import numpy as np from functools import reduce def memoize(f): memo = {} def helper(x): if x not in memo: memo[x] = f(x) return memo[x] return helper @memoize def idx2_tri(iijj): ''' iijj should be a 2-tuple return triangular compound index for (0-indexed counting) ''' ij1=min(iijj) ij2=max(iijj) return ij1+(ij2*(ij2+1))//2 # return ij1+(ij2*(ij2-1))//2 def pad(arr_in,outshape): arr_out = np.zeros(outshape,dtype=np.complex128) dataslice = tuple(slice(0,arr_in.shape[dim]) for dim in range(len(outshape))) arr_out[dataslice] = arr_in return arr_out def idx40(i,j,k,l): return idx2_tri((idx2_tri((i,k)),idx2_tri((j,l)))) def idx4(i,j,k,l): return idx2_tri((idx2_tri((i-1,k-1)),idx2_tri((j-1,l-1))))+1 def stri4(i,j,k,l): return (4*'{:5d}').format(i,j,k,l) def stri4z(i,j,k,l,zr,zi): return (4*'{:5d}'+2*'{:25.16e}').format(i,j,k,l,zr,zi) def stri2z(i,j,zr,zi): return (2*'{:5d}'+2*'{:25.16e}').format(i,j,zr,zi) def strijklikjli4z(i,j,k,l,zr,zi): return ('{:10d}'+ 2*'{:8d}'+4*'{:5d}'+2*'{:25.16e}').format(idx4(i,j,k,l),idx2_tri((i-1,k-1))+1,idx2_tri((j-1,l-1))+1,i,j,k,l,zr,zi) def makesq(vlist,n1,n2): ''' make hermitian matrices of size (n2 x n2) from from lower triangles vlist is n1 lower triangles in flattened form given: ([a,b,c,d,e,f,g,h,i,j,k,l,m,n,o,p,q,r,s,t],2,4) output a 2x4x4 array, where each 4x4 is the square constructed from the lower triangle [ [ [a b* d* g*] [b c e* h*] [d e f i*] [g h i j ] ], [ [k l* n* q*] [l m o* r*] [n o p s*] [q r s t ] ] ] ''' out=np.zeros([n1,n2,n2],dtype=np.complex128) n0 = vlist.shape[0] lmask=np.tri(n2,dtype=bool) for i in range(n0): out[i][lmask] = vlist[i].conj() out2=out.transpose([0,2,1]) for i in range(n0): out2[i][lmask] = vlist[i] return out2 def makesq3(vlist,n2): ''' make hermitian matrices of size (n2 x n2) from from lower triangles vlist is n1 lower triangles in flattened form given: ([a,b,c,d,e,f,g,h,i,j,k,l,m,n,o,p,q,r,s,t],2,4) output a 2x4x4 array, where each 4x4 is the square constructed from the lower triangle [ [ [a b* d* g*] [b c e* h*] [d e f i*] [g h i j ] ], [ [k l* n* q*] [l m o* r*] [n o p s*] [q r s t ] ] ] ''' n0 = vlist.shape[0] out=np.zeros([n0,n2,n2],dtype=np.complex128) lmask=np.tri(n2,dtype=bool) for i in range(n0): out[i][lmask] = vlist[i].conj() out2=out.transpose([0,2,1]) for i in range(n0): out2[i][lmask] = vlist[i] return out2 def makesq2(vlist,n1,n2): out=np.zeros([n1,n2,n2],dtype=np.complex128) lmask=np.tri(n2,dtype=bool) tmp=np.zeros([n2,n2],dtype=np.complex128) tmp2=np.zeros([n2,n2],dtype=np.complex128) for i in range(n1): tmp[lmask] = vlist[i].conj() tmp2=tmp.T tmp2[lmask] = vlist[i] out[i] = tmp2.copy() return out def get_phase(cell, kpts, kmesh=None): ''' The unitary transformation that transforms the supercell basis k-mesh adapted basis. ''' from pyscf.pbc import tools from pyscf import lib latt_vec = cell.lattice_vectors() if kmesh is None: # Guess kmesh scaled_k = cell.get_scaled_kpts(kpts).round(8) kmesh = (len(np.unique(scaled_k[:,0])), len(np.unique(scaled_k[:,1])), len(np.unique(scaled_k[:,2]))) R_rel_a = np.arange(kmesh[0]) R_rel_b = np.arange(kmesh[1]) R_rel_c = np.arange(kmesh[2]) R_vec_rel = lib.cartesian_prod((R_rel_a, R_rel_b, R_rel_c)) R_vec_abs = np.einsum('nu, uv -> nv', R_vec_rel, latt_vec) NR = len(R_vec_abs) phase = np.exp(1j*np.einsum('Ru, ku -> Rk', R_vec_abs, kpts)) phase /= np.sqrt(NR) # normalization in supercell # R_rel_mesh has to be construct exactly same to the Ts in super_cell function scell = tools.super_cell(cell, kmesh) return scell, phase def mo_k2gamma(cell, mo_energy, mo_coeff, kpts, kmesh=None): ''' Transform MOs in Kpoints to the equivalents supercell ''' from pyscf import lib import scipy.linalg as la scell, phase = get_phase(cell, kpts, kmesh) E_g = np.hstack(mo_energy) C_k = np.asarray(mo_coeff) Nk, Nao, Nmo = C_k.shape NR = phase.shape[0] # Transform AO indices C_gamma = np.einsum('Rk, kum -> Rukm', phase, C_k) C_gamma = C_gamma.reshape(Nao*NR, Nk*Nmo) E_sort_idx = np.argsort(E_g) E_g = E_g[E_sort_idx] C_gamma = C_gamma[:,E_sort_idx] s = scell.pbc_intor('int1e_ovlp') assert(abs(reduce(np.dot, (C_gamma.conj().T, s, C_gamma)) - np.eye(Nmo*Nk)).max() < 1e-7) # Transform MO indices E_k_degen = abs(E_g[1:] - E_g[:-1]).max() < 1e-5 if np.any(E_k_degen): degen_mask = np.append(False, E_k_degen) | np.append(E_k_degen, False) shift = min(E_g[degen_mask]) - .1 f = np.dot(C_gamma[:,degen_mask] * (E_g[degen_mask] - shift), C_gamma[:,degen_mask].conj().T) assert(abs(f.imag).max() < 1e-5) e, na_orb = la.eigh(f.real, s, type=2) C_gamma[:,degen_mask] = na_orb[:, e>0] if abs(C_gamma.imag).max() < 1e-7: print('!Warning Some complexe pollutions in MOs are present') C_gamma = C_gamma.real if abs(reduce(np.dot, (C_gamma.conj().T, s, C_gamma)) - np.eye(Nmo*Nk)).max() < 1e-7: print('!Warning Some complexe pollutions in MOs are present') s_k = cell.pbc_intor('int1e_ovlp', kpts=kpts) # overlap between k-point unitcell and gamma-point supercell s_k_g = np.einsum('kuv,Rk->kuRv', s_k, phase.conj()).reshape(Nk,Nao,NR*Nao) # The unitary transformation from k-adapted orbitals to gamma-point orbitals mo_phase = lib.einsum('kum,kuv,vi->kmi', C_k.conj(), s_k_g, C_gamma) return mo_phase def qp2rename(): import shutil qp2names={} qp2names['mo_coef_complex'] = 'C.qp' qp2names['bielec_ao_complex'] = 'W.qp' qp2names['kinetic_ao_complex'] = 'T.qp' qp2names['ne_ao_complex'] = 'V.qp' qp2names['overlap_ao_complex'] = 'S.qp' for old,new in qp2names.items(): shutil.move(old,new) shutil.copy('e_nuc','E.qp') def print_mo_bi(mf,kconserv=None,outfilename='W.mo.qp',cas_idx=None,bielec_int_threshold = 1E-8): cell = mf.cell kpts = mf.kpts #nao = mf.cell.nao #Nk = kpts.shape[0] mo_coeff = mf.mo_coeff # Mo_coeff actif mo_k = np.array([c[:,cas_idx] for c in mo_coeff] if cas_idx is not None else mo_coeff) Nk, nao, nmo = mo_k.shape if (kconserv is None): from pyscf.pbc import tools kconserv = tools.get_kconserv(cell, kpts) with open(outfilename,'w') as outfile: for d, kd in enumerate(kpts): for c, kc in enumerate(kpts): if c > d: break #idx2_cd = idx2_tri((c,d)) for b, kb in enumerate(kpts): if b > d: break a = kconserv[b,c,d] if a > d: continue #if idx2_tri((a,b)) > idx2_cd: continue #if ((c==d) and (a>b)): continue ka = kpts[a] eri_4d_mo_kpt = mf.with_df.ao2mo([mo_k[a], mo_k[b], mo_k[c], mo_k[d]], [ka,kb,kc,kd],compact=False).reshape((nmo,)*4) eri_4d_mo_kpt *= 1./Nk for l in range(nmo): ll=l+d*nmo for j in range(nmo): jj=j+c*nmo if jj>ll: break idx2_jjll = idx2_tri((jj,ll)) for k in range(nmo): kk=k+b*nmo if kk>ll: break for i in range(nmo): ii=i+a*nmo if idx2_tri((ii,kk)) > idx2_jjll: break if ((jj==ll) and (ii>kk)): break v=eri_4d_mo_kpt[i,k,j,l] if (abs(v) > bielec_int_threshold): outfile.write(stri4z(ii+1,jj+1,kk+1,ll+1, v.real,v.imag)+'\n') def print_ao_bi(mf,kconserv=None,outfilename='W.ao.qp',bielec_int_threshold = 1E-8): cell = mf.cell kpts = mf.kpts nao = mf.cell.nao Nk = kpts.shape[0] if (kconserv is None): from pyscf.pbc.tools import get_kconserv kconserv = get_kconserv(cell, kpts) with open(outfilename,'w') as outfile: for d, kd in enumerate(kpts): for c, kc in enumerate(kpts): if c > d: break #idx2_cd = idx2_tri((c,d)) for b, kb in enumerate(kpts): if b > d: break a = kconserv[b,c,d] if a > d: continue #if idx2_tri((a,b)) > idx2_cd: continue #if ((c==d) and (a>b)): continue ka = kpts[a] eri_4d_ao_kpt = mf.with_df.get_ao_eri(kpts=[ka,kb,kc,kd], compact=False).reshape((nao,)*4) eri_4d_ao_kpt *= 1./Nk for l in range(nao): ll=l+d*nao for j in range(nao): jj=j+c*nao if jj>ll: break idx2_jjll = idx2_tri((jj,ll)) for k in range(nao): kk=k+b*nao if kk>ll: break for i in range(nao): ii=i+a*nao if idx2_tri((ii,kk)) > idx2_jjll: break if ((jj==ll) and (ii>kk)): break v=eri_4d_ao_kpt[i,k,j,l] if (abs(v) > bielec_int_threshold): outfile.write(stri4z(ii+1,jj+1,kk+1,ll+1, v.real,v.imag)+'\n') def print_kcon_chem_to_phys(kcon,fname): ''' input: kconserv in chem notation kcon_c[a,b,c] = d where (ab|cd) is allowed by symmetry output: kconserv in phys notation kcon_p[i,j,k] = l where is allowed by symmetry (printed to file) ''' Nk,n2,n3 = kcon.shape if (n2!=n3 or Nk!=n2): raise Exception('print_kcon_chem_to_phys called with non-cubic array') with open(fname,'w') as outfile: for a in range(Nk): for b in range(Nk): for c in range(Nk): d = kcon[a,b,c] outfile.write(stri4(a+1,c+1,b+1,d+1)+'\n') def print_kpts_unblocked(ints_k,outfilename,thresh): ''' for ints_k of shape (Nk,n1,n2), print the elements of the corresponding block-diagonal matrix of shape (Nk*n1,Nk*n2) in file ''' Nk,n1,n2 = ints_k.shape with open(outfilename,'w') as outfile: for ik in range(Nk): shift1 = ik*n1+1 shift2 = ik*n2+1 for i1 in range(n1): for i2 in range(n2): int_ij = ints_k[ik,i1,i2] if abs(int_ij) > thresh: outfile.write(stri2z(i1+shift1, i2+shift2, int_ij.real, int_ij.imag)+'\n') return def print_kpts_unblocked_upper(ints_k,outfilename,thresh): ''' for hermitian ints_k of shape (Nk,n1,n1), print the elements of the corresponding block-diagonal matrix of shape (Nk*n1,Nk*n1) in file (only upper triangle is printed) ''' Nk,n1,n2 = ints_k.shape if (n1!=n2): raise Exception('print_kpts_unblocked_upper called with non-square matrix') with open(outfilename,'w') as outfile: for ik in range(Nk): shift = ik*n1+1 for i1 in range(n1): for i2 in range(i1,n1): int_ij = ints_k[ik,i1,i2] if abs(int_ij) > thresh: outfile.write(stri2z(i1+shift, i2+shift, int_ij.real, int_ij.imag)+'\n') return def get_kin_ao(mf): nao = mf.cell.nao_nr() Nk = len(mf.kpts) return np.reshape(mf.cell.pbc_intor('int1e_kin',1,1,kpts=mf.kpts),(Nk,nao,nao)) def get_ovlp_ao(mf): nao = mf.cell.nao_nr() Nk = len(mf.kpts) return np.reshape(mf.get_ovlp(cell=mf.cell,kpts=mf.kpts),(Nk,nao,nao)) def get_pot_ao(mf): nao = mf.cell.nao_nr() Nk = len(mf.kpts) if mf.cell.pseudo: v_kpts_ao = np.reshape(mf.with_df.get_pp(kpts=mf.kpts),(Nk,nao,nao)) else: v_kpts_ao = np.reshape(mf.with_df.get_nuc(kpts=mf.kpts),(Nk,nao,nao)) if len(mf.cell._ecpbas) > 0: from pyscf.pbc.gto import ecp v_kpts_ao += np.reshape(ecp.ecp_int(mf.cell, mf.kpts),(Nk,nao,nao)) return v_kpts_ao def ao_to_mo_1e(ao_kpts,mo_coef): return np.einsum('kim,kij,kjn->kmn',mo_coef.conj(),ao_kpts,mo_coef) def get_j3ao_old(fname,nao,Nk): ''' returns list of Nk_pair arrays of shape (naux,nao,nao) if naux is the same for each pair, returns numpy array if naux is not the same for each pair, returns array of arrays ''' import h5py with h5py.File(fname,'r') as intfile: j3c = intfile.get('j3c') j3ckeys = list(j3c.keys()) j3ckeys.sort(key=lambda strkey:int(strkey)) # in new(?) version of PySCF, there is an extra layer of groups before the datasets # datasets used to be [/j3c/0, /j3c/1, /j3c/2, ...] # datasets now are [/j3c/0/0, /j3c/1/0, /j3c/2/0, ...] j3clist = [j3c.get(i+'/0') for i in j3ckeys] #if j3clist==[None]*len(j3clist): if not(any(j3clist)): # if using older version, stop before last level j3clist = [j3c.get(i) for i in j3ckeys] naosq = nao*nao naotri = (nao*(nao+1))//2 nkinvsq = 1./np.sqrt(Nk) # dimensions are (kikj,iaux,jao,kao), where kikj is compound index of kpts i and j # output dimensions should be reversed (nao, nao, naux, nkptpairs) return np.array([(i.value.reshape([-1,nao,nao]) if (i.shape[1] == naosq) else makesq3(i.value,nao)) * nkinvsq for i in j3clist]) def get_j3ao(fname,nao,Nk): ''' returns padded df AO array fills in zeros when functions are dropped due to linear dependency last AO index corresponds to smallest kpt index? (k, mu, i, j) where i.kpt >= j.kpt ''' import h5py with h5py.File(fname,'r') as intfile: j3c = intfile.get('j3c') j3ckeys = list(j3c.keys()) nkpairs = len(j3ckeys) # get num order instead of lex order j3ckeys.sort(key=lambda strkey:int(strkey)) # in new(?) version of PySCF, there is an extra layer of groups before the datasets # datasets used to be [/j3c/0, /j3c/1, /j3c/2, ...] # datasets now are [/j3c/0/0, /j3c/1/0, /j3c/2/0, ...] keysub = '/0' if bool(j3c.get('0/0',getclass=True)) else '' naux = max(map(lambda k: j3c[k+keysub].shape[0],j3c.keys())) naosq = nao*nao naotri = (nao*(nao+1))//2 nkinvsq = 1./np.sqrt(Nk) j3arr = np.zeros((nkpairs,naux,nao,nao),dtype=np.complex128) for i,kpair in enumerate(j3ckeys): iaux,dim2 = j3c[kpair+keysub].shape if (dim2==naosq): j3arr[i,:iaux,:,:] = j3c[kpair+keysub][()].reshape([iaux,nao,nao]) * nkinvsq #j3arr[i,:iaux,:,:] = j3c[kpair+keysub][()].reshape([iaux,nao,nao]).transpose((0,2,1)) * nkinvsq else: j3arr[i,:iaux,:,:] = makesq3(j3c[kpair+keysub][()],nao) * nkinvsq #j3arr[i,:iaux,:,:] = makesq3(j3c[kpair+keysub][()].conj(),nao) * nkinvsq return j3arr def get_j3ao_new(fname,nao,Nk): ''' returns padded df AO array fills in zeros when functions are dropped due to linear dependency last AO index corresponds to largest kpt index? (k, mu, j, i) where i.kpt >= j.kpt ''' import h5py with h5py.File(fname,'r') as intfile: j3c = intfile.get('j3c') j3ckeys = list(j3c.keys()) nkpairs = len(j3ckeys) # get num order instead of lex order j3ckeys.sort(key=lambda strkey:int(strkey)) # in new(?) version of PySCF, there is an extra layer of groups before the datasets # datasets used to be [/j3c/0, /j3c/1, /j3c/2, ...] # datasets now are [/j3c/0/0, /j3c/1/0, /j3c/2/0, ...] keysub = '/0' if bool(j3c.get('0/0',getclass=True)) else '' naux = max(map(lambda k: j3c[k+keysub].shape[0],j3c.keys())) naosq = nao*nao naotri = (nao*(nao+1))//2 nkinvsq = 1./np.sqrt(Nk) j3arr = np.zeros((nkpairs,naux,nao,nao),dtype=np.complex128) for i,kpair in enumerate(j3ckeys): iaux,dim2 = j3c[kpair+keysub].shape if (dim2==naosq): j3arr[i,:iaux,:,:] = j3c[kpair+keysub][()].reshape([iaux,nao,nao]).transpose((0,2,1)) * nkinvsq else: j3arr[i,:iaux,:,:] = makesq3(j3c[kpair+keysub][()].conj(),nao) * nkinvsq return j3arr def print_df(j3arr,fname,thresh): with open(fname,'w') as outfile: for k,kpt_pair in enumerate(j3arr): for iaux,dfbasfunc in enumerate(kpt_pair): for i,i0 in enumerate(dfbasfunc): for j,v in enumerate(i0): if (abs(v) > thresh): outfile.write(stri4z(i+1,j+1,iaux+1,k+1,v.real,v.imag)+'\n') return def df_pad_ref_test(j3arr,nao,naux,nkpt_pairs): df_ao_tmp = np.zeros((nao,nao,naux,nkpt_pairs),dtype=np.complex128) for k,kpt_pair in enumerate(j3arr): for iaux,dfbasfunc in enumerate(kpt_pair): for i,i0 in enumerate(dfbasfunc): for j,v in enumerate(i0): df_ao_tmp[i,j,iaux,k]=v return df_ao_tmp def df_ao_to_mo(j3ao,mo_coef): from itertools import product Nk = mo_coef.shape[0] kpair_list = ((i,j,idx2_tri((i,j))) for (i,j) in product(range(Nk),repeat=2) if (i>=j)) return np.array([ np.einsum('mij,ik,jl->mkl',j3ao[kij],mo_coef[ki].conj(),mo_coef[kj]) for ki,kj,kij in kpair_list]) def df_ao_to_mo_new(j3ao,mo_coef): #TODO: fix this (C/F ordering, conj, transpose, view cmplx->float) from itertools import product Nk = mo_coef.shape[0] return np.array([ np.einsum('mji,ik,jl->mlk',j3ao[idx2_tri((ki,kj))],mo_coef[ki].conj(),mo_coef[kj]) for ki,kj in product(range(Nk),repeat=2) if (ki>=kj)],dtype=np.complex128) def df_ao_to_mo_test(j3ao,mo_coef): from itertools import product Nk = mo_coef.shape[0] return np.array([ np.einsum('mij,ik,jl->mkl',j3ao[idx2_tri((ki,kj))],mo_coef[ki].conj(),mo_coef[kj]) for ki,kj in product(range(Nk),repeat=2) if (ki>=kj)]) def pyscf2QP2_mo(cell,mf,kpts,kmesh=None,cas_idx=None, int_threshold = 1E-8,qph5path='qpdat.h5'): pyscf2QP2(cell,mf,kpts,kmesh,cas_idx,int_threshold,qph5path, print_ao_ints_df=False, print_mo_ints_df=True, print_ao_ints_mono=False, print_mo_ints_mono=True) return def pyscf2QP2(cell,mf, kpts, kmesh=None, cas_idx=None, int_threshold = 1E-8, qph5path = 'qpdat.h5', print_ao_ints_bi=False, print_mo_ints_bi=False, print_ao_ints_df=True, print_mo_ints_df=False, print_ao_ints_mono=True, print_mo_ints_mono=False, print_debug=False): ''' kpts = List of kpoints coordinates. Cannot be null, for gamma is other script kmesh = Mesh of kpoints (optional) cas_idx = List of active MOs. If not specified all MOs are actives int_threshold = The integral will be not printed in they are bellow that ''' # from pyscf.pbc import ao2mo from pyscf.pbc import tools import h5py # import scipy from scipy.linalg import block_diag mo_coef_threshold = int_threshold ovlp_threshold = int_threshold kin_threshold = int_threshold ne_threshold = int_threshold bielec_int_threshold = int_threshold thresh_mono = int_threshold # qph5path = 'qpdat.h5' # create hdf5 file, delete old data if exists with h5py.File(qph5path,'w') as qph5: qph5.create_group('nuclei') qph5.create_group('electrons') qph5.create_group('ao_basis') qph5.create_group('mo_basis') mo_coeff = mf.mo_coeff # Mo_coeff actif mo_k = np.array([c[:,cas_idx] for c in mo_coeff] if cas_idx is not None else mo_coeff) e_k = np.array([e[cas_idx] for e in mf.mo_energy] if cas_idx is not None else mf.mo_energy) Nk, nao, nmo = mo_k.shape print("n Kpts", Nk) print("n active Mos per kpt", nmo) print("n AOs per kpt", nao) ########################################## # # # Nuclei # # # ########################################## natom = cell.natm print('n_atom per kpt', natom) atom_xyz = mf.cell.atom_coords() if not(mf.cell.unit.startswith(('B','b','au','AU'))): from pyscf.data.nist import BOHR atom_xyz /= BOHR # always convert to au with h5py.File(qph5path,'a') as qph5: qph5['nuclei'].attrs['kpt_num']=Nk qph5['nuclei'].attrs['nucl_num']=natom qph5.create_dataset('nuclei/nucl_coord',data=atom_xyz) qph5.create_dataset('nuclei/nucl_charge',data=mf.cell.atom_charges()) strtype=h5py.special_dtype(vlen=str) atom_dset=qph5.create_dataset('nuclei/nucl_label',(natom,),dtype=strtype) for i in range(natom): atom_dset[i] = mf.cell.atom_pure_symbol(i) ########################################## # # # Basis # # # ########################################## # nucleus on which each AO is centered ao_nucl=[i[0] for i in mf.cell.ao_labels(fmt=False,base=1)] with h5py.File(qph5path,'a') as qph5: qph5['mo_basis'].attrs['mo_num']=Nk*nmo qph5['ao_basis'].attrs['ao_num']=Nk*nao qph5['ao_basis'].attrs['ao_basis']=mf.cell.basis qph5.create_dataset('ao_basis/ao_nucl',data=Nk*ao_nucl) ########################################## # # # Electrons # # # ########################################## nelec = cell.nelectron neleca,nelecb = cell.nelec print('num_elec per kpt', nelec) with h5py.File(qph5path,'a') as qph5: #in old version: param << nelec*Nk, nmo*Nk, natom*Nk qph5['electrons'].attrs['elec_alpha_num']=neleca*Nk qph5['electrons'].attrs['elec_beta_num']=nelecb*Nk ########################################## # # # Nuclear Repulsion # # # ########################################## #Total energy shift due to Ewald probe charge = -1/2 * Nelec*madelung/cell.vol = shift = tools.pbc.madelung(cell, kpts)*cell.nelectron * -.5 e_nuc = (cell.energy_nuc() + shift)*Nk print('nucl_repul', e_nuc) with h5py.File(qph5path,'a') as qph5: qph5['nuclei'].attrs['nuclear_repulsion']=e_nuc ########################################## # # # MO Coef # # # ########################################## with h5py.File(qph5path,'a') as qph5: # k,mo,ao(,2) mo_coef_f = np.array(mo_k.transpose((0,2,1)),order='c',dtype=np.complex128) mo_coef_blocked=block_diag(*mo_k) mo_coef_blocked_f = block_diag(*mo_coef_f) #qph5.create_dataset('mo_basis/mo_coef_real',data=mo_coef_blocked.real) #qph5.create_dataset('mo_basis/mo_coef_imag',data=mo_coef_blocked.imag) #qph5.create_dataset('mo_basis/mo_coef_kpts_real',data=mo_k.real) #qph5.create_dataset('mo_basis/mo_coef_kpts_imag',data=mo_k.imag) print(mo_coef_f.dtype) print(mo_coef_blocked_f.dtype) qph5.create_dataset('mo_basis/mo_coef_complex',data=mo_coef_blocked_f.view(dtype=np.float64).reshape((Nk*nmo,Nk*nao,2))) qph5.create_dataset('mo_basis/mo_coef_kpts',data=mo_coef_f.view(dtype=np.float64).reshape((Nk,nmo,nao,2))) if print_debug: print_kpts_unblocked(mo_k,'C.qp',mo_coef_threshold) ########################################## # # # Integrals Mono # # # ########################################## ne_ao = get_pot_ao(mf) kin_ao = get_kin_ao(mf) ovlp_ao = get_ovlp_ao(mf) if print_ao_ints_mono: with h5py.File(qph5path,'a') as qph5: kin_ao_blocked=block_diag(*kin_ao) ovlp_ao_blocked=block_diag(*ovlp_ao) ne_ao_blocked=block_diag(*ne_ao) kin_ao_f = np.array(kin_ao.transpose((0,2,1)),order='c',dtype=np.complex128) ovlp_ao_f = np.array(ovlp_ao.transpose((0,2,1)),order='c',dtype=np.complex128) ne_ao_f = np.array(ne_ao.transpose((0,2,1)),order='c',dtype=np.complex128) kin_ao_blocked_f = block_diag(*kin_ao_f) ovlp_ao_blocked_f = block_diag(*ovlp_ao_f) ne_ao_blocked_f = block_diag(*ne_ao_f) #qph5.create_dataset('ao_one_e_ints/ao_integrals_kinetic_real',data=kin_ao_blocked.real) #qph5.create_dataset('ao_one_e_ints/ao_integrals_kinetic_imag',data=kin_ao_blocked.imag) #qph5.create_dataset('ao_one_e_ints/ao_integrals_overlap_real',data=ovlp_ao_blocked.real) #qph5.create_dataset('ao_one_e_ints/ao_integrals_overlap_imag',data=ovlp_ao_blocked.imag) #qph5.create_dataset('ao_one_e_ints/ao_integrals_n_e_real', data=ne_ao_blocked.real) #qph5.create_dataset('ao_one_e_ints/ao_integrals_n_e_imag', data=ne_ao_blocked.imag) #qph5.create_dataset('ao_one_e_ints/ao_integrals_kinetic',data=kin_ao_blocked_f.view(dtype=np.float64).reshape((Nk*nao,Nk*nao,2))) #qph5.create_dataset('ao_one_e_ints/ao_integrals_overlap',data=ovlp_ao_blocked_f.view(dtype=np.float64).reshape((Nk*nao,Nk*nao,2))) #qph5.create_dataset('ao_one_e_ints/ao_integrals_n_e', data=ne_ao_blocked_f.view(dtype=np.float64).reshape((Nk*nao,Nk*nao,2))) qph5.create_dataset('ao_one_e_ints/ao_integrals_kinetic_kpts',data=kin_ao_f.view(dtype=np.float64).reshape((Nk,nao,nao,2))) qph5.create_dataset('ao_one_e_ints/ao_integrals_overlap_kpts',data=ovlp_ao_f.view(dtype=np.float64).reshape((Nk,nao,nao,2))) qph5.create_dataset('ao_one_e_ints/ao_integrals_n_e_kpts', data=ne_ao_f.view(dtype=np.float64).reshape((Nk,nao,nao,2))) if print_debug: for fname,ints in zip(('S.qp','V.qp','T.qp'), (ovlp_ao, ne_ao, kin_ao)): print_kpts_unblocked_upper(ints,fname,thresh_mono) if print_mo_ints_mono: kin_mo = ao_to_mo_1e(kin_ao,mo_k) ovlp_mo = ao_to_mo_1e(ovlp_ao,mo_k) ne_mo = ao_to_mo_1e(ne_ao,mo_k) kin_mo_blocked=block_diag(*kin_mo) ovlp_mo_blocked=block_diag(*ovlp_mo) ne_mo_blocked=block_diag(*ne_mo) with h5py.File(qph5path,'a') as qph5: kin_mo_f = np.array(kin_mo.transpose((0,2,1)),order='c',dtype=np.complex128) ovlp_mo_f = np.array(ovlp_mo.transpose((0,2,1)),order='c',dtype=np.complex128) ne_mo_f = np.array(ne_mo.transpose((0,2,1)),order='c',dtype=np.complex128) kin_mo_blocked_f = block_diag(*kin_mo_f) ovlp_mo_blocked_f = block_diag(*ovlp_mo_f) ne_mo_blocked_f = block_diag(*ne_mo_f) #qph5.create_dataset('mo_one_e_ints/mo_integrals_kinetic_real',data=kin_mo_blocked.real) #qph5.create_dataset('mo_one_e_ints/mo_integrals_kinetic_imag',data=kin_mo_blocked.imag) #qph5.create_dataset('mo_one_e_ints/mo_integrals_overlap_real',data=ovlp_mo_blocked.real) #qph5.create_dataset('mo_one_e_ints/mo_integrals_overlap_imag',data=ovlp_mo_blocked.imag) #qph5.create_dataset('mo_one_e_ints/mo_integrals_n_e_real', data=ne_mo_blocked.real) #qph5.create_dataset('mo_one_e_ints/mo_integrals_n_e_imag', data=ne_mo_blocked.imag) #qph5.create_dataset('mo_one_e_ints/mo_integrals_kinetic',data=kin_mo_blocked_f.view(dtype=np.float64).reshape((Nk*nmo,Nk*nmo,2))) #qph5.create_dataset('mo_one_e_ints/mo_integrals_overlap',data=ovlp_mo_blocked_f.view(dtype=np.float64).reshape((Nk*nmo,Nk*nmo,2))) #qph5.create_dataset('mo_one_e_ints/mo_integrals_n_e', data=ne_mo_blocked_f.view(dtype=np.float64).reshape((Nk*nmo,Nk*nmo,2))) qph5.create_dataset('mo_one_e_ints/mo_integrals_kinetic_kpts',data=kin_mo_f.view(dtype=np.float64).reshape((Nk,nmo,nmo,2))) qph5.create_dataset('mo_one_e_ints/mo_integrals_overlap_kpts',data=ovlp_mo_f.view(dtype=np.float64).reshape((Nk,nmo,nmo,2))) qph5.create_dataset('mo_one_e_ints/mo_integrals_n_e_kpts', data=ne_mo_f.view(dtype=np.float64).reshape((Nk,nmo,nmo,2))) if print_debug: for fname,ints in zip(('S.mo.qp','V.mo.qp','T.mo.qp'), (ovlp_mo, ne_mo, kin_mo)): print_kpts_unblocked_upper(ints,fname,thresh_mono) ########################################## # # # k-points # # # ########################################## kconserv = tools.get_kconserv(cell, kpts) with h5py.File(qph5path,'a') as qph5: kcon_f_phys = np.array(kconserv.transpose((1,2,0)),order='c') qph5.create_dataset('nuclei/kconserv',data=kcon_f_phys+1) if print_debug: print_kcon_chem_to_phys(kconserv,'K.qp') ########################################## # # # Integrals Bi # # # ########################################## j3arr = get_j3ao(mf.with_df._cderi,nao,Nk) # test? nkpt_pairs should be (Nk*(Nk+1))//2 nkpt_pairs, naux, _, _ = j3arr.shape print("n df fitting functions", naux) with h5py.File(qph5path,'a') as qph5: qph5.create_group('ao_two_e_ints') qph5['ao_two_e_ints'].attrs['df_num']=naux j3ao_new = get_j3ao_new(mf.with_df._cderi,nao,Nk) if print_ao_ints_df: if print_debug: print_df(j3arr,'D.qp',bielec_int_threshold) with h5py.File(qph5path,'a') as qph5: #qph5.create_dataset('ao_two_e_ints/df_ao_integrals_real',data=j3arr.transpose((2,3,1,0)).real) #qph5.create_dataset('ao_two_e_ints/df_ao_integrals_imag',data=j3arr.transpose((2,3,1,0)).imag) qph5.create_dataset('ao_two_e_ints/df_ao_integrals',data=j3ao_new.view(dtype=np.float64).reshape((nkpt_pairs,naux,nao,nao,2))) if print_mo_ints_df: j3mo = df_ao_to_mo(j3arr,mo_k) j3mo_new = df_ao_to_mo_new(j3ao_new,mo_k) if print_debug: print_df(j3mo,'D.mo.qp',bielec_int_threshold) with h5py.File(qph5path,'a') as qph5: #qph5.create_dataset('mo_two_e_ints/df_mo_integrals_real',data=j3mo.transpose((2,3,1,0)).real) #qph5.create_dataset('mo_two_e_ints/df_mo_integrals_imag',data=j3mo.transpose((2,3,1,0)).imag) qph5.create_dataset('mo_two_e_ints/df_mo_integrals',data=j3mo_new.view(dtype=np.float64).reshape((nkpt_pairs,naux,nmo,nmo,2))) if (print_ao_ints_bi): print_ao_bi(mf,kconserv,'W.qp',bielec_int_threshold) if (print_mo_ints_bi): print_mo_bi(mf,kconserv,'W.mo.qp',cas_idx,bielec_int_threshold) return