def psi4_clean():
"""Function to put Psi4 back to a clean state. In particular deletes
scratch files and resets Psi variables. Call as last part of the real
deriv call to Psi4.
"""
psi4.clean_variables()
psi4.clean()
def __init__(self, molecule, basis, numpy_memory=2.e9, scf_type="PK", use_c=False):
# Set defaults
maxiter = 40
E_conv = 1.0E-6
D_conv = 1.0E-3
# Integral generation from Psi4's MintsHelper
start_time = time.time()
self.basis_name = basis
self.molecule = molecule
self.basis = pc.BasisSet.build(self.molecule, "ORBITAL", basis)
self.mints = pc.MintsHelper(self.basis)
self.S = np.asarray(self.mints.ao_overlap())
# Get nbf and ndocc for closed shell molecules
self.nbf = self.S.shape[0]
self.nel = sum(self.molecule.Z(n) for n in range(self.molecule.natom()))
self.nel -= self.molecule.molecular_charge()
if not (self.nel / 2.0).is_integer():
raise ValueError("RHF: Molecule did not have an even number of electrons!")
self.ndocc = int(self.nel / 2.0)
print('\nNumber of occupied orbitals: %d' % self.ndocc)
print('Number of basis functions: %d' % self.nbf)
# Run a quick check to make sure everything will fit into memory
I_Size = (self.nbf**4) * 8.e-9
print("\nSize of the ERI tensor will be %4.2f GB." % I_Size)
# Estimate memory usage
memory_footprint = I_Size * 1.5
if I_Size > numpy_memory:
pc.clean()
raise Exception("Estimated memory utilization (%4.2f GB) exceeds numpy_memory \
limit of %4.2f GB." % (memory_footprint, numpy_memory))
# Compute required quantities for SCF
self.V = np.asarray(self.mints.ao_potential())
self.T = np.asarray(self.mints.ao_kinetic())
# self.I = np.asarray(self.mints.ao_eri())
self.JK = jk.build_JK(self.molecule, self.basis_name, scf_type, use_c)
self.Enuc = self.molecule.nuclear_repulsion_energy()
print('\nTotal time taken for integrals: %.3f seconds.' % (time.time() - start_time))
t = time.time()
# Build H_core
self.H = self.T + self.V
# Orthogonalizer A = S^(-1/2) using Psi4's matrix power.
A = self.mints.ao_overlap()
A.power(-0.5, 1.e-16)
self.A = np.asarray(A)
print('\nTotal time taken for setup: %.3f seconds' % (time.time() - start_time))
def _clean_psi_environ(do_clean: bool):
"""Reset work environment to new Psi4 instance state.
This includes global variables (P::e.globals, P::e.arrays, P::e.options) and any
non-explicitly-retained PSIO-managed scratch files.
"""
if do_clean:
core.clean_variables()
core.clean_options()
core.clean()
def compute_energy(self, maxiter=12, E_conv=1.e-6, D_conv=1.e-4):
print('\nStarting SCF iterations:\n')
t = time.time()
E = 0.0
Eold = 0.0
Dold = np.zeros_like(self.H)
self.form_orbitals(self.H)
for SCF_ITER in range(1, maxiter + 1):
# Build Fock matrix
self.build_fock(self.D)
# Build DIIS error vector
diis_e = np.dot(self.F, self.D).dot(self.S) - np.dot(
self.S, self.D).dot(self.F)
# Make sure that error is normalized!
diis_e = (self.A).dot(diis_e).dot(self.A)
# SCF energy and update
SCF_E = np.einsum('pq,pq->', self.F + self.H, self.D) + self.Enuc
dRMS = np.mean(diis_e**2)**0.5
print(
'SCF Iteration %3d: Energy = %4.16f dE = % 1.5E dRMS = %1.5E'
% (SCF_ITER, SCF_E, (SCF_E - Eold), dRMS))
if (abs(SCF_E - Eold) < E_conv) and (dRMS < D_conv):
break
Eold = SCF_E
Dold = self.D.copy()
self.form_orbitals(self.F)
if SCF_ITER == maxiter:
pc.clean()
raise Exception("Maximum number of SCF cycles exceeded.")
print('Total time for SCF iterations: %.3f seconds \n' %
(time.time() - t))
print('Final SCF energy: %.8f hartree' % SCF_E)
self.SCF_E = SCF_E
return SCF_E
def __exit__(self, type, value, traceback):
for calc in (calcid(*x)
for x in itertools.product(('m1', 'm2',
'd'), ('m', 'd'), ('low',
'high'))):
core.IO.set_default_namespace(self.fmt_ns(calc))
core.IOManager.shared_object().set_specific_retention(
psif.PSIF_DFSCF_BJ, False)
try:
extras.clean_numpy_files()
except OSError:
pass
extras.numpy_files = []
core.clean()
os.chdir(self._original_path)
def compute(self,
mol_name='m1',
basis_center='m',
basis_quality='low',
mp2=False,
mp2_dm=False,
save_jk=False):
calc = calcid(mol_name, basis_center, basis_quality)
molecule = self.molecule(calc)
molecule.set_name(self.fmt_ns(calc))
basis = self.basis_sets[basis_quality]
self._banner(calc, mp2, mp2_dm)
optstash = p4util.optproc.OptionsState(['SCF', 'DF_INTS_IO'],
['DF_INTS_IO'],
['SCF', 'GUESS'])
self._init_ns(calc)
self._init_df(calc)
with psiopts(
'SCF_TYPE DF',
'MP2_TYPE DF',
'BASIS %s' % basis,
'DF_BASIS_SCF %s-JKFIT' % basis,
'DF_BASIS_MP2 %s-RI' % basis,
'SCF SAVE_JK %s' % save_jk,
'ONEPDM TRUE',
'NUM_FROZEN_DOCC %d' % nfrozen_core(molecule),
):
wfn = scf_helper('scf', molecule=molecule)
assert nfrozen_core(molecule) == wfn.nfrzc()
if mp2 and not mp2_dm:
wfn = run_dfmp2('df-mp2', molecule=molecule, ref_wfn=wfn)
if mp2 and mp2_dm:
wfn = run_dfmp2_gradient('df-mp2',
molecule=molecule,
ref_wfn=wfn)
if mp2_dm and not mp2:
raise ValueError('These options dont make sense')
self.wfn_cache[calc] = wfn
optstash.restore()
core.clean()
return wfn
def compute_energy(self, maxiter=12, E_conv=1.e-6, D_conv=1.e-4):
print('\nStarting SCF iterations:\n')
t = time.time()
E = 0.0
Eold = 0.0
Dold = np.zeros_like(self.H)
self.form_orbitals(self.H)
for SCF_ITER in range(1, maxiter + 1):
# Build Fock matrix
self.build_fock(self.D)
# Build DIIS error vector
diis_e = np.dot(self.F, self.D).dot(self.S) - np.dot(self.S, self.D).dot(self.F)
# Make sure that error is normalized!
diis_e = (self.A).dot(diis_e).dot(self.A)
# SCF energy and update
SCF_E = np.einsum('pq,pq->', self.F + self.H, self.D) + self.Enuc
dRMS = np.mean(diis_e**2)**0.5
print('SCF Iteration %3d: Energy = %4.16f dE = % 1.5E dRMS = %1.5E' % (SCF_ITER, SCF_E, (SCF_E - Eold),
dRMS))
if (abs(SCF_E - Eold) < E_conv) and (dRMS < D_conv):
break
Eold = SCF_E
Dold = self.D.copy()
self.form_orbitals(self.F)
if SCF_ITER == maxiter:
pc.clean()
raise Exception("Maximum number of SCF cycles exceeded.")
print('Total time for SCF iterations: %.3f seconds \n' % (time.time() - t))
print('Final SCF energy: %.8f hartree' % SCF_E)
self.SCF_E = SCF_E
return SCF_E
def fd_db_run(self, executable, nThreads=1, jobs_in_progress=False):
self.pr('(ROA) Running finite-difference computations.\n')
cwd = os.getcwd() + '/'
# Want to change to json later.
def runDisp(subDir):
rootDir = os.getcwd() + '/'
self.pr("Running displacement %s\n" % subDir)
rc = subprocess.run(executable, cwd=rootDir + '/' + subDir)
if rc.returncode != 0:
raise ("Tensor calculation failed.")
def batch(batch_list, batch_size):
b = []
for elem in batch_list:
b.append(elem)
if len(b) == batch_size:
yield b
b.clear()
yield b
self.update_status_fd_db(print_status=True, jobs_in_progress=False)
todo = [
lbl for lbl, info in self.db['jobs'].items()
if info['status'] == 'not_started'
]
self.pr('(ROA) Remaining jobs todo: {}\n'.format(str(todo)))
fd_threads = []
for b in batch(todo, nThreads):
fd_threads.clear()
for job_lbl in b:
t = threading.Thread(target=runDisp, args=(job_lbl, ))
fd_threads.append(t)
t.start()
for t in fd_threads:
t.join()
core.clean()
def database(name, db_name, **kwargs):
r"""Function to access the molecule objects and reference energies of
popular chemical databases.
:aliases: db()
:returns: (*float*) Mean absolute deviation of the database in kcal/mol
:PSI variables:
.. hlist::
:columns: 1
* :psivar:`db_name DATABASE MEAN SIGNED DEVIATION`
* :psivar:`db_name DATABASE MEAN ABSOLUTE DEVIATION`
* :psivar:`db_name DATABASE ROOT-MEAN-SQUARE DEVIATION`
* Python dictionaries of results accessible as ``DB_RGT`` and ``DB_RXN``.
.. note:: It is very easy to make a database from a collection of xyz files
using the script :source:`psi4/share/psi4/scripts/ixyz2database.py`.
See :ref:`sec:createDatabase` for details.
.. caution:: Some features are not yet implemented. Buy a developer some coffee.
- In sow/reap mode, use only global options (e.g., the local option set by ``set scf scf_type df`` will not be respected).
.. note:: To access a database that is not embedded in a |PSIfour|
distribution, add the path to the directory containing the database
to the environment variable :envvar:`PYTHONPATH`.
:type name: str
:param name: ``'scf'`` || ``'sapt0'`` || ``'ccsd(t)'`` || etc.
First argument, usually unlabeled. Indicates the computational method
to be applied to the database. May be any valid argument to
:py:func:`psi4.driver.energy`.
:type db_name: str
:param db_name: ``'BASIC'`` || ``'S22'`` || ``'HTBH'`` || etc.
Second argument, usually unlabeled. Indicates the requested database
name, matching (case insensitive) the name of a python file in
``psi4/share/databases`` or :envvar:`PYTHONPATH`. Consult that
directory for available databases and literature citations.
:type func: :ref:`function <op_py_function>`
:param func: |dl| ``energy`` |dr| || ``optimize`` || ``cbs``
Indicates the type of calculation to be performed on each database
member. The default performs a single-point ``energy('name')``, while
``optimize`` perfoms a geometry optimization on each reagent, and
``cbs`` performs a compound single-point energy. If a nested series
of python functions is intended (see :ref:`sec:intercalls`), use
keyword ``db_func`` instead of ``func``.
:type mode: str
:param mode: |dl| ``'continuous'`` |dr| || ``'sow'`` || ``'reap'``
Indicates whether the calculations required to complete the
database are to be run in one file (``'continuous'``) or are to be
farmed out in an embarrassingly parallel fashion
(``'sow'``/``'reap'``). For the latter, run an initial job with
``'sow'`` and follow instructions in its output file.
:type cp: :ref:`boolean <op_py_boolean>`
:param cp: ``'on'`` || |dl| ``'off'`` |dr|
Indicates whether counterpoise correction is employed in computing
interaction energies. Use this option and NOT the ``bsse_type="cp"``
function for BSSE correction in database(). Option available
(See :ref:`sec:availableDatabases`) only for databases of bimolecular complexes.
:type rlxd: :ref:`boolean <op_py_boolean>`
:param rlxd: ``'on'`` || |dl| ``'off'`` |dr|
Indicates whether correction for deformation energy is
employed in computing interaction energies. Option available
(See :ref:`sec:availableDatabases`) only for databases of bimolecular complexes
with non-frozen monomers, e.g., HBC6.
:type symm: :ref:`boolean <op_py_boolean>`
:param symm: |dl| ``'on'`` |dr| || ``'off'``
Indicates whether the native symmetry of the database reagents is
employed (``'on'``) or whether it is forced to :math:`C_1` symmetry
(``'off'``). Some computational methods (e.g., SAPT) require no
symmetry, and this will be set by database().
:type zpe: :ref:`boolean <op_py_boolean>`
:param zpe: ``'on'`` || |dl| ``'off'`` |dr|
Indicates whether zero-point-energy corrections are appended to
single-point energy values. Option valid only for certain
thermochemical databases. Disabled until Hessians ready.
:type benchmark: str
:param benchmark: |dl| ``'default'`` |dr| || ``'S22A'`` || etc.
Indicates whether a non-default set of reference energies, if
available (See :ref:`sec:availableDatabases`), are employed for the
calculation of error statistics.
:type tabulate: List[str]
:param tabulate: |dl| ``[]`` |dr| || ``['scf total energy', 'natom']`` || etc.
Indicates whether to form tables of variables other than the
primary requested energy. Available for any PSI variable.
:type subset: Union[str, List[str]]
:param subset:
Indicates a subset of the full database to run. This is a very
flexible option and can be used in three distinct ways, outlined
below. Note that two take a string and the last takes an array.
See :ref:`sec:availableDatabases` for available values.
* ``'small'`` || ``'large'`` || ``'equilibrium'``
Calls predefined subsets of the requested database, either
``'small'``, a few of the smallest database members,
``'large'``, the largest of the database members, or
``'equilibrium'``, the equilibrium geometries for a database
composed of dissociation curves.
* ``'BzBz_S'`` || ``'FaOOFaON'`` || ``'ArNe'`` || ``'HB'`` || etc.
For databases composed of dissociation curves, or otherwise
divided into subsets, individual curves and subsets can be
called by name. Consult the database python files for available
molecular systems (case insensitive).
* ``[1,2,5]`` || ``['1','2','5']`` || ``['BzMe-3.5', 'MeMe-5.0']`` || etc.
Specify a list of database members to run. Consult the
database python files for available molecular systems. This
is the only portion of database input that is case sensitive;
choices for this keyword must match the database python file.
:examples:
>>> # [1] Two-stage SCF calculation on short, equilibrium, and long helium dimer
>>> db('scf','RGC10',cast_up='sto-3g',subset=['HeHe-0.85','HeHe-1.0','HeHe-1.5'], tabulate=['scf total energy','natom'])
>>> # [2] Counterpoise-corrected interaction energies for three complexes in S22
>>> # Error statistics computed wrt an old benchmark, S22A
>>> database('mp2','S22',cp=1,subset=[16,17,8],benchmark='S22A')
>>> # [3] SAPT0 on the neon dimer dissociation curve
>>> db('sapt0',subset='NeNe',cp=0,symm=0,db_name='RGC10')
>>> # [4] Optimize system 1 in database S22, producing tables of scf and mp2 energy
>>> db('mp2','S22',db_func=optimize,subset=[1], tabulate=['mp2 total energy','current energy'])
>>> # [5] CCSD on the smallest systems of HTBH, a hydrogen-transfer database
>>> database('ccsd','HTBH',subset='small', tabulate=['ccsd total energy', 'mp2 total energy'])
"""
lowername = name #TODO
kwargs = p4util.kwargs_lower(kwargs)
# Wrap any positional arguments into kwargs (for intercalls among wrappers)
if not ('name' in kwargs) and name:
kwargs['name'] = name #.lower()
if not ('db_name' in kwargs) and db_name:
kwargs['db_name'] = db_name
# Establish function to call
func = kwargs.pop('db_func', kwargs.pop('func', energy))
kwargs['db_func'] = func
# Bounce to CP if bsse kwarg (someday)
if kwargs.get('bsse_type', None) is not None:
raise ValidationError(
"""Database: Cannot specify bsse_type for database. Use the cp keyword withing database instead."""
)
allowoptexceeded = kwargs.get('allowoptexceeded', False)
optstash = p4util.OptionsState(['WRITER_FILE_LABEL'], ['SCF', 'REFERENCE'])
# Wrapper wholly defines molecule. discard any passed-in
kwargs.pop('molecule', None)
# Paths to search for database files: here + PSIPATH + library + PYTHONPATH
db_paths = []
db_paths.append(os.getcwd())
db_paths.extend(os.environ.get('PSIPATH', '').split(os.path.pathsep))
db_paths.append(os.path.join(core.get_datadir(), 'databases'))
db_paths.append(os.path.dirname(__file__))
db_paths = list(map(os.path.abspath, db_paths))
sys.path[1:1] = db_paths
# TODO this should be modernized a la interface_cfour
# Define path and load module for requested database
database = p4util.import_ignorecase(db_name)
if database is None:
core.print_out('\nPython module for database %s failed to load\n\n' %
(db_name))
core.print_out('\nSearch path that was tried:\n')
core.print_out(", ".join(map(str, sys.path)))
raise ValidationError("Python module loading problem for database " +
str(db_name))
else:
dbse = database.dbse
HRXN = database.HRXN
ACTV = database.ACTV
RXNM = database.RXNM
BIND = database.BIND
TAGL = database.TAGL
GEOS = database.GEOS
try:
DATA = database.DATA
except AttributeError:
DATA = {}
user_writer_file_label = core.get_global_option('WRITER_FILE_LABEL')
user_reference = core.get_global_option('REFERENCE')
# Configuration based upon e_name & db_name options
# Force non-supramolecular if needed
if not hasattr(lowername, '__call__') and re.match(r'^.*sapt', lowername):
try:
database.ACTV_SA
except AttributeError:
raise ValidationError(
'Database %s not suitable for non-supramolecular calculation.'
% (db_name))
else:
ACTV = database.ACTV_SA
# Force open-shell if needed
openshell_override = 0
if user_reference in ['RHF', 'RKS']:
try:
database.isOS
except AttributeError:
pass
else:
if p4util.yes.match(str(database.isOS)):
openshell_override = 1
core.print_out(
'\nSome reagents in database %s require an open-shell reference; will be reset to UHF/UKS as needed.\n'
% (db_name))
# Configuration based upon database keyword options
# Option symmetry- whether symmetry treated normally or turned off (currently req'd for dfmp2 & dft)
db_symm = kwargs.get('symm', True)
symmetry_override = 0
if db_symm is False:
symmetry_override = 1
elif db_symm is True:
pass
else:
raise ValidationError("""Symmetry mode '%s' not valid.""" % (db_symm))
# Option mode of operation- whether db run in one job or files farmed out
db_mode = kwargs.pop('db_mode', kwargs.pop('mode', 'continuous')).lower()
kwargs['db_mode'] = db_mode
if db_mode == 'continuous':
pass
elif db_mode == 'sow':
pass
elif db_mode == 'reap':
db_linkage = kwargs.get('linkage', None)
if db_linkage is None:
raise ValidationError(
"""Database execution mode 'reap' requires a linkage option."""
)
else:
raise ValidationError("""Database execution mode '%s' not valid.""" %
(db_mode))
# Option counterpoise- whether for interaction energy databases run in bsse-corrected or not
db_cp = kwargs.get('cp', False)
if db_cp is True:
try:
database.ACTV_CP
except AttributeError:
raise ValidationError(
"""Counterpoise correction mode 'yes' invalid for database %s."""
% (db_name))
else:
ACTV = database.ACTV_CP
elif db_cp is False:
pass
else:
raise ValidationError(
"""Counterpoise correction mode '%s' not valid.""" % (db_cp))
# Option relaxed- whether for non-frozen-monomer interaction energy databases include deformation correction or not?
db_rlxd = kwargs.get('rlxd', False)
if db_rlxd is True:
if db_cp is True:
try:
database.ACTV_CPRLX
database.RXNM_CPRLX
except AttributeError:
raise ValidationError(
'Deformation and counterpoise correction mode \'yes\' invalid for database %s.'
% (db_name))
else:
ACTV = database.ACTV_CPRLX
RXNM = database.RXNM_CPRLX
elif db_cp is False:
try:
database.ACTV_RLX
except AttributeError:
raise ValidationError(
'Deformation correction mode \'yes\' invalid for database %s.'
% (db_name))
else:
ACTV = database.ACTV_RLX
elif db_rlxd is False:
#elif no.match(str(db_rlxd)):
pass
else:
raise ValidationError('Deformation correction mode \'%s\' not valid.' %
(db_rlxd))
# Option zero-point-correction- whether for thermochem databases jobs are corrected by zpe
db_zpe = kwargs.get('zpe', False)
if db_zpe is True:
raise ValidationError(
'Zero-point-correction mode \'yes\' not yet implemented.')
elif db_zpe is False:
pass
else:
raise ValidationError('Zero-point-correction \'mode\' %s not valid.' %
(db_zpe))
# Option benchmark- whether error statistics computed wrt alternate reference energies
db_benchmark = 'default'
if 'benchmark' in kwargs:
db_benchmark = kwargs['benchmark']
if db_benchmark.lower() == 'default':
pass
else:
BIND = p4util.getattr_ignorecase(database, 'BIND_' + db_benchmark)
if BIND is None:
raise ValidationError(
'Special benchmark \'%s\' not available for database %s.' %
(db_benchmark, db_name))
# Option tabulate- whether tables of variables other than primary energy method are formed
# TODO db(func=cbs,tabulate=[non-current-energy]) # broken
db_tabulate = []
if 'tabulate' in kwargs:
db_tabulate = kwargs['tabulate']
# Option subset- whether all of the database or just a portion is run
db_subset = HRXN
if 'subset' in kwargs:
db_subset = kwargs['subset']
if isinstance(db_subset, (str, bytes)):
if db_subset.lower() == 'small':
try:
database.HRXN_SM
except AttributeError:
raise ValidationError(
"""Special subset 'small' not available for database %s."""
% (db_name))
else:
HRXN = database.HRXN_SM
elif db_subset.lower() == 'large':
try:
database.HRXN_LG
except AttributeError:
raise ValidationError(
"""Special subset 'large' not available for database %s."""
% (db_name))
else:
HRXN = database.HRXN_LG
elif db_subset.lower() == 'equilibrium':
try:
database.HRXN_EQ
except AttributeError:
raise ValidationError(
"""Special subset 'equilibrium' not available for database %s."""
% (db_name))
else:
HRXN = database.HRXN_EQ
else:
HRXN = p4util.getattr_ignorecase(database, db_subset)
if HRXN is None:
HRXN = p4util.getattr_ignorecase(database, 'HRXN_' + db_subset)
if HRXN is None:
raise ValidationError(
"""Special subset '%s' not available for database %s."""
% (db_subset, db_name))
else:
temp = []
for rxn in db_subset:
if rxn in HRXN:
temp.append(rxn)
else:
raise ValidationError(
"""Subset element '%s' not a member of database %s.""" %
(str(rxn), db_name))
HRXN = temp
temp = []
for rxn in HRXN:
temp.append(ACTV['%s-%s' % (dbse, rxn)])
HSYS = p4util.drop_duplicates(sum(temp, []))
# Sow all the necessary reagent computations
core.print_out("\n\n")
p4util.banner(("Database %s Computation" % (db_name)))
core.print_out("\n")
# write index of calcs to output file
instructions = """\n The database single-job procedure has been selected through mode='continuous'.\n"""
instructions += """ Calculations for the reagents will proceed in the order below and will be followed\n"""
instructions += """ by summary results for the database.\n\n"""
for rgt in HSYS:
instructions += """ %-s\n""" % (rgt)
core.print_out(instructions)
# Loop through chemical systems
ERGT = {}
ERXN = {}
VRGT = {}
VRXN = {}
for rgt in HSYS:
VRGT[rgt] = {}
core.print_out('\n')
p4util.banner(' Database {} Computation: Reagent {} \n {}'.format(
db_name, rgt, TAGL[rgt]))
core.print_out('\n')
molecule = core.Molecule.from_dict(GEOS[rgt].to_dict())
molecule.set_name(rgt)
molecule.update_geometry()
if symmetry_override:
molecule.reset_point_group('c1')
molecule.fix_orientation(True)
molecule.fix_com(True)
molecule.update_geometry()
if (openshell_override) and (molecule.multiplicity() != 1):
if user_reference == 'RHF':
core.set_global_option('REFERENCE', 'UHF')
elif user_reference == 'RKS':
core.set_global_option('REFERENCE', 'UKS')
core.set_global_option(
'WRITER_FILE_LABEL', user_writer_file_label +
('' if user_writer_file_label == '' else '-') + rgt)
if allowoptexceeded:
try:
ERGT[rgt] = func(molecule=molecule, **kwargs)
except ConvergenceError:
core.print_out(f"Optimization exceeded cycles for {rgt}")
ERGT[rgt] = 0.0
else:
ERGT[rgt] = func(molecule=molecule, **kwargs)
core.print_variables()
core.print_out(" Database Contributions Map:\n {}\n".format('-' *
75))
for rxn in HRXN:
db_rxn = dbse + '-' + str(rxn)
if rgt in ACTV[db_rxn]:
core.print_out(
' reagent {} contributes by {:.4f} to reaction {}\n'.
format(rgt, RXNM[db_rxn][rgt], db_rxn))
core.print_out('\n')
for envv in db_tabulate:
VRGT[rgt][envv.upper()] = core.variable(envv)
core.set_global_option("REFERENCE", user_reference)
core.clean()
#core.opt_clean()
core.clean_variables()
# Reap all the necessary reaction computations
core.print_out("\n")
p4util.banner(("Database %s Results" % (db_name)))
core.print_out("\n")
maxactv = []
for rxn in HRXN:
maxactv.append(len(ACTV[dbse + '-' + str(rxn)]))
maxrgt = max(maxactv)
table_delimit = '-' * (62 + 20 * maxrgt)
tables = ''
# find any reactions that are incomplete
FAIL = collections.defaultdict(int)
for rxn in HRXN:
db_rxn = dbse + '-' + str(rxn)
for i in range(len(ACTV[db_rxn])):
if abs(ERGT[ACTV[db_rxn][i]]) < 1.0e-12:
if not allowoptexceeded:
FAIL[rxn] = 1
# tabulate requested process::environment variables
tables += """ For each VARIABLE requested by tabulate, a 'Reaction Value' will be formed from\n"""
tables += """ 'Reagent' values according to weightings 'Wt', as for the REQUESTED ENERGY below.\n"""
tables += """ Depending on the nature of the variable, this may or may not make any physical sense.\n"""
for rxn in HRXN:
db_rxn = dbse + '-' + str(rxn)
VRXN[db_rxn] = {}
for envv in db_tabulate:
envv = envv.upper()
tables += """\n ==> %s <==\n\n""" % (envv.title())
tables += _tblhead(maxrgt, table_delimit, 2)
for rxn in HRXN:
db_rxn = dbse + '-' + str(rxn)
if FAIL[rxn]:
tables += """\n%23s %8s %8s %8s %8s""" % (db_rxn, '', '****',
'', '')
for i in range(len(ACTV[db_rxn])):
tables += """ %16.8f %2.0f""" % (VRGT[
ACTV[db_rxn][i]][envv], RXNM[db_rxn][ACTV[db_rxn][i]])
else:
VRXN[db_rxn][envv] = 0.0
for i in range(len(ACTV[db_rxn])):
VRXN[db_rxn][envv] += VRGT[
ACTV[db_rxn][i]][envv] * RXNM[db_rxn][ACTV[db_rxn][i]]
tables += """\n%23s %16.8f """ % (
db_rxn, VRXN[db_rxn][envv])
for i in range(len(ACTV[db_rxn])):
tables += """ %16.8f %2.0f""" % (VRGT[
ACTV[db_rxn][i]][envv], RXNM[db_rxn][ACTV[db_rxn][i]])
tables += """\n %s\n""" % (table_delimit)
# tabulate primary requested energy variable with statistics
count_rxn = 0
minDerror = 100000.0
maxDerror = 0.0
MSDerror = 0.0
MADerror = 0.0
RMSDerror = 0.0
tables += """\n ==> %s <==\n\n""" % ('Requested Energy')
tables += _tblhead(maxrgt, table_delimit, 1)
for rxn in HRXN:
db_rxn = dbse + '-' + str(rxn)
if FAIL[rxn]:
tables += """\n%23s %8.4f %8s %10s %10s""" % (
db_rxn, BIND[db_rxn], '****', '****', '****')
for i in range(len(ACTV[db_rxn])):
tables += """ %16.8f %2.0f""" % (ERGT[ACTV[db_rxn][i]],
RXNM[db_rxn][ACTV[db_rxn][i]])
else:
ERXN[db_rxn] = 0.0
for i in range(len(ACTV[db_rxn])):
ERXN[db_rxn] += ERGT[ACTV[db_rxn][i]] * RXNM[db_rxn][
ACTV[db_rxn][i]]
error = constants.hartree2kcalmol * ERXN[db_rxn] - BIND[db_rxn]
tables += """\n%23s %8.4f %8.4f %10.4f %10.4f""" % (
db_rxn, BIND[db_rxn], constants.hartree2kcalmol * ERXN[db_rxn],
error, error * constants.cal2J)
for i in range(len(ACTV[db_rxn])):
tables += """ %16.8f %2.0f""" % (ERGT[ACTV[db_rxn][i]],
RXNM[db_rxn][ACTV[db_rxn][i]])
if abs(error) < abs(minDerror):
minDerror = error
if abs(error) > abs(maxDerror):
maxDerror = error
MSDerror += error
MADerror += abs(error)
RMSDerror += error * error
count_rxn += 1
tables += """\n %s\n""" % (table_delimit)
if count_rxn:
MSDerror /= float(count_rxn)
MADerror /= float(count_rxn)
RMSDerror = math.sqrt(RMSDerror / float(count_rxn))
tables += """%23s %19s %10.4f %10.4f\n""" % (
'Minimal Dev', '', minDerror, minDerror * constants.cal2J)
tables += """%23s %19s %10.4f %10.4f\n""" % (
'Maximal Dev', '', maxDerror, maxDerror * constants.cal2J)
tables += """%23s %19s %10.4f %10.4f\n""" % (
'Mean Signed Dev', '', MSDerror, MSDerror * constants.cal2J)
tables += """%23s %19s %10.4f %10.4f\n""" % (
'Mean Absolute Dev', '', MADerror, MADerror * constants.cal2J)
tables += """%23s %19s %10.4f %10.4f\n""" % (
'RMS Dev', '', RMSDerror, RMSDerror * constants.cal2J)
tables += """ %s\n""" % (table_delimit)
core.set_variable('%s DATABASE MEAN SIGNED DEVIATION' % (db_name),
MSDerror)
core.set_variable('%s DATABASE MEAN ABSOLUTE DEVIATION' % (db_name),
MADerror)
core.set_variable('%s DATABASE ROOT-MEAN-SQUARE DEVIATION' % (db_name),
RMSDerror)
core.print_out(tables)
finalenergy = MADerror
else:
finalenergy = 0.0
optstash.restore()
DB_RGT.clear()
DB_RGT.update(VRGT)
DB_RXN.clear()
DB_RXN.update(VRXN)
return finalenergy
def compute_nbody_components(func, method_string, metadata):
"""Computes requested N-body components.
Performs requested computations for psi4::Molecule object `molecule` according to
`compute_list` with function `func` at `method_string` level of theory.
Parameters
----------
func : {'energy', 'gradient', 'hessian'}
Function object to be called within N-Body procedure.
method_string : str
Indicates level of theory to be passed to function `func`.
metadata : dict of str
Dictionary of N-body metadata.
Required ``'key': value`` pairs:
``'compute_list'``: dict of int: set
List of computations to perform. Keys indicate body-levels, e.g,. `compute_list[2]` is the
list of all 2-body computations required.
``'kwargs'``: dict
Arbitrary keyword arguments to be passed to function `func`.
Returns
-------
dict of str: dict
Dictionary containing computed N-body components.
Contents:
``'energies'``: dict of set: float64
Dictionary containing all energy components required for given N-body procedure.
``'ptype'``: dict of set: float64 or dict of set: psi4.Matrix
Dictionary of returned quantities from calls of function `func` during N-body computations
``'intermediates'``: dict of str: float64
Dictionary of psivars for intermediate N-body computations to be set at the end of the
N-body procedure.
"""
# Get required metadata
kwargs = metadata['kwargs']
molecule = metadata['molecule']
#molecule = core.get_active_molecule()
compute_list = metadata['compute_dict']['all']
# Now compute the energies
energies_dict = {}
gradients_dict = {}
ptype_dict = {}
intermediates_dict = {}
if kwargs.get('charge_method', False) and not metadata['embedding_charges']:
metadata['embedding_charges'] = driver_nbody_helper.compute_charges(kwargs['charge_method'],
kwargs.get('charge_type', 'MULLIKEN_CHARGES').upper(), molecule)
for count, n in enumerate(compute_list.keys()):
core.print_out("\n ==> N-Body: Now computing %d-body complexes <==\n\n" % n)
total = len(compute_list[n])
for num, pair in enumerate(compute_list[n]):
core.print_out(
"\n N-Body: Computing complex (%d/%d) with fragments %s in the basis of fragments %s.\n\n" %
(num + 1, total, str(pair[0]), str(pair[1])))
ghost = list(set(pair[1]) - set(pair[0]))
current_mol = molecule.extract_subsets(list(pair[0]), ghost)
current_mol.set_name("%s_%i_%i" % (current_mol.name(), count, num))
if metadata['embedding_charges']: driver_nbody_helper.electrostatic_embedding(metadata, pair=pair)
# Save energies info
ptype_dict[pair], wfn = func(method_string, molecule=current_mol, return_wfn=True, **kwargs)
core.set_global_option_python('EXTERN', None)
energies_dict[pair] = core.variable("CURRENT ENERGY")
gradients_dict[pair] = wfn.gradient()
var_key = "N-BODY (%s)@(%s) TOTAL ENERGY" % (', '.join([str(i) for i in pair[0]]), ', '.join(
[str(i) for i in pair[1]]))
intermediates_dict[var_key] = core.variable("CURRENT ENERGY")
core.print_out("\n N-Body: Complex Energy (fragments = %s, basis = %s: %20.14f)\n" % (str(
pair[0]), str(pair[1]), energies_dict[pair]))
# Flip this off for now, needs more testing
#if 'cp' in bsse_type_list and (len(bsse_type_list) == 1):
# core.set_global_option('DF_INTS_IO', 'LOAD')
core.clean()
return {
'energies': energies_dict,
'gradients': gradients_dict,
'ptype': ptype_dict,
'intermediates': intermediates_dict
}
def compute_nbody_components(func, method_string, metadata):
"""Computes requested N-body components.
Performs requested computations for psi4::Molecule object `molecule` according to
`compute_list` with function `func` at `method_string` level of theory.
Parameters
----------
func : str
{'energy', 'gradient', 'hessian'}
Function object to be called within N-Body procedure.
method_string : str
Indicates level of theory to be passed to function `func`.
metadata : dict of str
Dictionary of N-body metadata.
Required ``'key': value`` pairs:
``'compute_list'``: dict of int: set
List of computations to perform. Keys indicate body-levels, e.g,. `compute_list[2]` is the
list of all 2-body computations required.
``'kwargs'``: dict
Arbitrary keyword arguments to be passed to function `func`.
Returns
-------
dict of str: dict
Dictionary containing computed N-body components.
Contents:
``'energies'``: dict of set: float64
Dictionary containing all energy components required for given N-body procedure.
``'ptype'``: dict of set: float64 or dict of set: psi4.Matrix
Dictionary of returned quantities from calls of function `func` during N-body computations
``'intermediates'``: dict of str: float64
Dictionary of psivars for intermediate N-body computations to be set at the end of the
N-body procedure.
"""
# Get required metadata
kwargs = metadata['kwargs']
molecule = metadata['molecule']
#molecule = core.get_active_molecule()
compute_list = metadata['compute_dict']['all']
# Now compute the energies
energies_dict = {}
gradients_dict = {}
ptype_dict = {}
intermediates_dict = {}
if kwargs.get('charge_method',
False) and not metadata['embedding_charges']:
metadata['embedding_charges'] = driver_nbody_helper.compute_charges(
kwargs['charge_method'],
kwargs.get('charge_type', 'MULLIKEN_CHARGES').upper(), molecule)
for count, n in enumerate(compute_list.keys()):
core.print_out(
"\n ==> N-Body: Now computing %d-body complexes <==\n\n" % n)
total = len(compute_list[n])
for num, pair in enumerate(compute_list[n]):
core.print_out(
"\n N-Body: Computing complex (%d/%d) with fragments %s in the basis of fragments %s.\n\n"
% (num + 1, total, str(pair[0]), str(pair[1])))
ghost = list(set(pair[1]) - set(pair[0]))
current_mol = molecule.extract_subsets(list(pair[0]), ghost)
current_mol.set_name("%s_%i_%i" % (current_mol.name(), count, num))
if metadata['embedding_charges']:
driver_nbody_helper.electrostatic_embedding(metadata,
pair=pair)
# Save energies info
ptype_dict[pair], wfn = func(method_string,
molecule=current_mol,
return_wfn=True,
**kwargs)
core.set_global_option_python('EXTERN', None)
energies_dict[pair] = core.variable("CURRENT ENERGY")
gradients_dict[pair] = wfn.gradient()
var_key = "N-BODY (%s)@(%s) TOTAL ENERGY" % (', '.join(
[str(i)
for i in pair[0]]), ', '.join([str(i) for i in pair[1]]))
intermediates_dict[var_key] = core.variable("CURRENT ENERGY")
core.print_out(
"\n N-Body: Complex Energy (fragments = %s, basis = %s: %20.14f)\n"
% (str(pair[0]), str(pair[1]), energies_dict[pair]))
# Flip this off for now, needs more testing
#if 'cp' in bsse_type_list and (len(bsse_type_list) == 1):
# core.set_global_option('DF_INTS_IO', 'LOAD')
core.clean()
return {
'energies': energies_dict,
'gradients': gradients_dict,
'ptype': ptype_dict,
'intermediates': intermediates_dict
}
def _clean_psi_environ(do_clean):
if do_clean:
psi4.core.clean_variables()
psi4.core.clean_options()
core.clean()
def nbody_gufunc(func, method_string, **kwargs):
"""
Computes the nbody interaction energy, gradient, or Hessian depending on input.
This is a generalized univeral function for computing interaction quantities.
:returns: *return type of func* |w--w| The interaction data.
:returns: (*float*, :ref:`Wavefunction<sec:psimod_Wavefunction>`) |w--w| interaction data and wavefunction with energy/gradient/hessian set appropriately when **return_wfn** specified.
:type func: function
:param func: ``energy`` || etc.
Python function that accepts method_string and a molecule. Returns a
energy, gradient, or Hessian as requested.
:type method_string: string
:param method_string: ``'scf'`` || ``'mp2'`` || ``'ci5'`` || etc.
First argument, lowercase and usually unlabeled. Indicates the computational
method to be passed to func.
:type molecule: :ref:`molecule <op_py_molecule>`
:param molecule: ``h2o`` || etc.
The target molecule, if not the last molecule defined.
:type return_wfn: :ref:`boolean <op_py_boolean>`
:param return_wfn: ``'on'`` || |dl| ``'off'`` |dr|
Indicate to additionally return the :ref:`Wavefunction<sec:psimod_Wavefunction>`
calculation result as the second element of a tuple.
:type bsse_type: string or list
:param bsse_type: ``'cp'`` || ``['nocp', 'vmfc']`` || |dl| ``None`` |dr| || etc.
Type of BSSE correction to compute: CP, NoCP, or VMFC. The first in this
list is returned by this function. By default, this function is not called.
:type max_nbody: int
:param max_nbody: ``3`` || etc.
Maximum n-body to compute, cannot exceed the number of fragments in the moleucle.
:type ptype: string
:param ptype: ``'energy'`` || ``'gradient'`` || ``'hessian'``
Type of the procedure passed in.
:type return_total_data: :ref:`boolean <op_py_boolean>`
:param return_total_data: ``'on'`` || |dl| ``'off'`` |dr|
If True returns the total data (energy/gradient/etc) of the system,
otherwise returns interaction data.
"""
### ==> Parse some kwargs <==
kwargs = p4util.kwargs_lower(kwargs)
return_wfn = kwargs.pop('return_wfn', False)
ptype = kwargs.pop('ptype', None)
return_total_data = kwargs.pop('return_total_data', False)
molecule = kwargs.pop('molecule', core.get_active_molecule())
molecule.update_geometry()
core.clean_variables()
if ptype not in ['energy', 'gradient', 'hessian']:
raise ValidationError(
"""N-Body driver: The ptype '%s' is not regonized.""" % ptype)
# Figure out BSSE types
do_cp = False
do_nocp = False
do_vmfc = False
return_method = False
# Must be passed bsse_type
bsse_type_list = kwargs.pop('bsse_type')
if bsse_type_list is None:
raise ValidationError("N-Body GUFunc: Must pass a bsse_type")
if not isinstance(bsse_type_list, list):
bsse_type_list = [bsse_type_list]
for num, btype in enumerate(bsse_type_list):
if btype.lower() == 'cp':
do_cp = True
if (num == 0): return_method = 'cp'
elif btype.lower() == 'nocp':
do_nocp = True
if (num == 0): return_method = 'nocp'
elif btype.lower() == 'vmfc':
do_vmfc = True
if (num == 0): return_method = 'vmfc'
else:
raise ValidationError(
"N-Body GUFunc: bsse_type '%s' is not recognized" %
btype.lower())
max_nbody = kwargs.get('max_nbody', -1)
max_frag = molecule.nfragments()
if max_nbody == -1:
max_nbody = molecule.nfragments()
else:
max_nbody = min(max_nbody, max_frag)
# What levels do we need?
nbody_range = range(1, max_nbody + 1)
fragment_range = range(1, max_frag + 1)
# Flip this off for now, needs more testing
# If we are doing CP lets save them integrals
#if 'cp' in bsse_type_list and (len(bsse_type_list) == 1):
# # Set to save RI integrals for repeated full-basis computations
# ri_ints_io = core.get_global_option('DF_INTS_IO')
# # inquire if above at all applies to dfmp2 or just scf
# core.set_global_option('DF_INTS_IO', 'SAVE')
# psioh = core.IOManager.shared_object()
# psioh.set_specific_retention(97, True)
bsse_str = bsse_type_list[0]
if len(bsse_type_list) > 1:
bsse_str = str(bsse_type_list)
core.print_out("\n\n")
core.print_out(" ===> N-Body Interaction Abacus <===\n")
core.print_out(" BSSE Treatment: %s\n" %
bsse_str)
cp_compute_list = {x: set() for x in nbody_range}
nocp_compute_list = {x: set() for x in nbody_range}
vmfc_compute_list = {x: set() for x in nbody_range}
vmfc_level_list = {x: set()
for x in nbody_range
} # Need to sum something slightly different
# Build up compute sets
if do_cp:
# Everything is in dimer basis
basis_tuple = tuple(fragment_range)
for nbody in nbody_range:
for x in it.combinations(fragment_range, nbody):
cp_compute_list[nbody].add((x, basis_tuple))
if do_nocp:
# Everything in monomer basis
for nbody in nbody_range:
for x in it.combinations(fragment_range, nbody):
nocp_compute_list[nbody].add((x, x))
if do_vmfc:
# Like a CP for all combinations of pairs or greater
for nbody in nbody_range:
for cp_combos in it.combinations(fragment_range, nbody):
basis_tuple = tuple(cp_combos)
for interior_nbody in nbody_range:
for x in it.combinations(cp_combos, interior_nbody):
combo_tuple = (x, basis_tuple)
vmfc_compute_list[interior_nbody].add(combo_tuple)
vmfc_level_list[len(basis_tuple)].add(combo_tuple)
# Build a comprehensive compute_range
compute_list = {x: set() for x in nbody_range}
for n in nbody_range:
compute_list[n] |= cp_compute_list[n]
compute_list[n] |= nocp_compute_list[n]
compute_list[n] |= vmfc_compute_list[n]
core.print_out(" Number of %d-body computations: %d\n" %
(n, len(compute_list[n])))
# Build size and slices dictionaries
fragment_size_dict = {
frag: molecule.extract_subsets(frag).natom()
for frag in range(1, max_frag + 1)
}
start = 0
fragment_slice_dict = {}
for k, v in fragment_size_dict.items():
fragment_slice_dict[k] = slice(start, start + v)
start += v
molecule_total_atoms = sum(fragment_size_dict.values())
# Now compute the energies
energies_dict = {}
ptype_dict = {}
for n in compute_list.keys():
core.print_out(
"\n ==> N-Body: Now computing %d-body complexes <==\n\n" % n)
print("\n ==> N-Body: Now computing %d-body complexes <==\n" % n)
total = len(compute_list[n])
for num, pair in enumerate(compute_list[n]):
core.print_out(
"\n N-Body: Computing complex (%d/%d) with fragments %s in the basis of fragments %s.\n\n"
% (num + 1, total, str(pair[0]), str(pair[1])))
ghost = list(set(pair[1]) - set(pair[0]))
current_mol = molecule.extract_subsets(list(pair[0]), ghost)
ptype_dict[pair] = func(method_string,
molecule=current_mol,
**kwargs)
energies_dict[pair] = core.get_variable("CURRENT ENERGY")
core.print_out(
"\n N-Body: Complex Energy (fragments = %s, basis = %s: %20.14f)\n"
% (str(pair[0]), str(pair[1]), energies_dict[pair]))
# Flip this off for now, needs more testing
#if 'cp' in bsse_type_list and (len(bsse_type_list) == 1):
# core.set_global_option('DF_INTS_IO', 'LOAD')
core.clean()
# Final dictionaries
cp_energy_by_level = {n: 0.0 for n in nbody_range}
nocp_energy_by_level = {n: 0.0 for n in nbody_range}
cp_energy_body_dict = {n: 0.0 for n in nbody_range}
nocp_energy_body_dict = {n: 0.0 for n in nbody_range}
vmfc_energy_body_dict = {n: 0.0 for n in nbody_range}
# Build out ptype dictionaries if needed
if ptype != 'energy':
if ptype == 'gradient':
arr_shape = (molecule_total_atoms, 3)
elif ptype == 'hessian':
arr_shape = (molecule_total_atoms * 3, molecule_total_atoms * 3)
else:
raise KeyError("N-Body: ptype '%s' not recognized" % ptype)
cp_ptype_by_level = {n: np.zeros(arr_shape) for n in nbody_range}
nocp_ptype_by_level = {n: np.zeros(arr_shape) for n in nbody_range}
vmfc_ptype_by_level = {n: np.zeros(arr_shape) for n in nbody_range}
cp_ptype_body_dict = {n: np.zeros(arr_shape) for n in nbody_range}
nocp_ptype_body_dict = {n: np.zeros(arr_shape) for n in nbody_range}
vmfc_ptype_body_dict = {n: np.zeros(arr_shape) for n in nbody_range}
else:
cp_ptype_by_level, cp_ptype_body_dict = None, None
nocp_ptype_by_level, nocp_ptype_body_dict = None, None
vmfc_ptype_body_dict = None
# Sum up all of the levels
for n in nbody_range:
# Energy
cp_energy_by_level[n] = sum(energies_dict[v]
for v in cp_compute_list[n])
nocp_energy_by_level[n] = sum(energies_dict[v]
for v in nocp_compute_list[n])
# Special vmfc case
if n > 1:
vmfc_energy_body_dict[n] = vmfc_energy_body_dict[n - 1]
for tup in vmfc_level_list[n]:
vmfc_energy_body_dict[n] += (
(-1)**(n - len(tup[0]))) * energies_dict[tup]
# Do ptype
if ptype != 'energy':
_sum_cluster_ptype_data(ptype, ptype_dict, cp_compute_list[n],
fragment_slice_dict, fragment_size_dict,
cp_ptype_by_level[n])
_sum_cluster_ptype_data(ptype, ptype_dict, nocp_compute_list[n],
fragment_slice_dict, fragment_size_dict,
nocp_ptype_by_level[n])
_sum_cluster_ptype_data(ptype,
ptype_dict,
vmfc_level_list[n],
fragment_slice_dict,
fragment_size_dict,
vmfc_ptype_by_level[n],
vmfc=True)
# Compute cp energy and ptype
if do_cp:
for n in nbody_range:
if n == max_frag:
cp_energy_body_dict[n] = cp_energy_by_level[n]
if ptype != 'energy':
cp_ptype_body_dict[n][:] = cp_ptype_by_level[n]
continue
for k in range(1, n + 1):
take_nk = nCr(max_frag - k - 1, n - k)
sign = ((-1)**(n - k))
value = cp_energy_by_level[k]
cp_energy_body_dict[n] += take_nk * sign * value
if ptype != 'energy':
value = cp_ptype_by_level[k]
cp_ptype_body_dict[n] += take_nk * sign * value
_print_nbody_energy(cp_energy_body_dict, "Counterpoise Corrected (CP)")
cp_interaction_energy = cp_energy_body_dict[
max_nbody] - cp_energy_body_dict[1]
core.set_variable('Counterpoise Corrected Total Energy',
cp_energy_body_dict[max_nbody])
core.set_variable('Counterpoise Corrected Interaction Energy',
cp_interaction_energy)
for n in nbody_range[1:]:
var_key = 'CP-CORRECTED %d-BODY INTERACTION ENERGY' % n
core.set_variable(var_key,
cp_energy_body_dict[n] - cp_energy_body_dict[1])
# Compute nocp energy and ptype
if do_nocp:
for n in nbody_range:
if n == max_frag:
nocp_energy_body_dict[n] = nocp_energy_by_level[n]
if ptype != 'energy':
nocp_ptype_body_dict[n][:] = nocp_ptype_by_level[n]
continue
for k in range(1, n + 1):
take_nk = nCr(max_frag - k - 1, n - k)
sign = ((-1)**(n - k))
value = nocp_energy_by_level[k]
nocp_energy_body_dict[n] += take_nk * sign * value
if ptype != 'energy':
value = nocp_ptype_by_level[k]
nocp_ptype_body_dict[n] += take_nk * sign * value
_print_nbody_energy(nocp_energy_body_dict,
"Non-Counterpoise Corrected (NoCP)")
nocp_interaction_energy = nocp_energy_body_dict[
max_nbody] - nocp_energy_body_dict[1]
core.set_variable('Non-Counterpoise Corrected Total Energy',
nocp_energy_body_dict[max_nbody])
core.set_variable('Non-Counterpoise Corrected Interaction Energy',
nocp_interaction_energy)
for n in nbody_range[1:]:
var_key = 'NOCP-CORRECTED %d-BODY INTERACTION ENERGY' % n
core.set_variable(
var_key, nocp_energy_body_dict[n] - nocp_energy_body_dict[1])
# Compute vmfc energy and ptype
if do_vmfc:
_print_nbody_energy(vmfc_energy_body_dict,
"Valiron-Mayer Function Couterpoise (VMFC)")
vmfc_interaction_energy = vmfc_energy_body_dict[
max_nbody] - vmfc_energy_body_dict[1]
core.set_variable('Valiron-Mayer Function Couterpoise Total Energy',
vmfc_energy_body_dict[max_nbody])
core.set_variable(
'Valiron-Mayer Function Couterpoise Interaction Energy',
vmfc_interaction_energy)
for n in nbody_range[1:]:
var_key = 'VMFC-CORRECTED %d-BODY INTERACTION ENERGY' % n
core.set_variable(
var_key, vmfc_energy_body_dict[n] - vmfc_energy_body_dict[1])
if return_method == 'cp':
ptype_body_dict = cp_ptype_body_dict
energy_body_dict = cp_energy_body_dict
elif return_method == 'nocp':
ptype_body_dict = nocp_ptype_body_dict
energy_body_dict = nocp_energy_body_dict
elif return_method == 'vmfc':
ptype_body_dict = vmfc_ptype_body_dict
energy_body_dict = vmfc_energy_body_dict
else:
raise ValidationError(
"N-Body Wrapper: Invalid return type. Should never be here, please post this error on github."
)
# Figure out and build return types
if return_total_data:
ret_energy = energy_body_dict[max_nbody]
else:
ret_energy = energy_body_dict[max_nbody]
ret_energy -= energy_body_dict[1]
if ptype != 'energy':
if return_total_data:
np_final_ptype = ptype_body_dict[max_nbody].copy()
else:
np_final_ptype = ptype_body_dict[max_nbody].copy()
np_final_ptype -= ptype_body_dict[1]
ret_ptype = core.Matrix.from_array(np_final_ptype)
else:
ret_ptype = ret_energy
# Build and set a wavefunction
wfn = core.Wavefunction.build(molecule, 'sto-3g')
wfn.cdict["nbody_energy"] = energies_dict
wfn.cdict["nbody_ptype"] = ptype_dict
wfn.cdict["nbody_body_energy"] = energy_body_dict
wfn.cdict["nbody_body_ptype"] = ptype_body_dict
if ptype == 'gradient':
wfn.set_gradient(ret_ptype)
elif ptype == 'hessian':
wfn.set_hessian(ret_ptype)
core.set_variable("CURRENT ENERGY", ret_energy)
if return_wfn:
return (ret_ptype, wfn)
else:
return ret_ptype
def multi_level(func, **kwargs):
"""
Use different levels of theory for different expansion levels
See kwargs description in driver_nbody.nbody_gufunc
:returns: *return type of func* |w--w| The data.
:returns: (*float*, :py:class:`~psi4.core.Wavefunction`) |w--w| data and wavefunction with energy/gradient/hessian set appropriately when **return_wfn** specified.
"""
from psi4.driver.driver_nbody import nbody_gufunc
from psi4.driver.driver_nbody import _print_nbody_energy
ptype = kwargs['ptype']
return_wfn = kwargs.get('return_wfn', False)
kwargs['return_wfn'] = True
levels = kwargs.pop('levels')
for i in levels:
if isinstance(i, str): levels[i.lower()] = levels.pop(i)
supersystem = levels.pop('supersystem', False)
molecule = kwargs.get('molecule', core.get_active_molecule())
kwargs['bsse_type'] = [kwargs['bsse_type']] if isinstance(kwargs['bsse_type'], str) else kwargs['bsse_type']
natoms = molecule.natom()
# Initialize with zeros
energy_result, gradient_result, hessian_result = 0, None, None
energy_body_contribution = {b: {} for b in kwargs['bsse_type']}
energy_body_dict = {b: {} for b in kwargs['bsse_type']}
wfns = {}
if ptype in ['gradient', 'hessian']:
gradient_result = np.zeros((natoms, 3))
if ptype == 'hessian':
hessian_result = np.zeros((natoms * 3, natoms * 3))
if kwargs.get('charge_method', False) and not kwargs.get('embedding_charges', False):
kwargs['embedding_charges'] = compute_charges(kwargs['charge_method'],
kwargs.get('charge_type', 'MULLIKEN_CHARGES').upper(), molecule)
for n in sorted(levels)[::-1]:
molecule.set_name('%i' %n)
kwargs_copy = kwargs.copy()
kwargs_copy['max_nbody'] = n
energy_bsse_dict = {b: 0 for b in kwargs['bsse_type']}
if isinstance(levels[n], str):
# If a new level of theory is provided, compute contribution
ret, wfn = nbody_gufunc(func, levels[n], **kwargs_copy)
wfns[n] = wfn
else:
# For the n-body contribution, use available data from the higher order levels[n]-body
wfn = wfns[levels[n]]
for m in range(n - 1, n + 1):
if m == 0: continue
# Subtract the (n-1)-body contribution from the n-body contribution to get the n-body effect
sign = (-1)**(1 - m // n)
for b in kwargs['bsse_type']:
energy_bsse_dict[b] += sign * wfn.variable('%i%s' % (m, b.lower()))
if ptype in ['gradient', 'hessian']:
gradient_result += sign * np.array(wfn.variable('GRADIENT ' + str(m)))
# Keep 1-body contribution to compute interaction data
if n == 1:
gradient1 = np.array(wfn.variable('GRADIENT ' + str(m)))
if ptype == 'hessian':
hessian_result += sign * np.array(wfn.variable('HESSIAN ' + str(m)))
if n == 1:
hessian1 = np.array(wfn.variable('HESSIAN ' + str(m)))
energy_result += energy_bsse_dict[kwargs['bsse_type'][0]]
for b in kwargs['bsse_type']:
energy_body_contribution[b][n] = energy_bsse_dict[b]
if supersystem:
# Super system recovers higher order effects at a lower level
molecule.set_name('supersystem')
kwargs_copy = kwargs.copy()
kwargs_copy.pop('bsse_type')
kwargs_copy.pop('ptype')
ret, wfn_super = func(supersystem, **kwargs_copy)
core.clean()
kwargs_copy = kwargs.copy()
kwargs_copy['bsse_type'] = 'nocp'
kwargs_copy['max_nbody'] = max(levels)
# Subtract lower order effects to avoid double counting
ret, wfn = nbody_gufunc(func, supersystem, **kwargs_copy)
energy_result += wfn_super.energy() - wfn.variable(str(max(levels)))
for b in kwargs['bsse_type']:
energy_body_contribution[b][molecule.nfragments()] = wfn_super.energy() - wfn.variable(
str(max(levels)))
if ptype in ['gradient', 'hessian']:
gradient_result += np.array(wfn_super.gradient()) - np.array(wfn.variable('GRADIENT ' + str(max(levels))))
if ptype == 'hessian':
hessian_result += np.array(wfn_super.hessian()) - np.array(wfn.variable('HESSIAN ' + str(max(levels))))
levels['supersystem'] = supersystem
for b in kwargs['bsse_type']:
for n in energy_body_contribution[b]:
energy_body_dict[b][n] = sum(
[energy_body_contribution[b][i] for i in range(1, n + 1) if i in energy_body_contribution[b]])
is_embedded = kwargs.get('embedding_charges', False) or kwargs.get('charge_method', False)
for b in kwargs['bsse_type']:
_print_nbody_energy(energy_body_dict[b], '%s-corrected multilevel many-body expansion' % b.upper(),
is_embedded)
if not kwargs['return_total_data']:
# Remove monomer cotribution for interaction data
energy_result -= energy_body_dict[kwargs['bsse_type'][0]][1]
if ptype in ['gradient', 'hessian']:
gradient_result -= gradient1
if ptype == 'hessian':
hessian_result -= hessian1
wfn_out = core.Wavefunction.build(molecule, 'def2-svp')
core.set_variable("CURRENT ENERGY", energy_result)
wfn_out.set_variable("CURRENT ENERGY", energy_result)
gradient_result = core.Matrix.from_array(gradient_result) if gradient_result is not None else None
wfn_out.set_gradient(gradient_result)
hessian_result = core.Matrix.from_array(hessian_result) if hessian_result is not None else None
wfn_out.set_hessian(hessian_result)
ptype_result = eval(ptype + '_result')
for b in kwargs['bsse_type']:
for i in energy_body_dict[b]:
wfn_out.set_variable(str(i) + b, energy_body_dict[b][i])
if kwargs['return_wfn']:
return (ptype_result, wfn_out)
else:
return ptype_result
def run_gaussian_2(name, **kwargs):
# throw an exception for open-shells
if (core.get_option('SCF','REFERENCE') != 'RHF' ):
raise ValidationError("""g2 computations require "reference rhf".""")
# stash user options:
optstash = p4util.OptionsState(
['FNOCC','COMPUTE_TRIPLES'],
['FNOCC','COMPUTE_MP4_TRIPLES'],
['FREEZE_CORE'],
['MP2_TYPE'],
['SCF','SCF_TYPE'])
# override default scf_type
core.set_local_option('SCF','SCF_TYPE','PK')
# optimize geometry at scf level
core.clean()
core.set_global_option('BASIS',"6-31G(D)")
driver.optimize('scf')
core.clean()
# scf frequencies for zpe
# NOTE This line should not be needed, but without it there's a seg fault
scf_e, ref = driver.frequency('scf', return_wfn=True)
# thermodynamic properties
du = core.get_variable('INTERNAL ENERGY CORRECTION')
dh = core.get_variable('ENTHALPY CORRECTION')
dg = core.get_variable('GIBBS FREE ENERGY CORRECTION')
freqs = ref.frequencies()
nfreq = freqs.dim(0)
freqsum = 0.0
for i in range(0, nfreq):
freqsum += freqs.get(i)
zpe = freqsum / p4const.psi_hartree2wavenumbers * 0.8929 * 0.5
core.clean()
# optimize geometry at mp2 (no frozen core) level
# note: freeze_core isn't an option in MP2
core.set_global_option('FREEZE_CORE',"FALSE")
core.set_global_option('MP2_TYPE', 'CONV')
driver.optimize('mp2')
core.clean()
# qcisd(t)
core.set_local_option('FNOCC','COMPUTE_MP4_TRIPLES',"TRUE")
core.set_global_option('FREEZE_CORE',"TRUE")
core.set_global_option('BASIS',"6-311G(D_P)")
ref = driver.proc.run_fnocc('qcisd(t)', return_wfn=True, **kwargs)
# HLC: high-level correction based on number of valence electrons
nirrep = ref.nirrep()
frzcpi = ref.frzcpi()
nfzc = 0
for i in range (0,nirrep):
nfzc += frzcpi[i]
nalpha = ref.nalpha() - nfzc
nbeta = ref.nbeta() - nfzc
# hlc of gaussian-2
hlc = -0.00481 * nalpha -0.00019 * nbeta
# hlc of gaussian-1
hlc1 = -0.00614 * nalpha
eqci_6311gdp = core.get_variable("QCISD(T) TOTAL ENERGY")
emp4_6311gd = core.get_variable("MP4 TOTAL ENERGY")
emp2_6311gd = core.get_variable("MP2 TOTAL ENERGY")
core.clean()
# correction for diffuse functions
core.set_global_option('BASIS',"6-311+G(D_P)")
driver.energy('mp4')
emp4_6311pg_dp = core.get_variable("MP4 TOTAL ENERGY")
emp2_6311pg_dp = core.get_variable("MP2 TOTAL ENERGY")
core.clean()
# correction for polarization functions
core.set_global_option('BASIS',"6-311G(2DF_P)")
driver.energy('mp4')
emp4_6311g2dfp = core.get_variable("MP4 TOTAL ENERGY")
emp2_6311g2dfp = core.get_variable("MP2 TOTAL ENERGY")
core.clean()
# big basis mp2
core.set_global_option('BASIS',"6-311+G(3DF_2P)")
#run_fnocc('_mp2',**kwargs)
driver.energy('mp2')
emp2_big = core.get_variable("MP2 TOTAL ENERGY")
core.clean()
eqci = eqci_6311gdp
e_delta_g2 = emp2_big + emp2_6311gd - emp2_6311g2dfp - emp2_6311pg_dp
e_plus = emp4_6311pg_dp - emp4_6311gd
e_2df = emp4_6311g2dfp - emp4_6311gd
eg2 = eqci + e_delta_g2 + e_plus + e_2df
eg2_mp2_0k = eqci + (emp2_big - emp2_6311gd) + hlc + zpe
core.print_out('\n')
core.print_out(' ==> G1/G2 Energy Components <==\n')
core.print_out('\n')
core.print_out(' QCISD(T): %20.12lf\n' % eqci)
core.print_out(' E(Delta): %20.12lf\n' % e_delta_g2)
core.print_out(' E(2DF): %20.12lf\n' % e_2df)
core.print_out(' E(+): %20.12lf\n' % e_plus)
core.print_out(' E(G1 HLC): %20.12lf\n' % hlc1)
core.print_out(' E(G2 HLC): %20.12lf\n' % hlc)
core.print_out(' E(ZPE): %20.12lf\n' % zpe)
core.print_out('\n')
core.print_out(' ==> 0 Kelvin Results <==\n')
core.print_out('\n')
eg2_0k = eg2 + zpe + hlc
core.print_out(' G1: %20.12lf\n' % (eqci + e_plus + e_2df + hlc1 + zpe))
core.print_out(' G2(MP2): %20.12lf\n' % eg2_mp2_0k)
core.print_out(' G2: %20.12lf\n' % eg2_0k)
core.set_variable("G1 TOTAL ENERGY",eqci + e_plus + e_2df + hlc1 + zpe)
core.set_variable("G2 TOTAL ENERGY",eg2_0k)
core.set_variable("G2(MP2) TOTAL ENERGY",eg2_mp2_0k)
core.print_out('\n')
T = core.get_global_option('T')
core.print_out(' ==> %3.0lf Kelvin Results <==\n'% T)
core.print_out('\n')
internal_energy = eg2_mp2_0k + du - zpe / 0.8929
enthalpy = eg2_mp2_0k + dh - zpe / 0.8929
gibbs = eg2_mp2_0k + dg - zpe / 0.8929
core.print_out(' G2(MP2) energy: %20.12lf\n' % internal_energy )
core.print_out(' G2(MP2) enthalpy: %20.12lf\n' % enthalpy)
core.print_out(' G2(MP2) free energy: %20.12lf\n' % gibbs)
core.print_out('\n')
core.set_variable("G2(MP2) INTERNAL ENERGY",internal_energy)
core.set_variable("G2(MP2) ENTHALPY",enthalpy)
core.set_variable("G2(MP2) FREE ENERGY",gibbs)
internal_energy = eg2_0k + du - zpe / 0.8929
enthalpy = eg2_0k + dh - zpe / 0.8929
gibbs = eg2_0k + dg - zpe / 0.8929
core.print_out(' G2 energy: %20.12lf\n' % internal_energy )
core.print_out(' G2 enthalpy: %20.12lf\n' % enthalpy)
core.print_out(' G2 free energy: %20.12lf\n' % gibbs)
core.set_variable("CURRENT ENERGY",eg2_0k)
core.set_variable("G2 INTERNAL ENERGY",internal_energy)
core.set_variable("G2 ENTHALPY",enthalpy)
core.set_variable("G2 FREE ENERGY",gibbs)
core.clean()
optstash.restore()
# return 0K g2 results
return eg2_0k
def multi_level(func, **kwargs):
"""
Use different levels of theory for different expansion levels
See kwargs description in driver_nbody.nbody_gufunc
:returns: *return type of func* |w--w| The data.
:returns: (*float*, :py:class:`~psi4.core.Wavefunction`) |w--w| data and wavefunction with energy/gradient/hessian set appropriately when **return_wfn** specified.
"""
from psi4.driver.driver_nbody import _print_nbody_energy, nbody_gufunc
ptype = kwargs['ptype']
return_wfn = kwargs.get('return_wfn', False)
kwargs['return_wfn'] = True
levels = {}
for k, v in kwargs.pop('levels').items():
if isinstance(k, str):
levels[k.lower()] = v
else:
levels[k] = v
supersystem = levels.pop('supersystem', False)
molecule = kwargs.get('molecule', core.get_active_molecule())
kwargs['bsse_type'] = [kwargs['bsse_type']] if isinstance(kwargs['bsse_type'], str) else kwargs['bsse_type']
natoms = molecule.natom()
# Initialize with zeros
energy_result, gradient_result, hessian_result = 0, None, None
energy_body_contribution = {b: {} for b in kwargs['bsse_type']}
energy_body_dict = {b: {} for b in kwargs['bsse_type']}
wfns = {}
if ptype in ['gradient', 'hessian']:
gradient_result = np.zeros((natoms, 3))
if ptype == 'hessian':
hessian_result = np.zeros((natoms * 3, natoms * 3))
if kwargs.get('charge_method', False) and not kwargs.get('embedding_charges', False):
kwargs['embedding_charges'] = compute_charges(kwargs['charge_method'],
kwargs.get('charge_type', 'MULLIKEN_CHARGES').upper(), molecule)
for n in sorted(levels)[::-1]:
molecule.set_name('%i' % n)
kwargs_copy = kwargs.copy()
kwargs_copy['max_nbody'] = n
energy_bsse_dict = {b: 0 for b in kwargs['bsse_type']}
if isinstance(levels[n], str):
# If a new level of theory is provided, compute contribution
ret, wfn = nbody_gufunc(func, levels[n], **kwargs_copy)
wfns[n] = wfn
else:
# For the n-body contribution, use available data from the higher order levels[n]-body
wfn = wfns[levels[n]]
for m in range(n - 1, n + 1):
if m == 0: continue
# Subtract the (n-1)-body contribution from the n-body contribution to get the n-body effect
sign = (-1)**(1 - m // n)
for b in kwargs['bsse_type']:
energy_bsse_dict[b] += sign * wfn.variable('%i%s' % (m, b.lower()))
if ptype in ['gradient', 'hessian']:
gradient_result += sign * np.array(wfn.variable('GRADIENT ' + str(m)))
# Keep 1-body contribution to compute interaction data
if n == 1:
gradient1 = np.array(wfn.variable('GRADIENT ' + str(m)))
if ptype == 'hessian':
hessian_result += sign * np.array(wfn.variable('HESSIAN ' + str(m)))
if n == 1:
hessian1 = np.array(wfn.variable('HESSIAN ' + str(m)))
energy_result += energy_bsse_dict[kwargs['bsse_type'][0]]
for b in kwargs['bsse_type']:
energy_body_contribution[b][n] = energy_bsse_dict[b]
if supersystem:
# Super system recovers higher order effects at a lower level
molecule.set_name('supersystem')
kwargs_copy = kwargs.copy()
kwargs_copy.pop('bsse_type')
kwargs_copy.pop('ptype')
ret, wfn_super = func(supersystem, **kwargs_copy)
core.clean()
kwargs_copy = kwargs.copy()
kwargs_copy['bsse_type'] = 'nocp'
kwargs_copy['max_nbody'] = max(levels)
# Subtract lower order effects to avoid double counting
ret, wfn = nbody_gufunc(func, supersystem, **kwargs_copy)
energy_result += wfn_super.energy() - wfn.variable(str(max(levels)))
for b in kwargs['bsse_type']:
energy_body_contribution[b][molecule.nfragments()] = wfn_super.energy() - wfn.variable(
str(max(levels)))
if ptype in ['gradient', 'hessian']:
gradient_result += np.array(wfn_super.gradient()) - np.array(wfn.variable('GRADIENT ' + str(max(levels))))
if ptype == 'hessian':
hessian_result += np.array(wfn_super.hessian()) - np.array(wfn.variable('HESSIAN ' + str(max(levels))))
levels['supersystem'] = supersystem
for b in kwargs['bsse_type']:
for n in energy_body_contribution[b]:
energy_body_dict[b][n] = sum(
[energy_body_contribution[b][i] for i in range(1, n + 1) if i in energy_body_contribution[b]])
is_embedded = kwargs.get('embedding_charges', False) or kwargs.get('charge_method', False)
for b in kwargs['bsse_type']:
_print_nbody_energy(energy_body_dict[b], '%s-corrected multilevel many-body expansion' % b.upper(),
is_embedded)
if not kwargs['return_total_data']:
# Remove monomer contribution for interaction data
energy_result -= energy_body_dict[kwargs['bsse_type'][0]][1]
if ptype in ['gradient', 'hessian']:
gradient_result -= gradient1
if ptype == 'hessian':
hessian_result -= hessian1
wfn_out = core.Wavefunction.build(molecule, 'def2-svp')
core.set_variable("CURRENT ENERGY", energy_result)
wfn_out.set_variable("CURRENT ENERGY", energy_result)
if gradient_result is not None:
wfn_out.set_gradient(core.Matrix.from_array(gradient_result))
if hessian_result is not None:
wfn_out.set_hessian(core.Matrix.from_array(hessian_result) )
ptype_result = eval(ptype + '_result')
for b in kwargs['bsse_type']:
for i in energy_body_dict[b]:
wfn_out.set_variable(str(i) + b, energy_body_dict[b][i])
if kwargs['return_wfn']:
return (ptype_result, wfn_out)
else:
return ptype_result
def nbody_gufunc(func, method_string, **kwargs):
"""
Computes the nbody interaction energy, gradient, or Hessian depending on input.
This is a generalized univeral function for computing interaction quantities.
:returns: *return type of func* |w--w| The interaction data.
:returns: (*float*, :py:class:`~psi4.core.Wavefunction`) |w--w| interaction data and wavefunction with energy/gradient/hessian set appropriately when **return_wfn** specified.
:type func: function
:param func: ``energy`` || etc.
Python function that accepts method_string and a molecule. Returns a
energy, gradient, or Hessian as requested.
:type method_string: string
:param method_string: ``'scf'`` || ``'mp2'`` || ``'ci5'`` || etc.
First argument, lowercase and usually unlabeled. Indicates the computational
method to be passed to func.
:type molecule: :ref:`molecule <op_py_molecule>`
:param molecule: ``h2o`` || etc.
The target molecule, if not the last molecule defined.
:type return_wfn: :ref:`boolean <op_py_boolean>`
:param return_wfn: ``'on'`` || |dl| ``'off'`` |dr|
Indicate to additionally return the :py:class:`~psi4.core.Wavefunction`
calculation result as the second element of a tuple.
:type bsse_type: string or list
:param bsse_type: ``'cp'`` || ``['nocp', 'vmfc']`` || |dl| ``None`` |dr| || etc.
Type of BSSE correction to compute: CP, NoCP, or VMFC. The first in this
list is returned by this function. By default, this function is not called.
:type max_nbody: int
:param max_nbody: ``3`` || etc.
Maximum n-body to compute, cannot exceed the number of fragments in the moleucle.
:type ptype: string
:param ptype: ``'energy'`` || ``'gradient'`` || ``'hessian'``
Type of the procedure passed in.
:type return_total_data: :ref:`boolean <op_py_boolean>`
:param return_total_data: ``'on'`` || |dl| ``'off'`` |dr|
If True returns the total data (energy/gradient/etc) of the system,
otherwise returns interaction data.
"""
### ==> Parse some kwargs <==
kwargs = p4util.kwargs_lower(kwargs)
return_wfn = kwargs.pop('return_wfn', False)
ptype = kwargs.pop('ptype', None)
return_total_data = kwargs.pop('return_total_data', False)
molecule = kwargs.pop('molecule', core.get_active_molecule())
molecule.update_geometry()
core.clean_variables()
if ptype not in ['energy', 'gradient', 'hessian']:
raise ValidationError("""N-Body driver: The ptype '%s' is not regonized.""" % ptype)
# Figure out BSSE types
do_cp = False
do_nocp = False
do_vmfc = False
return_method = False
# Must be passed bsse_type
bsse_type_list = kwargs.pop('bsse_type')
if bsse_type_list is None:
raise ValidationError("N-Body GUFunc: Must pass a bsse_type")
if not isinstance(bsse_type_list, list):
bsse_type_list = [bsse_type_list]
for num, btype in enumerate(bsse_type_list):
if btype.lower() == 'cp':
do_cp = True
if (num == 0): return_method = 'cp'
elif btype.lower() == 'nocp':
do_nocp = True
if (num == 0): return_method = 'nocp'
elif btype.lower() == 'vmfc':
do_vmfc = True
if (num == 0): return_method = 'vmfc'
else:
raise ValidationError("N-Body GUFunc: bsse_type '%s' is not recognized" % btype.lower())
max_nbody = kwargs.get('max_nbody', -1)
max_frag = molecule.nfragments()
if max_nbody == -1:
max_nbody = molecule.nfragments()
else:
max_nbody = min(max_nbody, max_frag)
# What levels do we need?
nbody_range = range(1, max_nbody + 1)
fragment_range = range(1, max_frag + 1)
# Flip this off for now, needs more testing
# If we are doing CP lets save them integrals
#if 'cp' in bsse_type_list and (len(bsse_type_list) == 1):
# # Set to save RI integrals for repeated full-basis computations
# ri_ints_io = core.get_global_option('DF_INTS_IO')
# # inquire if above at all applies to dfmp2 or just scf
# core.set_global_option('DF_INTS_IO', 'SAVE')
# psioh = core.IOManager.shared_object()
# psioh.set_specific_retention(97, True)
bsse_str = bsse_type_list[0]
if len(bsse_type_list) >1:
bsse_str = str(bsse_type_list)
core.print_out("\n\n")
core.print_out(" ===> N-Body Interaction Abacus <===\n")
core.print_out(" BSSE Treatment: %s\n" % bsse_str)
cp_compute_list = {x:set() for x in nbody_range}
nocp_compute_list = {x:set() for x in nbody_range}
vmfc_compute_list = {x:set() for x in nbody_range}
vmfc_level_list = {x:set() for x in nbody_range} # Need to sum something slightly different
# Build up compute sets
if do_cp:
# Everything is in dimer basis
basis_tuple = tuple(fragment_range)
for nbody in nbody_range:
for x in it.combinations(fragment_range, nbody):
cp_compute_list[nbody].add( (x, basis_tuple) )
if do_nocp:
# Everything in monomer basis
for nbody in nbody_range:
for x in it.combinations(fragment_range, nbody):
nocp_compute_list[nbody].add( (x, x) )
if do_vmfc:
# Like a CP for all combinations of pairs or greater
for nbody in nbody_range:
for cp_combos in it.combinations(fragment_range, nbody):
basis_tuple = tuple(cp_combos)
for interior_nbody in nbody_range:
for x in it.combinations(cp_combos, interior_nbody):
combo_tuple = (x, basis_tuple)
vmfc_compute_list[interior_nbody].add( combo_tuple )
vmfc_level_list[len(basis_tuple)].add( combo_tuple )
# Build a comprehensive compute_range
compute_list = {x:set() for x in nbody_range}
for n in nbody_range:
compute_list[n] |= cp_compute_list[n]
compute_list[n] |= nocp_compute_list[n]
compute_list[n] |= vmfc_compute_list[n]
core.print_out(" Number of %d-body computations: %d\n" % (n, len(compute_list[n])))
# Build size and slices dictionaries
fragment_size_dict = {frag: molecule.extract_subsets(frag).natom() for
frag in range(1, max_frag+1)}
start = 0
fragment_slice_dict = {}
for k, v in fragment_size_dict.items():
fragment_slice_dict[k] = slice(start, start + v)
start += v
molecule_total_atoms = sum(fragment_size_dict.values())
# Now compute the energies
energies_dict = {}
ptype_dict = {}
for n in compute_list.keys():
core.print_out("\n ==> N-Body: Now computing %d-body complexes <==\n\n" % n)
total = len(compute_list[n])
for num, pair in enumerate(compute_list[n]):
core.print_out("\n N-Body: Computing complex (%d/%d) with fragments %s in the basis of fragments %s.\n\n" %
(num + 1, total, str(pair[0]), str(pair[1])))
ghost = list(set(pair[1]) - set(pair[0]))
current_mol = molecule.extract_subsets(list(pair[0]), ghost)
ptype_dict[pair] = func(method_string, molecule=current_mol, **kwargs)
energies_dict[pair] = core.get_variable("CURRENT ENERGY")
core.print_out("\n N-Body: Complex Energy (fragments = %s, basis = %s: %20.14f)\n" %
(str(pair[0]), str(pair[1]), energies_dict[pair]))
# Flip this off for now, needs more testing
#if 'cp' in bsse_type_list and (len(bsse_type_list) == 1):
# core.set_global_option('DF_INTS_IO', 'LOAD')
core.clean()
# Final dictionaries
cp_energy_by_level = {n: 0.0 for n in nbody_range}
nocp_energy_by_level = {n: 0.0 for n in nbody_range}
cp_energy_body_dict = {n: 0.0 for n in nbody_range}
nocp_energy_body_dict = {n: 0.0 for n in nbody_range}
vmfc_energy_body_dict = {n: 0.0 for n in nbody_range}
# Build out ptype dictionaries if needed
if ptype != 'energy':
if ptype == 'gradient':
arr_shape = (molecule_total_atoms, 3)
elif ptype == 'hessian':
arr_shape = (molecule_total_atoms * 3, molecule_total_atoms * 3)
else:
raise KeyError("N-Body: ptype '%s' not recognized" % ptype)
cp_ptype_by_level = {n: np.zeros(arr_shape) for n in nbody_range}
nocp_ptype_by_level = {n: np.zeros(arr_shape) for n in nbody_range}
vmfc_ptype_by_level = {n: np.zeros(arr_shape) for n in nbody_range}
cp_ptype_body_dict = {n: np.zeros(arr_shape) for n in nbody_range}
nocp_ptype_body_dict = {n: np.zeros(arr_shape) for n in nbody_range}
vmfc_ptype_body_dict = {n: np.zeros(arr_shape) for n in nbody_range}
else:
cp_ptype_by_level, cp_ptype_body_dict = None, None
nocp_ptype_by_level, nocp_ptype_body_dict = None, None
vmfc_ptype_body_dict = None
# Sum up all of the levels
for n in nbody_range:
# Energy
cp_energy_by_level[n] = sum(energies_dict[v] for v in cp_compute_list[n])
nocp_energy_by_level[n] = sum(energies_dict[v] for v in nocp_compute_list[n])
# Special vmfc case
if n > 1:
vmfc_energy_body_dict[n] = vmfc_energy_body_dict[n - 1]
for tup in vmfc_level_list[n]:
vmfc_energy_body_dict[n] += ((-1) ** (n - len(tup[0]))) * energies_dict[tup]
# Do ptype
if ptype != 'energy':
_sum_cluster_ptype_data(ptype, ptype_dict, cp_compute_list[n],
fragment_slice_dict, fragment_size_dict,
cp_ptype_by_level[n])
_sum_cluster_ptype_data(ptype, ptype_dict, nocp_compute_list[n],
fragment_slice_dict, fragment_size_dict,
nocp_ptype_by_level[n])
_sum_cluster_ptype_data(ptype, ptype_dict, vmfc_level_list[n],
fragment_slice_dict, fragment_size_dict,
vmfc_ptype_by_level[n], vmfc=True)
# Compute cp energy and ptype
if do_cp:
for n in nbody_range:
if n == max_frag:
cp_energy_body_dict[n] = cp_energy_by_level[n]
if ptype != 'energy':
cp_ptype_body_dict[n][:] = cp_ptype_by_level[n]
continue
for k in range(1, n + 1):
take_nk = nCr(max_frag - k - 1, n - k)
sign = ((-1) ** (n - k))
value = cp_energy_by_level[k]
cp_energy_body_dict[n] += take_nk * sign * value
if ptype != 'energy':
value = cp_ptype_by_level[k]
cp_ptype_body_dict[n] += take_nk * sign * value
_print_nbody_energy(cp_energy_body_dict, "Counterpoise Corrected (CP)")
cp_interaction_energy = cp_energy_body_dict[max_nbody] - cp_energy_body_dict[1]
core.set_variable('Counterpoise Corrected Total Energy', cp_energy_body_dict[max_nbody])
core.set_variable('Counterpoise Corrected Interaction Energy', cp_interaction_energy)
for n in nbody_range[1:]:
var_key = 'CP-CORRECTED %d-BODY INTERACTION ENERGY' % n
core.set_variable(var_key, cp_energy_body_dict[n] - cp_energy_body_dict[1])
# Compute nocp energy and ptype
if do_nocp:
for n in nbody_range:
if n == max_frag:
nocp_energy_body_dict[n] = nocp_energy_by_level[n]
if ptype != 'energy':
nocp_ptype_body_dict[n][:] = nocp_ptype_by_level[n]
continue
for k in range(1, n + 1):
take_nk = nCr(max_frag - k - 1, n - k)
sign = ((-1) ** (n - k))
value = nocp_energy_by_level[k]
nocp_energy_body_dict[n] += take_nk * sign * value
if ptype != 'energy':
value = nocp_ptype_by_level[k]
nocp_ptype_body_dict[n] += take_nk * sign * value
_print_nbody_energy(nocp_energy_body_dict, "Non-Counterpoise Corrected (NoCP)")
nocp_interaction_energy = nocp_energy_body_dict[max_nbody] - nocp_energy_body_dict[1]
core.set_variable('Non-Counterpoise Corrected Total Energy', nocp_energy_body_dict[max_nbody])
core.set_variable('Non-Counterpoise Corrected Interaction Energy', nocp_interaction_energy)
for n in nbody_range[1:]:
var_key = 'NOCP-CORRECTED %d-BODY INTERACTION ENERGY' % n
core.set_variable(var_key, nocp_energy_body_dict[n] - nocp_energy_body_dict[1])
# Compute vmfc energy and ptype
if do_vmfc:
_print_nbody_energy(vmfc_energy_body_dict, "Valiron-Mayer Function Couterpoise (VMFC)")
vmfc_interaction_energy = vmfc_energy_body_dict[max_nbody] - vmfc_energy_body_dict[1]
core.set_variable('Valiron-Mayer Function Couterpoise Total Energy', vmfc_energy_body_dict[max_nbody])
core.set_variable('Valiron-Mayer Function Couterpoise Interaction Energy', vmfc_interaction_energy)
for n in nbody_range[1:]:
var_key = 'VMFC-CORRECTED %d-BODY INTERACTION ENERGY' % n
core.set_variable(var_key, vmfc_energy_body_dict[n] - vmfc_energy_body_dict[1])
if return_method == 'cp':
ptype_body_dict = cp_ptype_body_dict
energy_body_dict = cp_energy_body_dict
elif return_method == 'nocp':
ptype_body_dict = nocp_ptype_body_dict
energy_body_dict = nocp_energy_body_dict
elif return_method == 'vmfc':
ptype_body_dict = vmfc_ptype_body_dict
energy_body_dict = vmfc_energy_body_dict
else:
raise ValidationError("N-Body Wrapper: Invalid return type. Should never be here, please post this error on github.")
# Figure out and build return types
if return_total_data:
ret_energy = energy_body_dict[max_nbody]
else:
ret_energy = energy_body_dict[max_nbody]
ret_energy -= energy_body_dict[1]
if ptype != 'energy':
if return_total_data:
np_final_ptype = ptype_body_dict[max_nbody].copy()
else:
np_final_ptype = ptype_body_dict[max_nbody].copy()
np_final_ptype -= ptype_body_dict[1]
ret_ptype = core.Matrix.from_array(np_final_ptype)
else:
ret_ptype = ret_energy
# Build and set a wavefunction
wfn = core.Wavefunction.build(molecule, 'sto-3g')
wfn.nbody_energy = energies_dict
wfn.nbody_ptype = ptype_dict
wfn.nbody_body_energy = energy_body_dict
wfn.nbody_body_ptype = ptype_body_dict
if ptype == 'gradient':
wfn.set_gradient(ret_ptype)
elif ptype == 'hessian':
wfn.set_hessian(ret_ptype)
core.set_variable("CURRENT ENERGY", ret_energy)
if return_wfn:
return (ret_ptype, wfn)
else:
return ret_ptype
def _clean_psi_environ(do_clean):
if do_clean:
psi4.core.clean_variables()
psi4.core.clean_options()
core.clean()
def run_gaussian_2(name, **kwargs):
# throw an exception for open-shells
if (core.get_option('SCF', 'REFERENCE') != 'RHF'):
raise ValidationError("""g2 computations require "reference rhf".""")
# stash user options:
optstash = p4util.OptionsState(['FNOCC', 'COMPUTE_TRIPLES'],
['FNOCC', 'COMPUTE_MP4_TRIPLES'], ['BASIS'],
['FREEZE_CORE'], ['MP2_TYPE'], ['SCF_TYPE'])
# override default scf_type
core.set_global_option('SCF_TYPE', 'PK')
# optimize geometry at scf level
core.clean()
core.set_global_option('BASIS', "6-31G(D)")
driver.optimize('scf')
core.clean()
# scf frequencies for zpe
# NOTE This line should not be needed, but without it there's a seg fault
scf_e, ref = driver.frequency('scf', return_wfn=True)
# thermodynamic properties
du = core.variable('THERMAL ENERGY CORRECTION')
dh = core.variable('ENTHALPY CORRECTION')
dg = core.variable('GIBBS FREE ENERGY CORRECTION')
freqs = ref.frequencies()
nfreq = freqs.dim(0)
freqsum = 0.0
for i in range(0, nfreq):
freqsum += freqs.get(i)
zpe = freqsum / constants.hartree2wavenumbers * 0.8929 * 0.5
core.clean()
# optimize geometry at mp2 (no frozen core) level
# note: freeze_core isn't an option in MP2
core.set_global_option('FREEZE_CORE', "FALSE")
core.set_global_option('MP2_TYPE', 'CONV')
driver.optimize('mp2')
core.clean()
# qcisd(t)
core.set_local_option('FNOCC', 'COMPUTE_MP4_TRIPLES', "TRUE")
core.set_global_option('FREEZE_CORE', "TRUE")
core.set_global_option('BASIS', "6-311G(D_P)")
ref = driver.proc.run_fnocc('qcisd(t)', return_wfn=True, **kwargs)
# HLC: high-level correction based on number of valence electrons
nirrep = ref.nirrep()
frzcpi = ref.frzcpi()
nfzc = 0
for i in range(0, nirrep):
nfzc += frzcpi[i]
nalpha = ref.nalpha() - nfzc
nbeta = ref.nbeta() - nfzc
# hlc of gaussian-2
hlc = -0.00481 * nalpha - 0.00019 * nbeta
# hlc of gaussian-1
hlc1 = -0.00614 * nalpha
eqci_6311gdp = core.variable("QCISD(T) TOTAL ENERGY")
emp4_6311gd = core.variable("MP4 TOTAL ENERGY")
emp2_6311gd = core.variable("MP2 TOTAL ENERGY")
core.clean()
# correction for diffuse functions
core.set_global_option('BASIS', "6-311+G(D_P)")
driver.energy('mp4')
emp4_6311pg_dp = core.variable("MP4 TOTAL ENERGY")
emp2_6311pg_dp = core.variable("MP2 TOTAL ENERGY")
core.clean()
# correction for polarization functions
core.set_global_option('BASIS', "6-311G(2DF_P)")
driver.energy('mp4')
emp4_6311g2dfp = core.variable("MP4 TOTAL ENERGY")
emp2_6311g2dfp = core.variable("MP2 TOTAL ENERGY")
core.clean()
# big basis mp2
core.set_global_option('BASIS', "6-311+G(3DF_2P)")
#run_fnocc('_mp2',**kwargs)
driver.energy('mp2')
emp2_big = core.variable("MP2 TOTAL ENERGY")
core.clean()
eqci = eqci_6311gdp
e_delta_g2 = emp2_big + emp2_6311gd - emp2_6311g2dfp - emp2_6311pg_dp
e_plus = emp4_6311pg_dp - emp4_6311gd
e_2df = emp4_6311g2dfp - emp4_6311gd
eg2 = eqci + e_delta_g2 + e_plus + e_2df
eg2_mp2_0k = eqci + (emp2_big - emp2_6311gd) + hlc + zpe
core.print_out('\n')
core.print_out(' ==> G1/G2 Energy Components <==\n')
core.print_out('\n')
core.print_out(' QCISD(T): %20.12lf\n' % eqci)
core.print_out(' E(Delta): %20.12lf\n' % e_delta_g2)
core.print_out(' E(2DF): %20.12lf\n' % e_2df)
core.print_out(' E(+): %20.12lf\n' % e_plus)
core.print_out(' E(G1 HLC): %20.12lf\n' % hlc1)
core.print_out(' E(G2 HLC): %20.12lf\n' % hlc)
core.print_out(' E(ZPE): %20.12lf\n' % zpe)
core.print_out('\n')
core.print_out(' ==> 0 Kelvin Results <==\n')
core.print_out('\n')
eg2_0k = eg2 + zpe + hlc
core.print_out(' G1: %20.12lf\n' %
(eqci + e_plus + e_2df + hlc1 + zpe))
core.print_out(' G2(MP2): %20.12lf\n' % eg2_mp2_0k)
core.print_out(' G2: %20.12lf\n' % eg2_0k)
core.set_variable("G1 TOTAL ENERGY", eqci + e_plus + e_2df + hlc1 + zpe)
core.set_variable("G2 TOTAL ENERGY", eg2_0k)
core.set_variable("G2(MP2) TOTAL ENERGY", eg2_mp2_0k)
core.print_out('\n')
T = core.get_global_option('T')
core.print_out(' ==> %3.0lf Kelvin Results <==\n' % T)
core.print_out('\n')
internal_energy = eg2_mp2_0k + du - zpe / 0.8929
enthalpy = eg2_mp2_0k + dh - zpe / 0.8929
gibbs = eg2_mp2_0k + dg - zpe / 0.8929
core.print_out(' G2(MP2) energy: %20.12lf\n' % internal_energy)
core.print_out(' G2(MP2) enthalpy: %20.12lf\n' % enthalpy)
core.print_out(' G2(MP2) free energy: %20.12lf\n' % gibbs)
core.print_out('\n')
core.set_variable("G2(MP2) INTERNAL ENERGY", internal_energy)
core.set_variable("G2(MP2) ENTHALPY", enthalpy)
core.set_variable("G2(MP2) FREE ENERGY", gibbs)
internal_energy = eg2_0k + du - zpe / 0.8929
enthalpy = eg2_0k + dh - zpe / 0.8929
gibbs = eg2_0k + dg - zpe / 0.8929
core.print_out(' G2 energy: %20.12lf\n' % internal_energy)
core.print_out(' G2 enthalpy: %20.12lf\n' % enthalpy)
core.print_out(' G2 free energy: %20.12lf\n' % gibbs)
core.set_variable("CURRENT ENERGY", eg2_0k)
core.set_variable("G2 INTERNAL ENERGY", internal_energy)
core.set_variable("G2 ENTHALPY", enthalpy)
core.set_variable("G2 FREE ENERGY", gibbs)
core.clean()
optstash.restore()
# return 0K g2 results
return eg2_0k
def __init__(self,
molecule,
basis,
numpy_memory=2.e9,
scf_type="PK",
use_c=False):
# Set defaults
maxiter = 40
E_conv = 1.0E-6
D_conv = 1.0E-3
# Integral generation from Psi4's MintsHelper
start_time = time.time()
self.basis_name = basis
self.molecule = molecule
self.basis = pc.BasisSet.build(self.molecule, "ORBITAL", basis)
self.mints = pc.MintsHelper(self.basis)
self.S = np.asarray(self.mints.ao_overlap())
# Get nbf and ndocc for closed shell molecules
self.nbf = self.S.shape[0]
self.nel = sum(
self.molecule.Z(n) for n in range(self.molecule.natom()))
self.nel -= self.molecule.molecular_charge()
if not (self.nel / 2.0).is_integer():
raise ValueError(
"RHF: Molecule did not have an even number of electrons!")
self.ndocc = int(self.nel / 2.0)
print('\nNumber of occupied orbitals: %d' % self.ndocc)
print('Number of basis functions: %d' % self.nbf)
# Run a quick check to make sure everything will fit into memory
I_Size = (self.nbf**4) * 8.e-9
print("\nSize of the ERI tensor will be %4.2f GB." % I_Size)
# Estimate memory usage
memory_footprint = I_Size * 1.5
if I_Size > numpy_memory:
pc.clean()
raise Exception(
"Estimated memory utilization (%4.2f GB) exceeds numpy_memory \
limit of %4.2f GB." %
(memory_footprint, numpy_memory))
# Compute required quantities for SCF
self.V = np.asarray(self.mints.ao_potential())
self.T = np.asarray(self.mints.ao_kinetic())
# self.I = np.asarray(self.mints.ao_eri())
self.JK = jk.build_JK(self.molecule, self.basis_name, scf_type, use_c)
self.Enuc = self.molecule.nuclear_repulsion_energy()
print('\nTotal time taken for integrals: %.3f seconds.' %
(time.time() - start_time))
t = time.time()
# Build H_core
self.H = self.T + self.V
# Orthogonalizer A = S^(-1/2) using Psi4's matrix power.
A = self.mints.ao_overlap()
A.power(-0.5, 1.e-16)
self.A = np.asarray(A)
print('\nTotal time taken for setup: %.3f seconds' %
(time.time() - start_time))