao.irp.f#L14>`_
|
||||
Beta density matrix in the AO basis
|
||||
|
||||
`fock_mo_to_ao <http://github.com/LCPQ/quantum_package/tree/master/src/Hartree_Fock/SCF.irp.f#L31>`_
|
||||
`run <http://github.com/LCPQ/quantum_package/tree/master/src/Hartree_Fock/SCF.irp.f#L7>`_
|
||||
Undocumented
|
||||
|
||||
`insert_new_scf_density_matrix <http://github.com/LCPQ/quantum_package/tree/master/src/Hartree_Fock/SCF.irp.f#L19>`_
|
||||
Undocumented
|
||||
|
||||
`it_scf <http://github.com/LCPQ/quantum_package/tree/master/src/Hartree_Fock/SCF.irp.f#L1>`_
|
||||
Number of the current SCF iteration
|
||||
|
||||
`scf_density_matrices <http://github.com/LCPQ/quantum_package/tree/master/src/Hartree_Fock/SCF.irp.f#L9>`_
|
||||
Density matrices at every SCF iteration
|
||||
|
||||
`scf_energies <http://github.com/LCPQ/quantum_package/tree/master/src/Hartree_Fock/SCF.irp.f#L10>`_
|
||||
Density matrices at every SCF iteration
|
||||
|
||||
`scf_interpolation_step <http://github.com/LCPQ/quantum_package/tree/master/src/Hartree_Fock/SCF.irp.f#L64>`_
|
||||
Undocumented
|
||||
|
||||
`scf_iterations <http://github.com/LCPQ/quantum_package/tree/master/src/Hartree_Fock/SCF.irp.f#L89>`_
|
||||
`scf <http://github.com/LCPQ/quantum_package/tree/master/src/Hartree_Fock/SCF.irp.f#L2>`_
|
||||
Undocumented
|
||||
|
||||
`diagonal_fock_matrix_mo <http://github.com/LCPQ/quantum_package/tree/master/src/Hartree_Fock/diagonalize_fock.irp.f#L1>`_
|
||||
@ -110,12 +98,6 @@ Documentation
|
||||
`eigenvectors_fock_matrix_mo <http://github.com/LCPQ/quantum_package/tree/master/src/Hartree_Fock/diagonalize_fock.irp.f#L2>`_
|
||||
Diagonal Fock matrix in the MO basis
|
||||
|
||||
`run <http://github.com/LCPQ/quantum_package/tree/master/src/Hartree_Fock/mo_SCF_iterations.irp.f#L7>`_
|
||||
Undocumented
|
||||
|
||||
`scf <http://github.com/LCPQ/quantum_package/tree/master/src/Hartree_Fock/mo_SCF_iterations.irp.f#L2>`_
|
||||
Undocumented
|
||||
|
||||
`do_diis <http://github.com/LCPQ/quantum_package/tree/master/src/Hartree_Fock/options.irp.f#L39>`_
|
||||
If True, compute integrals on the fly
|
||||
|
||||
|
@ -1,108 +1,23 @@
|
||||
BEGIN_PROVIDER [ integer, it_scf ]
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! Number of the current SCF iteration
|
||||
END_DOC
|
||||
it_scf = 0
|
||||
END_PROVIDER
|
||||
|
||||
BEGIN_PROVIDER [ double precision, SCF_density_matrices, (ao_num_align,ao_num,2,n_it_scf_max) ]
|
||||
&BEGIN_PROVIDER [ double precision, SCF_energies, (n_it_scf_max) ]
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! Density matrices at every SCF iteration
|
||||
END_DOC
|
||||
SCF_density_matrices = 0.d0
|
||||
SCF_energies = 0.d0
|
||||
END_PROVIDER
|
||||
|
||||
subroutine insert_new_SCF_density_matrix
|
||||
implicit none
|
||||
integer :: i,j
|
||||
do j=1,ao_num
|
||||
do i=1,ao_num
|
||||
SCF_density_matrices(i,j,1,it_scf) = HF_density_matrix_ao_alpha(i,j)
|
||||
SCF_density_matrices(i,j,2,it_scf) = HF_density_matrix_ao_beta(i,j)
|
||||
enddo
|
||||
enddo
|
||||
SCF_energies(it_scf) = HF_energy
|
||||
program scf
|
||||
call orthonormalize_mos
|
||||
call run
|
||||
end
|
||||
|
||||
subroutine Fock_mo_to_ao(FMO,LDFMO,FAO,LDFAO)
|
||||
subroutine run
|
||||
|
||||
use bitmasks
|
||||
implicit none
|
||||
integer, intent(in) :: LDFMO ! size(FMO,1)
|
||||
integer, intent(in) :: LDFAO ! size(FAO,1)
|
||||
double precision, intent(in) :: FMO(LDFMO,*)
|
||||
double precision, intent(out) :: FAO(LDFAO,*)
|
||||
double precision :: SCF_energy_before,SCF_energy_after,diag_H_mat_elem,get_mo_bielec_integral
|
||||
double precision :: E0
|
||||
integer :: i_it, i, j, k
|
||||
|
||||
E0 = HF_energy
|
||||
|
||||
double precision, allocatable :: T(:,:), M(:,:)
|
||||
! F_ao = S C F_mo C^t S
|
||||
allocate (T(mo_tot_num_align,mo_tot_num),M(ao_num_align,mo_tot_num))
|
||||
call dgemm('N','N', ao_num,ao_num,ao_num, 1.d0, &
|
||||
ao_overlap, size(ao_overlap,1), &
|
||||
mo_coef, size(mo_coef,1), &
|
||||
0.d0, &
|
||||
M, size(M,1))
|
||||
call dgemm('N','N', ao_num,mo_tot_num,mo_tot_num, 1.d0, &
|
||||
M, size(M,1), &
|
||||
FMO, size(FMO,1), &
|
||||
0.d0, &
|
||||
T, size(T,1))
|
||||
call dgemm('N','T', mo_tot_num,ao_num,mo_tot_num, 1.d0, &
|
||||
T, size(T,1), &
|
||||
mo_coef, size(mo_coef,1), &
|
||||
0.d0, &
|
||||
M, size(M,1))
|
||||
call dgemm('N','N', ao_num,ao_num,ao_num, 1.d0, &
|
||||
M, size(M,1), &
|
||||
ao_overlap, size(ao_overlap,1), &
|
||||
0.d0, &
|
||||
FAO, size(FAO,1))
|
||||
deallocate(T,M)
|
||||
end
|
||||
|
||||
subroutine SCF_interpolation_step
|
||||
implicit none
|
||||
integer :: i,j
|
||||
double precision :: c
|
||||
thresh_SCF = 1.d-10
|
||||
call damping_SCF
|
||||
mo_label = "Canonical"
|
||||
TOUCH mo_label mo_coef
|
||||
call save_mos
|
||||
|
||||
if (it_scf == 1) then
|
||||
return
|
||||
endif
|
||||
call random_number(c)
|
||||
c = c*0.5d0
|
||||
do j=1,ao_num
|
||||
do i=1,ao_num
|
||||
HF_density_matrix_ao_alpha(i,j) = c*SCF_density_matrices(i,j,1,it_scf-1)+SCF_density_matrices(i,j,1,it_scf) * (1.d0 - c)
|
||||
HF_density_matrix_ao_beta (i,j) = c*SCF_density_matrices(i,j,2,it_scf-1)+SCF_density_matrices(i,j,2,it_scf) * (1.d0 - c)
|
||||
enddo
|
||||
enddo
|
||||
TOUCH HF_density_matrix_ao_alpha HF_density_matrix_ao_beta
|
||||
|
||||
! call Fock_mo_to_ao(Fock_matrix_mo_alpha, size(Fock_matrix_mo_alpha,1),&
|
||||
! Fock_matrix_alpha_ao, size(Fock_matrix_alpha_ao,1) )
|
||||
! call Fock_mo_to_ao(Fock_matrix_mo_beta, size(Fock_matrix_mo_beta,1),&
|
||||
! Fock_matrix_beta_ao, size(Fock_matrix_beta_ao,1) )
|
||||
! SOFT_TOUCH Fock_matrix_alpha_ao Fock_matrix_beta_ao Fock_matrix_mo_alpha Fock_matrix_mo_beta
|
||||
end
|
||||
|
||||
subroutine scf_iterations
|
||||
implicit none
|
||||
integer :: i,j
|
||||
do i=1,n_it_scf_max
|
||||
it_scf += 1
|
||||
SOFT_TOUCH it_scf
|
||||
mo_coef = eigenvectors_Fock_matrix_mo
|
||||
TOUCH mo_coef
|
||||
call insert_new_SCF_density_matrix
|
||||
print *, HF_energy
|
||||
if (SCF_energies(it_scf)>SCF_energies(it_scf-1)) then
|
||||
call SCF_interpolation_step
|
||||
endif
|
||||
if (it_scf>1 ) then
|
||||
if (dabs(SCF_energies(it_scf)-SCF_energies(it_scf-1)) < thresh_SCF) then
|
||||
exit
|
||||
endif
|
||||
endif
|
||||
enddo
|
||||
end
|
||||
|
123
src/Hartree_Fock/damping_SCF.irp.f
Normal file
123
src/Hartree_Fock/damping_SCF.irp.f
Normal file
@ -0,0 +1,123 @@
|
||||
subroutine damping_SCF
|
||||
implicit none
|
||||
double precision :: E
|
||||
double precision, allocatable :: D_alpha(:,:), D_beta(:,:)
|
||||
double precision :: E_new
|
||||
double precision, allocatable :: D_new_alpha(:,:), D_new_beta(:,:), F_new(:,:)
|
||||
double precision, allocatable :: delta_alpha(:,:), delta_beta(:,:)
|
||||
double precision :: lambda, E_half, a, b, delta_D, delta_E, E_min
|
||||
|
||||
integer :: i,j,k
|
||||
logical :: saving
|
||||
character :: save_char
|
||||
|
||||
allocate( &
|
||||
D_alpha( ao_num_align, ao_num ), &
|
||||
D_beta( ao_num_align, ao_num ), &
|
||||
F_new( ao_num_align, ao_num ), &
|
||||
D_new_alpha( ao_num_align, ao_num ), &
|
||||
D_new_beta( ao_num_align, ao_num ), &
|
||||
delta_alpha( ao_num_align, ao_num ), &
|
||||
delta_beta( ao_num_align, ao_num ))
|
||||
|
||||
do j=1,ao_num
|
||||
do i=1,ao_num
|
||||
D_alpha(i,j) = HF_density_matrix_ao_alpha(i,j)
|
||||
D_beta (i,j) = HF_density_matrix_ao_beta (i,j)
|
||||
enddo
|
||||
enddo
|
||||
|
||||
|
||||
call write_time(output_hartree_fock)
|
||||
|
||||
write(output_hartree_fock,'(A4,X,A16, X, A16, X, A16, X, A4 )'), '====','================','================','================', '===='
|
||||
write(output_hartree_fock,'(A4,X,A16, X, A16, X, A16, X, A4 )'), ' N ', 'Energy ', 'Energy diff ', 'Density diff ', 'Save'
|
||||
write(output_hartree_fock,'(A4,X,A16, X, A16, X, A16, X, A4 )'), '====','================','================','================', '===='
|
||||
|
||||
E = HF_energy + 1.d0
|
||||
E_min = HF_energy
|
||||
delta_D = 0.d0
|
||||
do k=1,n_it_scf_max
|
||||
|
||||
delta_E = HF_energy - E
|
||||
E = HF_energy
|
||||
|
||||
if ( (delta_E < 0.d0).and.(dabs(delta_E) < thresh_scf) ) then
|
||||
exit
|
||||
endif
|
||||
|
||||
saving = E < E_min
|
||||
if (saving) then
|
||||
call save_mos
|
||||
save_char = 'X'
|
||||
E_min = E
|
||||
else
|
||||
save_char = ' '
|
||||
endif
|
||||
|
||||
write(output_hartree_fock,'(I4,X,F16.10, X, F16.10, X, F16.10, 3X, A )'), &
|
||||
k, E, delta_E, delta_D, save_char
|
||||
|
||||
D_alpha = HF_density_matrix_ao_alpha
|
||||
D_beta = HF_density_matrix_ao_beta
|
||||
mo_coef = eigenvectors_fock_matrix_mo
|
||||
TOUCH mo_coef
|
||||
|
||||
D_new_alpha = HF_density_matrix_ao_alpha
|
||||
D_new_beta = HF_density_matrix_ao_beta
|
||||
F_new = Fock_matrix_ao
|
||||
E_new = HF_energy
|
||||
|
||||
delta_alpha = D_new_alpha - D_alpha
|
||||
delta_beta = D_new_beta - D_beta
|
||||
|
||||
lambda = 0.5d0
|
||||
E_half = 0.d0
|
||||
do while (E_half > E)
|
||||
HF_density_matrix_ao_alpha = D_alpha + lambda * delta_alpha
|
||||
HF_density_matrix_ao_beta = D_beta + lambda * delta_beta
|
||||
TOUCH HF_density_matrix_ao_alpha HF_density_matrix_ao_beta
|
||||
mo_coef = eigenvectors_fock_matrix_mo
|
||||
TOUCH mo_coef
|
||||
E_half = HF_energy
|
||||
if ((E_half > E).and.(E_new < E)) then
|
||||
lambda = 1.d0
|
||||
exit
|
||||
else if ((E_half > E).and.(lambda > 1.d-3)) then
|
||||
lambda = 0.5d0 * lambda
|
||||
E_new = E_half
|
||||
else
|
||||
exit
|
||||
endif
|
||||
enddo
|
||||
|
||||
a = (E_new + E - 2.d0*E_half)*2.d0
|
||||
b = -E_new - 3.d0*E + 4.d0*E_half
|
||||
lambda = -lambda*b/a
|
||||
D_alpha = (1.d0-lambda) * D_alpha + lambda * D_new_alpha
|
||||
D_beta = (1.d0-lambda) * D_beta + lambda * D_new_beta
|
||||
delta_E = HF_energy - E
|
||||
do j=1,ao_num
|
||||
do i=1,ao_num
|
||||
delta_D = delta_D + &
|
||||
(D_alpha(i,j) - HF_density_matrix_ao_alpha(i,j))*(D_alpha(i,j) - HF_density_matrix_ao_alpha(i,j)) + &
|
||||
(D_beta (i,j) - HF_density_matrix_ao_beta (i,j))*(D_beta (i,j) - HF_density_matrix_ao_beta (i,j))
|
||||
enddo
|
||||
enddo
|
||||
delta_D = dsqrt(delta_D/dble(ao_num)**2)
|
||||
HF_density_matrix_ao_alpha = D_alpha
|
||||
HF_density_matrix_ao_beta = D_beta
|
||||
TOUCH HF_density_matrix_ao_alpha HF_density_matrix_ao_beta
|
||||
mo_coef = eigenvectors_fock_matrix_mo
|
||||
TOUCH mo_coef
|
||||
|
||||
|
||||
enddo
|
||||
write(output_hartree_fock,'(A4,X,A16, X, A16, X, A16, X, A4 )'), '====','================','================','================', '===='
|
||||
write(output_hartree_fock,*)
|
||||
|
||||
call write_double(output_hartree_fock, HF_energy, 'Hartree-Fock energy')
|
||||
call write_time(output_hartree_fock)
|
||||
|
||||
deallocate(D_alpha,D_beta,F_new,D_new_alpha,D_new_beta,delta_alpha,delta_beta)
|
||||
end
|
@ -1,23 +0,0 @@
|
||||
|
||||
program scf
|
||||
call orthonormalize_mos
|
||||
call run
|
||||
end
|
||||
|
||||
subroutine run
|
||||
|
||||
use bitmasks
|
||||
implicit none
|
||||
double precision :: SCF_energy_before,SCF_energy_after,diag_H_mat_elem,get_mo_bielec_integral
|
||||
double precision :: E0
|
||||
integer :: i_it, i, j, k
|
||||
|
||||
E0 = HF_energy
|
||||
|
||||
thresh_SCF = 1.d-10
|
||||
call damping_SCF
|
||||
mo_label = "Canonical"
|
||||
TOUCH mo_label mo_coef
|
||||
call save_mos
|
||||
|
||||
end
|
@ -9,12 +9,13 @@ Needed Modules
|
||||
.. NEEDED_MODULES file.
|
||||
|
||||
* `AOs <http://github.com/LCPQ/quantum_package/tree/master/src/AOs>`_
|
||||
* `Electrons <http://github.com/LCPQ/quantum_package/tree/master/src/Electrons>`_
|
||||
* `Ezfio_files <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files>`_
|
||||
* `MonoInts <http://github.com/LCPQ/quantum_package/tree/master/src/MonoInts>`_
|
||||
* `MOs <http://github.com/LCPQ/quantum_package/tree/master/src/MOs>`_
|
||||
* `Nuclei <http://github.com/LCPQ/quantum_package/tree/master/src/Nuclei>`_
|
||||
* `Output <http://github.com/LCPQ/quantum_package/tree/master/src/Output>`_
|
||||
* `Utils <http://github.com/LCPQ/quantum_package/tree/master/src/Utils>`_
|
||||
* `MonoInts <http://github.com/LCPQ/quantum_package/tree/master/src/MonoInts>`_
|
||||
|
||||
Documentation
|
||||
=============
|
||||
@ -22,19 +23,19 @@ Documentation
|
||||
.. Do not edit this section. It was auto-generated from the
|
||||
.. NEEDED_MODULES file.
|
||||
|
||||
`h_core_guess <http://github.com/LCPQ/quantum_package/tree/master/src/MOGuess/H_CORE_guess.irp.f#L/subroutine h_core_guess/;">`_
|
||||
`h_core_guess <http://github.com/LCPQ/quantum_package/tree/master/src/MOGuess/H_CORE_guess.irp.f#L1>`_
|
||||
Undocumented
|
||||
|
||||
`ao_ortho_lowdin_coef <http://github.com/LCPQ/quantum_package/tree/master/src/MOGuess/mo_ortho_lowdin.irp.f#L/BEGIN_PROVIDER [double precision, ao_ortho_lowdin_coef, (ao_num_align,ao_num)]/;">`_
|
||||
`ao_ortho_lowdin_coef <http://github.com/LCPQ/quantum_package/tree/master/src/MOGuess/mo_ortho_lowdin.irp.f#L2>`_
|
||||
matrix of the coefficients of the mos generated by the
|
||||
orthonormalization by the S^{-1/2} canonical transformation of the aos
|
||||
ao_ortho_lowdin_coef(i,j) = coefficient of the ith ao on the jth ao_ortho_lowdin orbital
|
||||
|
||||
`ao_ortho_lowdin_overlap <http://github.com/LCPQ/quantum_package/tree/master/src/MOGuess/mo_ortho_lowdin.irp.f#L/BEGIN_PROVIDER [double precision, ao_ortho_lowdin_overlap, (ao_num_align,ao_num)]/;">`_
|
||||
`ao_ortho_lowdin_overlap <http://github.com/LCPQ/quantum_package/tree/master/src/MOGuess/mo_ortho_lowdin.irp.f#L26>`_
|
||||
overlap matrix of the ao_ortho_lowdin
|
||||
supposed to be the Identity
|
||||
|
||||
`ao_ortho_lowdin_nucl_elec_integral <http://github.com/LCPQ/quantum_package/tree/master/src/MOGuess/pot_mo_ortho_lowdin_ints.irp.f#L/BEGIN_PROVIDER [double precision, ao_ortho_lowdin_nucl_elec_integral, (mo_tot_num_align,mo_tot_num)]/;">`_
|
||||
`ao_ortho_lowdin_nucl_elec_integral <http://github.com/LCPQ/quantum_package/tree/master/src/MOGuess/pot_mo_ortho_lowdin_ints.irp.f#L1>`_
|
||||
Undocumented
|
||||
|
||||
|
||||
|
@ -36,12 +36,15 @@ Documentation
|
||||
.. NEEDED_MODULES file.
|
||||
|
||||
`cholesky_mo <http://github.com/LCPQ/quantum_package/tree/master/src/MOs/cholesky_mo.irp.f#L1>`_
|
||||
Cholesky decomposition of MO Density matrix to
|
||||
Cholesky decomposition of AO Density matrix to
|
||||
generate MOs
|
||||
|
||||
`mo_density_matrix <http://github.com/LCPQ/quantum_package/tree/master/src/MOs/cholesky_mo.irp.f#L44>`_
|
||||
Density matrix in MO basis
|
||||
|
||||
`mo_density_matrix_virtual <http://github.com/LCPQ/quantum_package/tree/master/src/MOs/cholesky_mo.irp.f#L64>`_
|
||||
Density matrix in MO basis (virtual MOs)
|
||||
|
||||
`mo_coef <http://github.com/LCPQ/quantum_package/tree/master/src/MOs/mos.irp.f#L22>`_
|
||||
Molecular orbital coefficients on AO basis set
|
||||
mo_coef(i,j) = coefficient of the ith ao on the jth mo
|
||||
|
@ -1,5 +1,4 @@
|
||||
mo_basis
|
||||
ao_num integer
|
||||
mo_tot_num integer
|
||||
mo_coef double precision (ao_basis_ao_num,mo_basis_mo_tot_num)
|
||||
mo_label character*(64)
|
||||
|
@ -1,6 +1,6 @@
|
||||
OPENMP =1
|
||||
PROFILE =0
|
||||
DEBUG = 1
|
||||
DEBUG = 0
|
||||
|
||||
IRPF90_FLAGS+= --align=32
|
||||
FC = ifort -g
|
||||
|
@ -55,7 +55,7 @@ subroutine write_double(iunit,value,label)
|
||||
integer, intent(in) :: iunit
|
||||
double precision :: value
|
||||
character*(*) :: label
|
||||
character*(64), parameter :: f = '(A50,G16.8)'
|
||||
character*(64), parameter :: f = '(A50,G24.16)'
|
||||
character*(50) :: newlabel
|
||||
write(newlabel,'(A,A)') '* ',trim(label)
|
||||
write(iunit,f) newlabel, value
|
||||
|
@ -82,7 +82,7 @@ Documentation
|
||||
.. Do not edit this section. It was auto-generated from the
|
||||
.. NEEDED_MODULES file.
|
||||
|
||||
`pt2_moller_plesset <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/Moller_plesset.irp.f#L/subroutine pt2_moller_plesset(det_pert,c_pert,e_2_pert,H_pert_diag,Nint,ndet,n_st)/;">`_
|
||||
`pt2_moller_plesset <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/Moller_plesset.irp.f#L1>`_
|
||||
compute the standard Moller-Plesset perturbative first order coefficient and second order energetic contribution
|
||||
.br
|
||||
for the various n_st states.
|
||||
@ -92,7 +92,7 @@ Documentation
|
||||
e_2_pert(i) = <psi(i)|H|det_pert>^2/(difference of orbital energies)
|
||||
.br
|
||||
|
||||
`pt2_epstein_nesbet <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/epstein_nesbet.irp.f#L/subroutine pt2_epstein_nesbet(det_pert,c_pert,e_2_pert,H_pert_diag,Nint,ndet,N_st)/;">`_
|
||||
`pt2_epstein_nesbet <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/epstein_nesbet.irp.f#L1>`_
|
||||
compute the standard Epstein-Nesbet perturbative first order coefficient and second order energetic contribution
|
||||
.br
|
||||
for the various N_st states.
|
||||
@ -102,7 +102,7 @@ Documentation
|
||||
e_2_pert(i) = <psi(i)|H|det_pert>^2/( E(i) - <det_pert|H|det_pert> )
|
||||
.br
|
||||
|
||||
`pt2_epstein_nesbet_2x2 <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/epstein_nesbet.irp.f#L/subroutine pt2_epstein_nesbet_2x2(det_pert,c_pert,e_2_pert,H_pert_diag,Nint,ndet,N_st)/;">`_
|
||||
`pt2_epstein_nesbet_2x2 <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/epstein_nesbet.irp.f#L43>`_
|
||||
compute the Epstein-Nesbet 2x2 diagonalization coefficient and energetic contribution
|
||||
.br
|
||||
for the various N_st states.
|
||||
@ -112,7 +112,7 @@ Documentation
|
||||
c_pert(i) = e_2_pert(i)/ <psi(i)|H|det_pert>
|
||||
.br
|
||||
|
||||
`pt2_epstein_nesbet_sc2_projected <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/pert_sc2.irp.f#L/subroutine pt2_epstein_nesbet_SC2_projected(det_pert,c_pert,e_2_pert,H_pert_diag,Nint,ndet,N_st)/;">`_
|
||||
`pt2_epstein_nesbet_sc2_projected <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/pert_sc2.irp.f#L2>`_
|
||||
compute the Epstein-Nesbet perturbative first order coefficient and second order energetic contribution
|
||||
.br
|
||||
for the various N_st states,
|
||||
@ -135,23 +135,23 @@ Documentation
|
||||
.br
|
||||
H_pert_diag = <HF|H|det_pert> c_pert
|
||||
|
||||
`repeat_all_e_corr <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/pert_sc2.irp.f#L/double precision function repeat_all_e_corr(key_in)/;">`_
|
||||
`repeat_all_e_corr <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/pert_sc2.irp.f#L90>`_
|
||||
Undocumented
|
||||
|
||||
`fill_h_apply_buffer_selection <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/selection.irp.f#L/subroutine fill_H_apply_buffer_selection(n_selected,det_buffer,e_2_pert_buffer,coef_pert_buffer, &>`_
|
||||
`fill_h_apply_buffer_selection <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/selection.irp.f#L1>`_
|
||||
Fill the H_apply buffer with determiants for the selection
|
||||
|
||||
`remove_small_contributions <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/selection.irp.f#L/subroutine remove_small_contributions/;">`_
|
||||
`remove_small_contributions <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/selection.irp.f#L84>`_
|
||||
Remove determinants with small contributions. N_states is assumed to be
|
||||
provided.
|
||||
|
||||
`selection_criterion <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/selection.irp.f#L/BEGIN_PROVIDER [ double precision, selection_criterion ]/;">`_
|
||||
`selection_criterion <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/selection.irp.f#L71>`_
|
||||
Threshold to select determinants. Set by selection routines.
|
||||
|
||||
`selection_criterion_factor <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/selection.irp.f#L/&BEGIN_PROVIDER [ double precision, selection_criterion_factor ]/;">`_
|
||||
`selection_criterion_factor <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/selection.irp.f#L73>`_
|
||||
Threshold to select determinants. Set by selection routines.
|
||||
|
||||
`selection_criterion_min <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/selection.irp.f#L/&BEGIN_PROVIDER [ double precision, selection_criterion_min ]/;">`_
|
||||
`selection_criterion_min <http://github.com/LCPQ/quantum_package/tree/master/src/Perturbation/selection.irp.f#L72>`_
|
||||
Threshold to select determinants. Set by selection routines.
|
||||
|
||||
|
||||
|
@ -8,67 +8,9 @@ Documentation
|
||||
.. Do not edit this section. It was auto-generated from the
|
||||
.. NEEDED_MODULES file.
|
||||
|
||||
`cisd_sc2 <http://github.com/LCPQ/quantum_package/tree/master/src/SC2/SC2.irp.f#L1>`_
|
||||
CISD+SC2 method :: take off all the disconnected terms of a CISD (selected or not)
|
||||
.br
|
||||
dets_in : bitmasks corresponding to determinants
|
||||
.br
|
||||
u_in : guess coefficients on the various states. Overwritten
|
||||
on exit
|
||||
.br
|
||||
dim_in : leftmost dimension of u_in
|
||||
.br
|
||||
sze : Number of determinants
|
||||
.br
|
||||
N_st : Number of eigenstates
|
||||
.br
|
||||
Initial guess vectors are not necessarily orthonormal
|
||||
|
||||
`repeat_excitation <http://github.com/LCPQ/quantum_package/tree/master/src/SC2/SC2.irp.f#L169>`_
|
||||
Undocumented
|
||||
|
||||
`cisd <http://github.com/LCPQ/quantum_package/tree/master/src/SC2/cisd_SC2.irp.f#L1>`_
|
||||
Undocumented
|
||||
|
||||
`ci_sc2_eigenvectors <http://github.com/LCPQ/quantum_package/tree/master/src/SC2/diagonalize_CI_SC2.irp.f#L19>`_
|
||||
Eigenvectors/values of the CI matrix
|
||||
|
||||
`ci_sc2_electronic_energy <http://github.com/LCPQ/quantum_package/tree/master/src/SC2/diagonalize_CI_SC2.irp.f#L18>`_
|
||||
Eigenvectors/values of the CI matrix
|
||||
|
||||
`ci_sc2_energy <http://github.com/LCPQ/quantum_package/tree/master/src/SC2/diagonalize_CI_SC2.irp.f#L1>`_
|
||||
N_states lowest eigenvalues of the CI matrix
|
||||
|
||||
`diagonalize_ci_sc2 <http://github.com/LCPQ/quantum_package/tree/master/src/SC2/diagonalize_CI_SC2.irp.f#L38>`_
|
||||
Replace the coefficients of the CI states by the coefficients of the
|
||||
eigenstates of the CI matrix
|
||||
|
||||
`pt2_epstein_nesbet_sc2_projected <http://github.com/LCPQ/quantum_package/tree/master/src/SC2/pert_sc2.irp.f#L2>`_
|
||||
compute the Epstein-Nesbet perturbative first order coefficient and second order energetic contribution
|
||||
.br
|
||||
for the various N_st states,
|
||||
.br
|
||||
but with the correction in the denominator
|
||||
.br
|
||||
comming from the interaction of that determinant with all the others determinants
|
||||
.br
|
||||
that can be repeated by repeating all the double excitations
|
||||
.br
|
||||
: you repeat all the correlation energy already taken into account in CI_electronic_energy(1)
|
||||
.br
|
||||
that could be repeated to this determinant.
|
||||
.br
|
||||
In addition, for the perturbative energetic contribution you have the standard second order
|
||||
.br
|
||||
e_2_pert = <psi_i|H|det_pert>^2/(Delta_E)
|
||||
.br
|
||||
and also the purely projected contribution
|
||||
.br
|
||||
H_pert_diag = <HF|H|det_pert> c_pert
|
||||
|
||||
`repeat_all_e_corr <http://github.com/LCPQ/quantum_package/tree/master/src/SC2/pert_sc2.irp.f#L82>`_
|
||||
Undocumented
|
||||
|
||||
|
||||
|
||||
Needed Modules
|
||||
|
@ -2,3 +2,96 @@
|
||||
Selectors_full Module
|
||||
=====================
|
||||
|
||||
Documentation
|
||||
=============
|
||||
|
||||
.. Do not edit this section. It was auto-generated from the
|
||||
.. NEEDED_MODULES file.
|
||||
|
||||
`coef_hf_selector <http://github.com/LCPQ/quantum_package/tree/master/src/Selectors_full/e_corr_selectors.irp.f#L27>`_
|
||||
energy of correlation per determinant respect to the Hartree Fock determinant
|
||||
.br
|
||||
for the all the double excitations in the selectors determinants
|
||||
.br
|
||||
E_corr_per_selectors(i) = <D_i|H|HF> * c(D_i)/c(HF) if |D_i> is a double excitation
|
||||
.br
|
||||
E_corr_per_selectors(i) = -1000.d0 if it is not a double excitation
|
||||
.br
|
||||
coef_hf_selector = coefficient of the Hartree Fock determinant in the selectors determinants
|
||||
|
||||
`double_index_selectors <http://github.com/LCPQ/quantum_package/tree/master/src/Selectors_full/e_corr_selectors.irp.f#L4>`_
|
||||
degree of excitation respect to Hartree Fock for the wave function
|
||||
.br
|
||||
for the all the selectors determinants
|
||||
.br
|
||||
double_index_selectors = list of the index of the double excitations
|
||||
.br
|
||||
n_double_selectors = number of double excitations in the selectors determinants
|
||||
|
||||
`e_corr_per_selectors <http://github.com/LCPQ/quantum_package/tree/master/src/Selectors_full/e_corr_selectors.irp.f#L28>`_
|
||||
energy of correlation per determinant respect to the Hartree Fock determinant
|
||||
.br
|
||||
for the all the double excitations in the selectors determinants
|
||||
.br
|
||||
E_corr_per_selectors(i) = <D_i|H|HF> * c(D_i)/c(HF) if |D_i> is a double excitation
|
||||
.br
|
||||
E_corr_per_selectors(i) = -1000.d0 if it is not a double excitation
|
||||
.br
|
||||
coef_hf_selector = coefficient of the Hartree Fock determinant in the selectors determinants
|
||||
|
||||
`exc_degree_per_selectors <http://github.com/LCPQ/quantum_package/tree/master/src/Selectors_full/e_corr_selectors.irp.f#L3>`_
|
||||
degree of excitation respect to Hartree Fock for the wave function
|
||||
.br
|
||||
for the all the selectors determinants
|
||||
.br
|
||||
double_index_selectors = list of the index of the double excitations
|
||||
.br
|
||||
n_double_selectors = number of double excitations in the selectors determinants
|
||||
|
||||
`n_double_selectors <http://github.com/LCPQ/quantum_package/tree/master/src/Selectors_full/e_corr_selectors.irp.f#L5>`_
|
||||
degree of excitation respect to Hartree Fock for the wave function
|
||||
.br
|
||||
for the all the selectors determinants
|
||||
.br
|
||||
double_index_selectors = list of the index of the double excitations
|
||||
.br
|
||||
n_double_selectors = number of double excitations in the selectors determinants
|
||||
|
||||
`n_det_selectors <http://github.com/LCPQ/quantum_package/tree/master/src/Selectors_full/selectors.irp.f#L26>`_
|
||||
For Single reference wave functions, the number of selectors is 1 : the
|
||||
Hartree-Fock determinant
|
||||
|
||||
`psi_selectors <http://github.com/LCPQ/quantum_package/tree/master/src/Selectors_full/selectors.irp.f#L48>`_
|
||||
Determinants on which we apply <i|H|psi> for perturbation.
|
||||
|
||||
`psi_selectors_coef <http://github.com/LCPQ/quantum_package/tree/master/src/Selectors_full/selectors.irp.f#L49>`_
|
||||
Determinants on which we apply <i|H|psi> for perturbation.
|
||||
|
||||
`psi_selectors_size <http://github.com/LCPQ/quantum_package/tree/master/src/Selectors_full/selectors.irp.f#L21>`_
|
||||
Undocumented
|
||||
|
||||
`threshold_selectors <http://github.com/LCPQ/quantum_package/tree/master/src/Selectors_full/selectors.irp.f#L3>`_
|
||||
Percentage of the norm of the state-averaged wave function to
|
||||
consider for the selectors
|
||||
|
||||
|
||||
|
||||
Needed Modules
|
||||
==============
|
||||
|
||||
.. Do not edit this section. It was auto-generated from the
|
||||
.. NEEDED_MODULES file.
|
||||
|
||||
* `AOs <http://github.com/LCPQ/quantum_package/tree/master/src/AOs>`_
|
||||
* `BiInts <http://github.com/LCPQ/quantum_package/tree/master/src/BiInts>`_
|
||||
* `Bitmask <http://github.com/LCPQ/quantum_package/tree/master/src/Bitmask>`_
|
||||
* `Dets <http://github.com/LCPQ/quantum_package/tree/master/src/Dets>`_
|
||||
* `Electrons <http://github.com/LCPQ/quantum_package/tree/master/src/Electrons>`_
|
||||
* `Ezfio_files <http://github.com/LCPQ/quantum_package/tree/master/src/Ezfio_files>`_
|
||||
* `Hartree_Fock <http://github.com/LCPQ/quantum_package/tree/master/src/Hartree_Fock>`_
|
||||
* `MonoInts <http://github.com/LCPQ/quantum_package/tree/master/src/MonoInts>`_
|
||||
* `MOs <http://github.com/LCPQ/quantum_package/tree/master/src/MOs>`_
|
||||
* `Nuclei <http://github.com/LCPQ/quantum_package/tree/master/src/Nuclei>`_
|
||||
* `Output <http://github.com/LCPQ/quantum_package/tree/master/src/Output>`_
|
||||
* `Utils <http://github.com/LCPQ/quantum_package/tree/master/src/Utils>`_
|
||||
|
||||
|
@ -19,6 +19,9 @@ Documentation
|
||||
For Single reference wave functions, the generator is the
|
||||
Hartree-Fock determinant
|
||||
|
||||
`select_max <http://github.com/LCPQ/quantum_package/tree/master/src/SingleRefMethod/generators.irp.f#L43>`_
|
||||
Memo to skip useless selectors
|
||||
|
||||
|
||||
|
||||
Needed Modules
|
||||
|
@ -28,6 +28,7 @@ BEGIN_PROVIDER [ integer(bit_kind), psi_generators, (N_int,2,psi_det_size) ]
|
||||
call get_excitation_degree(HF_bitmask,psi_det(1,1,j),degree,N_int)
|
||||
if (degree == 0) then
|
||||
k = j
|
||||
exit
|
||||
endif
|
||||
end do
|
||||
|
||||
|
@ -48,7 +48,6 @@ subroutine ortho_lowdin(overlap,LDA,N,C,LDC,m)
|
||||
stop
|
||||
endif
|
||||
|
||||
|
||||
!$OMP PARALLEL DEFAULT(NONE) &
|
||||
!$OMP SHARED(S_half,U,D,Vt,n,C,m) &
|
||||
!$OMP PRIVATE(i,j,k)
|
||||
@ -178,7 +177,7 @@ subroutine apply_rotation(A,LDA,R,LDR,B,LDB,m,n)
|
||||
call dgemm('N','N',m,n,n,1.d0,A,LDA,R,LDR,0.d0,B,LDB)
|
||||
end
|
||||
|
||||
subroutine lapack_diag(eigvalues,eigvectors,H,nmax,n)
|
||||
subroutine lapack_diagd(eigvalues,eigvectors,H,nmax,n)
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! Diagonalize matrix H
|
||||
@ -244,3 +243,122 @@ subroutine lapack_diag(eigvalues,eigvectors,H,nmax,n)
|
||||
enddo
|
||||
deallocate(A,eigenvalues)
|
||||
end
|
||||
|
||||
subroutine lapack_diag(eigvalues,eigvectors,H,nmax,n)
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! Diagonalize matrix H
|
||||
!
|
||||
! H is untouched between input and ouptut
|
||||
!
|
||||
! eigevalues(i) = ith lowest eigenvalue of the H matrix
|
||||
!
|
||||
! eigvectors(i,j) = <i|psi_j> where i is the basis function and psi_j is the j th eigenvector
|
||||
!
|
||||
END_DOC
|
||||
integer, intent(in) :: n,nmax
|
||||
double precision, intent(out) :: eigvectors(nmax,n)
|
||||
double precision, intent(out) :: eigvalues(n)
|
||||
double precision, intent(in) :: H(nmax,n)
|
||||
double precision,allocatable :: eigenvalues(:)
|
||||
double precision,allocatable :: work(:)
|
||||
double precision,allocatable :: A(:,:)
|
||||
integer :: lwork, info, i,j,l,k, liwork
|
||||
|
||||
allocate(A(nmax,n),eigenvalues(n))
|
||||
! print*,'Diagonalization by jacobi'
|
||||
! print*,'n = ',n
|
||||
|
||||
A=H
|
||||
lwork = 2*n*n + 6*n+ 1
|
||||
allocate (work(lwork))
|
||||
|
||||
lwork = -1
|
||||
call DSYEV( 'V', 'U', n, A, nmax, eigenvalues, work, lwork, &
|
||||
info )
|
||||
if (info < 0) then
|
||||
print *, irp_here, ': DSYEV: the ',-info,'-th argument had an illegal value'
|
||||
stop 2
|
||||
endif
|
||||
lwork = int( work( 1 ) )
|
||||
deallocate (work)
|
||||
|
||||
allocate (work(lwork))
|
||||
call DSYEV( 'V', 'U', n, A, nmax, eigenvalues, work, lwork, &
|
||||
info )
|
||||
deallocate(work)
|
||||
|
||||
if (info < 0) then
|
||||
print *, irp_here, ': DSYEV: the ',-info,'-th argument had an illegal value'
|
||||
stop 2
|
||||
else if( info > 0 ) then
|
||||
write(*,*)'DSYEV Failed'
|
||||
stop 1
|
||||
end if
|
||||
|
||||
eigvectors = 0.d0
|
||||
eigvalues = 0.d0
|
||||
do j = 1, n
|
||||
eigvalues(j) = eigenvalues(j)
|
||||
do i = 1, n
|
||||
eigvectors(i,j) = A(i,j)
|
||||
enddo
|
||||
enddo
|
||||
deallocate(A,eigenvalues)
|
||||
end
|
||||
|
||||
subroutine lapack_partial_diag(eigvalues,eigvectors,H,nmax,n,n_st)
|
||||
implicit none
|
||||
BEGIN_DOC
|
||||
! Diagonalize matrix H
|
||||
!
|
||||
! H is untouched between input and ouptut
|
||||
!
|
||||
! eigevalues(i) = ith lowest eigenvalue of the H matrix
|
||||
!
|
||||
! eigvectors(i,j) = <i|psi_j> where i is the basis function and psi_j is the j th eigenvector
|
||||
!
|
||||
END_DOC
|
||||
integer, intent(in) :: n,nmax,n_st
|
||||
double precision, intent(out) :: eigvectors(nmax,n)
|
||||
double precision, intent(out) :: eigvalues(n)
|
||||
double precision, intent(in) :: H(nmax,n)
|
||||
double precision,allocatable :: work(:)
|
||||
integer ,allocatable :: iwork(:), isuppz(:)
|
||||
double precision,allocatable :: A(:,:)
|
||||
integer :: lwork, info, i,j,l,k,m, liwork
|
||||
|
||||
allocate(A(nmax,n))
|
||||
|
||||
A=H
|
||||
lwork = 2*n*n + 6*n+ 1
|
||||
liwork = 5*n + 3
|
||||
allocate (work(lwork),iwork(liwork),isuppz(2*N_st))
|
||||
|
||||
lwork = -1
|
||||
liwork = -1
|
||||
call DSYEVR( 'V', 'I', 'U', n, A, nmax, 0.d0, 0.d0, 1, n_st, 1.d-10, m, eigvalues, eigvectors, nmax, isuppz, work, lwork, &
|
||||
iwork, liwork, info )
|
||||
if (info < 0) then
|
||||
print *, irp_here, ': DSYEVR: the ',-info,'-th argument had an illegal value'
|
||||
stop 2
|
||||
endif
|
||||
lwork = int( work( 1 ) )
|
||||
liwork = iwork(1)
|
||||
deallocate (work,iwork)
|
||||
|
||||
allocate (work(lwork),iwork(liwork))
|
||||
call DSYEVR( 'V', 'I', 'U', n, A, nmax, 0.d0, 0.d0, 1, n_st, 1.d-10, m, eigvalues, eigvectors, nmax, isuppz, work, lwork, &
|
||||
iwork, liwork, info )
|
||||
deallocate(work,iwork)
|
||||
|
||||
if (info < 0) then
|
||||
print *, irp_here, ': DSYEVR: the ',-info,'-th argument had an illegal value'
|
||||
stop 2
|
||||
else if( info > 0 ) then
|
||||
write(*,*)'DSYEVR Failed'
|
||||
stop 1
|
||||
end if
|
||||
|
||||
deallocate(A)
|
||||
end
|
||||
|
@ -92,7 +92,7 @@ Documentation
|
||||
into
|
||||
fact_k (x-x_P)^iorder(1) (y-y_P)^iorder(2) (z-z_P)^iorder(3) exp(-p(r-P)^2)
|
||||
|
||||
`hermite <http://github.com/LCPQ/quantum_package/tree/master/src/Utils/integration.irp.f#L472>`_
|
||||
`hermite <http://github.com/LCPQ/quantum_package/tree/master/src/Utils/integration.irp.f#L477>`_
|
||||
Hermite polynomial
|
||||
|
||||
`multiply_poly <http://github.com/LCPQ/quantum_package/tree/master/src/Utils/integration.irp.f#L201>`_
|
||||
@ -108,10 +108,10 @@ Documentation
|
||||
\int_0^1 dx \exp(-p x^2) x^n
|
||||
.br
|
||||
|
||||
`rint1 <http://github.com/LCPQ/quantum_package/tree/master/src/Utils/integration.irp.f#L528>`_
|
||||
`rint1 <http://github.com/LCPQ/quantum_package/tree/master/src/Utils/integration.irp.f#L533>`_
|
||||
Standard version of rint
|
||||
|
||||
`rint_large_n <http://github.com/LCPQ/quantum_package/tree/master/src/Utils/integration.irp.f#L497>`_
|
||||
`rint_large_n <http://github.com/LCPQ/quantum_package/tree/master/src/Utils/integration.irp.f#L502>`_
|
||||
Version of rint for large values of n
|
||||
|
||||
`rint_sum <http://github.com/LCPQ/quantum_package/tree/master/src/Utils/integration.irp.f#L421>`_
|
||||
|
Loading…
Reference in New Issue
Block a user