Source code for pyscf.grad.tdrks

#!/usr/bin/env python
# Copyright 2014-2019 The PySCF Developers. All Rights Reserved.
#
# Licensed under the Apache License, Version 2.0 (the "License");
# you may not use this file except in compliance with the License.
# You may obtain a copy of the License at
#
#     http://www.apache.org/licenses/LICENSE-2.0
#
# Unless required by applicable law or agreed to in writing, software
# distributed under the License is distributed on an "AS IS" BASIS,
# WITHOUT WARRANTIES OR CONDITIONS OF ANY KIND, either express or implied.
# See the License for the specific language governing permissions and
# limitations under the License.
#
# Author: Qiming Sun <osirpt.sun@gmail.com>
#
# Ref:
# J. Chem. Phys. 117, 7433
#


from functools import reduce
import numpy
from pyscf import lib
from pyscf.lib import logger
from pyscf.dft import rks
from pyscf.dft import numint
from pyscf.scf import cphf
from pyscf.grad import rks as rks_grad
from pyscf.grad import tdrhf


#
# Given Y = 0, TDDFT gradients (XAX+XBY+YBX+YAY)^1 turn to TDA gradients (XAX)^1
#
[docs] def grad_elec(td_grad, x_y, singlet=True, atmlst=None, max_memory=2000, verbose=logger.INFO): ''' Electronic part of TDA, TDDFT nuclear gradients Args: td_grad : grad.tdrhf.Gradients or grad.tdrks.Gradients object. x_y : a two-element list of numpy arrays TDDFT X and Y amplitudes. If Y is set to 0, this function computes TDA energy gradients. ''' log = logger.new_logger(td_grad, verbose) time0 = logger.process_clock(), logger.perf_counter() mol = td_grad.mol mf = td_grad.base._scf mo_coeff = mf.mo_coeff mo_energy = mf.mo_energy mo_occ = mf.mo_occ nao, nmo = mo_coeff.shape nocc = (mo_occ>0).sum() nvir = nmo - nocc x, y = x_y xpy = (x+y).reshape(nocc,nvir).T xmy = (x-y).reshape(nocc,nvir).T orbv = mo_coeff[:,nocc:] orbo = mo_coeff[:,:nocc] dvv = numpy.einsum('ai,bi->ab', xpy, xpy) + numpy.einsum('ai,bi->ab', xmy, xmy) doo =-numpy.einsum('ai,aj->ij', xpy, xpy) - numpy.einsum('ai,aj->ij', xmy, xmy) dmxpy = reduce(numpy.dot, (orbv, xpy, orbo.T)) dmxmy = reduce(numpy.dot, (orbv, xmy, orbo.T)) dmzoo = reduce(numpy.dot, (orbo, doo, orbo.T)) dmzoo+= reduce(numpy.dot, (orbv, dvv, orbv.T)) mem_now = lib.current_memory()[0] max_memory = max(2000, td_grad.max_memory*.9-mem_now) ni = mf._numint ni.libxc.test_deriv_order(mf.xc, 3, raise_error=True) omega, alpha, hyb = ni.rsh_and_hybrid_coeff(mf.xc, mol.spin) f1vo, f1oo, vxc1, k1ao = \ _contract_xc_kernel(td_grad, mf.xc, dmxpy, dmzoo, True, True, singlet, max_memory) if ni.libxc.is_hybrid_xc(mf.xc): dm = (dmzoo, dmxpy+dmxpy.T, dmxmy-dmxmy.T) vj, vk = mf.get_jk(mol, dm, hermi=0) vk *= hyb if omega != 0: vk += mf.get_k(mol, dm, hermi=0, omega=omega) * (alpha-hyb) veff0doo = vj[0] * 2 - vk[0] + f1oo[0] + k1ao[0] * 2 wvo = reduce(numpy.dot, (orbv.T, veff0doo, orbo)) * 2 if singlet: veff = vj[1] * 2 - vk[1] + f1vo[0] * 2 else: veff = f1vo[0] - vk[1] veff0mop = reduce(numpy.dot, (mo_coeff.T, veff, mo_coeff)) wvo -= numpy.einsum('ki,ai->ak', veff0mop[:nocc,:nocc], xpy) * 2 wvo += numpy.einsum('ac,ai->ci', veff0mop[nocc:,nocc:], xpy) * 2 veff = -vk[2] veff0mom = reduce(numpy.dot, (mo_coeff.T, veff, mo_coeff)) wvo -= numpy.einsum('ki,ai->ak', veff0mom[:nocc,:nocc], xmy) * 2 wvo += numpy.einsum('ac,ai->ci', veff0mom[nocc:,nocc:], xmy) * 2 else: vj = mf.get_j(mol, (dmzoo, dmxpy+dmxpy.T), hermi=1) veff0doo = vj[0] * 2 + f1oo[0] + k1ao[0] * 2 wvo = reduce(numpy.dot, (orbv.T, veff0doo, orbo)) * 2 if singlet: veff = vj[1] * 2 + f1vo[0] * 2 else: veff = f1vo[0] veff0mop = reduce(numpy.dot, (mo_coeff.T, veff, mo_coeff)) wvo -= numpy.einsum('ki,ai->ak', veff0mop[:nocc,:nocc], xpy) * 2 wvo += numpy.einsum('ac,ai->ci', veff0mop[nocc:,nocc:], xpy) * 2 veff0mom = numpy.zeros((nmo,nmo)) # set singlet=None, generate function for CPHF type response kernel vresp = mf.gen_response(singlet=None, hermi=1) def fvind(x): dm = reduce(numpy.dot, (orbv, x.reshape(nvir,nocc)*2, orbo.T)) v1ao = vresp(dm+dm.T) return reduce(numpy.dot, (orbv.T, v1ao, orbo)).ravel() z1 = cphf.solve(fvind, mo_energy, mo_occ, wvo, max_cycle=td_grad.cphf_max_cycle, tol=td_grad.cphf_conv_tol)[0] z1 = z1.reshape(nvir,nocc) time1 = log.timer('Z-vector using CPHF solver', *time0) z1ao = reduce(numpy.dot, (orbv, z1, orbo.T)) veff = vresp(z1ao+z1ao.T) im0 = numpy.zeros((nmo,nmo)) im0[:nocc,:nocc] = reduce(numpy.dot, (orbo.T, veff0doo+veff, orbo)) im0[:nocc,:nocc]+= numpy.einsum('ak,ai->ki', veff0mop[nocc:,:nocc], xpy) im0[:nocc,:nocc]+= numpy.einsum('ak,ai->ki', veff0mom[nocc:,:nocc], xmy) im0[nocc:,nocc:] = numpy.einsum('ci,ai->ac', veff0mop[nocc:,:nocc], xpy) im0[nocc:,nocc:]+= numpy.einsum('ci,ai->ac', veff0mom[nocc:,:nocc], xmy) im0[nocc:,:nocc] = numpy.einsum('ki,ai->ak', veff0mop[:nocc,:nocc], xpy)*2 im0[nocc:,:nocc]+= numpy.einsum('ki,ai->ak', veff0mom[:nocc,:nocc], xmy)*2 zeta = lib.direct_sum('i+j->ij', mo_energy, mo_energy) * .5 zeta[nocc:,:nocc] = mo_energy[:nocc] zeta[:nocc,nocc:] = mo_energy[nocc:] dm1 = numpy.zeros((nmo,nmo)) dm1[:nocc,:nocc] = doo dm1[nocc:,nocc:] = dvv dm1[nocc:,:nocc] = z1 dm1[:nocc,:nocc] += numpy.eye(nocc)*2 # for ground state im0 = reduce(numpy.dot, (mo_coeff, im0+zeta*dm1, mo_coeff.T)) # Initialize hcore_deriv with the underlying SCF object because some # extensions (e.g. QM/MM, solvent) modifies the SCF object only. mf_grad = td_grad.base._scf.nuc_grad_method() hcore_deriv = mf_grad.hcore_generator(mol) s1 = mf_grad.get_ovlp(mol) dmz1doo = z1ao + dmzoo oo0 = reduce(numpy.dot, (orbo, orbo.T)) if ni.libxc.is_hybrid_xc(mf.xc): dm = (oo0, dmz1doo+dmz1doo.T, dmxpy+dmxpy.T, dmxmy-dmxmy.T) vj, vk = td_grad.get_jk(mol, dm) vk *= hyb if omega != 0: vk += td_grad.get_k(mol, dm, omega=omega) * (alpha-hyb) vj = vj.reshape(-1,3,nao,nao) vk = vk.reshape(-1,3,nao,nao) veff1 = -vk if singlet: veff1 += vj * 2 else: veff1[:2] += vj[:2] * 2 else: vj = td_grad.get_j(mol, (oo0, dmz1doo+dmz1doo.T, dmxpy+dmxpy.T)) vj = vj.reshape(-1,3,nao,nao) veff1 = numpy.zeros((4,3,nao,nao)) if singlet: veff1[:3] = vj * 2 else: veff1[:2] = vj[:2] * 2 fxcz1 = _contract_xc_kernel(td_grad, mf.xc, z1ao, None, False, False, True, max_memory)[0] veff1[0] += vxc1[1:] veff1[1] +=(f1oo[1:] + fxcz1[1:] + k1ao[1:]*2)*2 # *2 for dmz1doo+dmz1oo.T if singlet: veff1[2] += f1vo[1:] * 2 else: veff1[2] += f1vo[1:] time1 = log.timer('2e AO integral derivatives', *time1) if atmlst is None: atmlst = range(mol.natm) offsetdic = mol.offset_nr_by_atom() de = numpy.zeros((len(atmlst),3)) for k, ia in enumerate(atmlst): shl0, shl1, p0, p1 = offsetdic[ia] # Ground state gradients h1ao = hcore_deriv(ia) h1ao[:,p0:p1] += veff1[0,:,p0:p1] h1ao[:,:,p0:p1] += veff1[0,:,p0:p1].transpose(0,2,1) # oo0*2 for doubly occupied orbitals e1 = numpy.einsum('xpq,pq->x', h1ao, oo0) * 2 e1 += numpy.einsum('xpq,pq->x', h1ao, dmz1doo) e1 -= numpy.einsum('xpq,pq->x', s1[:,p0:p1], im0[p0:p1]) e1 -= numpy.einsum('xqp,pq->x', s1[:,p0:p1], im0[:,p0:p1]) e1 += numpy.einsum('xij,ij->x', veff1[1,:,p0:p1], oo0[p0:p1]) e1 += numpy.einsum('xij,ij->x', veff1[2,:,p0:p1], dmxpy[p0:p1,:]) * 2 e1 += numpy.einsum('xji,ij->x', veff1[2,:,p0:p1], dmxpy[:,p0:p1]) * 2 e1 += numpy.einsum('xij,ij->x', veff1[3,:,p0:p1], dmxmy[p0:p1,:]) * 2 e1 -= numpy.einsum('xji,ij->x', veff1[3,:,p0:p1], dmxmy[:,p0:p1]) * 2 e1 += td_grad.extra_force(ia, locals()) de[k] = e1 log.timer('TDRKS nuclear gradients', *time0) return de
# dmvo, dmoo in AO-representation # Note spin-trace is applied for fxc, kxc #TODO: to include the response of grids def _contract_xc_kernel(td_grad, xc_code, dmvo, dmoo=None, with_vxc=True, with_kxc=True, singlet=True, max_memory=2000): mol = td_grad.mol mf = td_grad.base._scf grids = mf.grids ni = mf._numint xctype = ni._xc_type(xc_code) mo_coeff = mf.mo_coeff mo_occ = mf.mo_occ nao, nmo = mo_coeff.shape shls_slice = (0, mol.nbas) ao_loc = mol.ao_loc_nr() # dmvo ~ reduce(numpy.dot, (orbv, Xai, orbo.T)) dmvo = (dmvo + dmvo.T) * .5 # because K_{ia,jb} == K_{ia,bj} f1vo = numpy.zeros((4,nao,nao)) # 0th-order, d/dx, d/dy, d/dz deriv = 2 if dmoo is not None: f1oo = numpy.zeros((4,nao,nao)) else: f1oo = None if with_vxc: v1ao = numpy.zeros((4,nao,nao)) else: v1ao = None if with_kxc: k1ao = numpy.zeros((4,nao,nao)) deriv = 3 else: k1ao = None if xctype == 'HF': return f1vo, f1oo, v1ao, k1ao elif xctype == 'LDA': fmat_, ao_deriv = _lda_eval_mat_, 1 elif xctype == 'GGA': fmat_, ao_deriv = _gga_eval_mat_, 2 elif xctype == 'MGGA': fmat_, ao_deriv = _mgga_eval_mat_, 2 logger.warn(td_grad, 'TDRKS-MGGA Gradients may be inaccurate due to grids response') else: raise NotImplementedError(f'td-rks for functional {xc_code}') if singlet: for ao, mask, weight, coords \ in ni.block_loop(mol, grids, nao, ao_deriv, max_memory): if xctype == 'LDA': ao0 = ao[0] else: ao0 = ao rho = ni.eval_rho2(mol, ao0, mo_coeff, mo_occ, mask, xctype, with_lapl=False) vxc, fxc, kxc = ni.eval_xc_eff(xc_code, rho, deriv, xctype=xctype)[1:] rho1 = ni.eval_rho(mol, ao0, dmvo, mask, xctype, hermi=1, with_lapl=False) * 2 # *2 for alpha + beta if xctype == 'LDA': rho1 = rho1[numpy.newaxis] wv = numpy.einsum('yg,xyg,g->xg', rho1, fxc, weight) fmat_(mol, f1vo, ao, wv, mask, shls_slice, ao_loc) if dmoo is not None: rho2 = ni.eval_rho(mol, ao0, dmoo, mask, xctype, hermi=1, with_lapl=False) * 2 if xctype == 'LDA': rho2 = rho2[numpy.newaxis] wv = numpy.einsum('yg,xyg,g->xg', rho2, fxc, weight) fmat_(mol, f1oo, ao, wv, mask, shls_slice, ao_loc) if with_vxc: fmat_(mol, v1ao, ao, vxc * weight, mask, shls_slice, ao_loc) if with_kxc: wv = numpy.einsum('yg,zg,xyzg,g->xg', rho1, rho1, kxc, weight) fmat_(mol, k1ao, ao, wv, mask, shls_slice, ao_loc) else: for ao, mask, weight, coords \ in ni.block_loop(mol, grids, nao, ao_deriv, max_memory): if xctype == 'LDA': ao0 = ao[0] else: ao0 = ao rho = ni.eval_rho2(mol, ao0, mo_coeff, mo_occ, mask, xctype, with_lapl=False) rho *= .5 rho = numpy.repeat(rho[numpy.newaxis], 2, axis=0) vxc, fxc, kxc = ni.eval_xc_eff(xc_code, rho, deriv, xctype=xctype)[1:] # fxc_t couples triplet excitation amplitues # 1/2 int (tia - tIA) fxc (tjb - tJB) = tia fxc_t tjb fxc_t = fxc[:,:,0] - fxc[:,:,1] fxc_t = fxc_t[0] - fxc_t[1] rho1 = ni.eval_rho(mol, ao0, dmvo, mask, xctype, hermi=1, with_lapl=False) if xctype == 'LDA': rho1 = rho1[numpy.newaxis] wv = numpy.einsum('yg,xyg,g->xg', rho1, fxc_t, weight) fmat_(mol, f1vo, ao, wv, mask, shls_slice, ao_loc) if dmoo is not None: # fxc_s == 2 * fxc of spin restricted xc kernel # provides f1oo to couple the interaction between first order MO # and density response of tddft amplitudes, which is described by dmoo fxc_s = fxc[0,:,0] + fxc[0,:,1] rho2 = ni.eval_rho(mol, ao0, dmoo, mask, xctype, hermi=1, with_lapl=False) if xctype == 'LDA': rho2 = rho2[numpy.newaxis] wv = numpy.einsum('yg,xyg,g->xg', rho2, fxc_s, weight) fmat_(mol, f1oo, ao, wv, mask, shls_slice, ao_loc) if with_vxc: vxc = vxc[0] fmat_(mol, v1ao, ao, vxc * weight, mask, shls_slice, ao_loc) if with_kxc: # kxc in terms of the triplet coupling # 1/2 int (tia - tIA) kxc (tjb - tJB) = tia kxc_t tjb kxc = kxc[0,:,0] - kxc[0,:,1] kxc = kxc[:,:,0] - kxc[:,:,1] wv = numpy.einsum('yg,zg,xyzg,g->xg', rho1, rho1, kxc, weight) fmat_(mol, k1ao, ao, wv, mask, shls_slice, ao_loc) f1vo[1:] *= -1 if f1oo is not None: f1oo[1:] *= -1 if v1ao is not None: v1ao[1:] *= -1 if k1ao is not None: k1ao[1:] *= -1 return f1vo, f1oo, v1ao, k1ao def _lda_eval_mat_(mol, vmat, ao, wv, mask, shls_slice, ao_loc): aow = numint._scale_ao(ao[0], wv[0]) for k in range(4): vmat[k] += numint._dot_ao_ao(mol, ao[k], aow, mask, shls_slice, ao_loc) return vmat def _gga_eval_mat_(mol, vmat, ao, wv, mask, shls_slice, ao_loc): wv[0] *= .5 # *.5 because vmat + vmat.T at the end aow = numint._scale_ao(ao[:4], wv[:4]) tmp = numint._dot_ao_ao(mol, ao[0], aow, mask, shls_slice, ao_loc) vmat[0] += tmp + tmp.T rks_grad._gga_grad_sum_(vmat[1:], mol, ao, wv, mask, ao_loc) return vmat def _mgga_eval_mat_(mol, vmat, ao, wv, mask, shls_slice, ao_loc): wv[0] *= .5 # *.5 because vmat + vmat.T at the end wv[4] *= .5 # *.5 for 1/2 in tau aow = numint._scale_ao(ao[:4], wv[:4]) tmp = numint._dot_ao_ao(mol, ao[0], aow, mask, shls_slice, ao_loc) vmat[0] += tmp + tmp.T vmat[0] += numint._tau_dot(mol, ao, ao, wv[4], mask, shls_slice, ao_loc) rks_grad._gga_grad_sum_(vmat[1:], mol, ao, wv[:4], mask, ao_loc) rks_grad._tau_grad_dot_(vmat[1:], mol, ao, wv[4], mask, ao_loc, True) return vmat
[docs] class Gradients(tdrhf.Gradients):
[docs] @lib.with_doc(grad_elec.__doc__) def grad_elec(self, xy, singlet, atmlst=None): return grad_elec(self, xy, singlet, atmlst, self.max_memory, self.verbose)
Grad = Gradients from pyscf import tdscf tdscf.rks.TDA.Gradients = tdscf.rks.TDDFT.Gradients = lib.class_as_method(Gradients)