/usr/share/psi/python/qcdb/molecule.py is in psi4-data 1:0.3-5.
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#@BEGIN LICENSE
#
# PSI4: an ab initio quantum chemistry software package
#
# This program is free software; you can redistribute it and/or modify
# it under the terms of the GNU General Public License as published by
# the Free Software Foundation; either version 2 of the License, or
# (at your option) any later version.
#
# This program is distributed in the hope that it will be useful,
# but WITHOUT ANY WARRANTY; without even the implied warranty of
# MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the
# GNU General Public License for more details.
#
# You should have received a copy of the GNU General Public License along
# with this program; if not, write to the Free Software Foundation, Inc.,
# 51 Franklin Street, Fifth Floor, Boston, MA 02110-1301 USA.
#
#@END LICENSE
#
import os
#import re
#import math
#import copy
#from periodictable import *
#from physconst import *
#from vecutil import *
#from exceptions import *
#from coordentry import *
import subprocess
import socket
import shutil
import random
from collections import defaultdict
from libmintsmolecule import *
class Molecule(LibmintsMolecule):
"""Class to store python extensions to the MoleculeLibmints class.
Multiple classes allows separation of libmints and extension methods.
"""
def __init__(self, psi4molstr=None):
"""Initialize Molecule object from LibmintsMolecule"""
LibmintsMolecule.__init__(self, psi4molstr)
# The comment line
self.tagline = ""
def __str__(self):
text = """ ==> qcdb Molecule %s <==\n\n""" % (self.name())
text += """ => %s <=\n\n""" % (self.tagline)
text += self.create_psi4_string_from_molecule()
return text
# def __getstate__(self):
# print 'im being pickled'
# return self.__dict__
# def __setstate__(self, d):
# print 'im being unpickled with these values', d
# self.__dict__ = d
@classmethod
def init_with_xyz(cls, xyzfilename, no_com=False, no_reorient=False, contentsNotFilename=False):
"""Pull information from an XYZ file. No fragment info detected.
Bohr/Angstrom pulled from first line if available. Charge,
multiplicity, tagline pulled from second line if available. Body
accepts atom symbol or atom charge in first column. Arguments
*no_com* and *no_reorient* can be used to turn off shift and
rotation. If *xyzfilename* is a string of the contents of an XYZ
file, rather than the name of a file, set *contentsNotFilename*
to ``True``.
>>> H2O = qcdb.Molecule.init_with_xyz('h2o.xyz')
"""
instance = cls()
instance.lock_frame = False
instance.PYmove_to_com = not no_com
instance.PYfix_orientation = no_reorient
if contentsNotFilename:
text = xyzfilename.splitlines()
else:
try:
infile = open(xyzfilename, 'r')
except IOError:
raise ValidationError("""Molecule::init_with_xyz: given filename '%s' does not exist.""" % (xyzfilename))
if os.stat(xyzfilename).st_size == 0:
raise ValidationError("""Molecule::init_with_xyz: given filename '%s' is blank.""" % (xyzfilename))
text = infile.readlines()
xyz1 = re.compile(r"^\s*(\d+)\s*(bohr|au)?\s*$", re.IGNORECASE)
xyz2 = re.compile(r'^\s*(-?\d+)\s+(\d+)\s+(.*)\s*$')
xyzN = re.compile(r"(?:\s*)([A-Z](?:[a-z])?)(?:\s+)(-?\d+\.\d+)(?:\s+)(-?\d+\.\d+)(?:\s+)(-?\d+\.\d+)(?:\s*)", re.IGNORECASE)
xyzC = re.compile(r"(?:\s*)(\d+\.?\d*)(?:\s+)(-?\d+\.\d+)(?:\s+)(-?\d+\.\d+)(?:\s+)(-?\d+\.\d+)(?:\s*)", re.IGNORECASE)
# Try to match the first line
if xyz1.match(text[0]):
fileNatom = int(xyz1.match(text[0]).group(1))
if xyz1.match(text[0]).group(2) == None:
fileUnits = 'Angstrom'
else:
fileUnits = 'Bohr'
else:
raise ValidationError("Molecule::init_with_xyz: Malformed first line\n%s" % (text[0]))
# Try to match the second line
if xyz2.match(text[1]):
instance.set_molecular_charge(int(xyz2.match(text[1]).group(1)))
instance.set_multiplicity(int(xyz2.match(text[1]).group(2)))
instance.tagline = xyz2.match(text[1]).group(3).strip()
else:
instance.tagline = text[1].strip()
# Next line begins the useful information.
for i in range(fileNatom):
try:
if xyzN.match(text[2 + i]):
fileAtom = xyzN.match(text[2 + i]).group(1).upper()
fileX = float(xyzN.match(text[2 + i]).group(2))
fileY = float(xyzN.match(text[2 + i]).group(3))
fileZ = float(xyzN.match(text[2 + i]).group(4))
# Check that the atom symbol is valid
if not fileAtom in el2z:
raise ValidationError('Illegal atom symbol in geometry specification: %s' % (fileAtom))
# Add it to the molecule.
instance.add_atom(el2z[fileAtom], fileX, fileY, fileZ, fileAtom, el2masses[fileAtom], el2z[fileAtom])
elif xyzC.match(text[2 + i]):
fileAtom = int(float(xyzC.match(text[2 + i]).group(1)))
fileX = float(xyzC.match(text[2 + i]).group(2))
fileY = float(xyzC.match(text[2 + i]).group(3))
fileZ = float(xyzC.match(text[2 + i]).group(4))
# Check that the atomic number is valid
if not fileAtom in z2el:
raise ValidationError('Illegal atom symbol in geometry specification: %d' % (fileAtom))
# Add it to the molecule.
instance.add_atom(fileAtom, fileX, fileY, fileZ, z2el[fileAtom], z2masses[fileAtom], fileAtom)
else:
raise ValidationError("Molecule::init_with_xyz: Malformed atom information line %d." % (i + 3))
except IndexError:
raise ValidationError("Molecule::init_with_xyz: Expected atom in file at line %d.\n%s" % (i + 3, text[i + 2]))
# We need to make 1 fragment with all atoms
instance.fragments.append([0, fileNatom - 1])
instance.fragment_types.append('Real')
instance.fragment_charges.append(instance.molecular_charge())
instance.fragment_multiplicities.append(instance.multiplicity())
# Set the units properly
instance.PYunits = fileUnits
if fileUnits == 'Bohr':
instance.input_units_to_au = 1.0
elif fileUnits == 'Angstrom':
instance.input_units_to_au = 1.0 / psi_bohr2angstroms
instance.update_geometry()
return instance
def save_string_xyz(self, save_ghosts=True):
"""Save a string for a XYZ-style file.
>>> H2OH2O.save_string_xyz()
6
-2 3 water_dimer
O -1.551007000000 -0.114520000000 0.000000000000
H -1.934259000000 0.762503000000 0.000000000000
H -0.599677000000 0.040712000000 0.000000000000
O 1.350625000000 0.111469000000 0.000000000000
H 1.680398000000 -0.373741000000 -0.758561000000
H 1.680398000000 -0.373741000000 0.758561000000
"""
factor = 1.0 if self.PYunits == 'Angstrom' else psi_bohr2angstroms
N = self.natom()
if not save_ghosts:
N = 0
for i in range(self.natom()):
if self.Z(i):
N += 1
text = "%d\n" % (N)
text += '%d %d %s\n' % (self.molecular_charge(), self.multiplicity(), self.tagline)
for i in range(self.natom()):
[x, y, z] = self.atoms[i].compute()
if save_ghosts or self.Z(i):
text += '%2s %17.12f %17.12f %17.12f\n' % ((self.symbol(i) if self.Z(i) else "Gh"), \
x * factor, y * factor, z * factor)
return text
# def save_string_for_psi4(self):
# """Returns a string of Molecule formatted for psi4.
# Includes fragments and reorienting, if specified.
#
# >>> print H2OH2O.save_string_for_psi4()
# 6
# 0 1
# O -1.55100700 -0.11452000 0.00000000
# H -1.93425900 0.76250300 0.00000000
# H -0.59967700 0.04071200 0.00000000
# --
# 0 1
# @X 0.00000000 0.00000000 0.00000000
# O 1.35062500 0.11146900 0.00000000
# H 1.68039800 -0.37374100 -0.75856100
# H 1.68039800 -0.37374100 0.75856100
# units Angstrom
#
# """
# Nfr = 0
# text = ""
# for fr in range(self.nfragments()):
# if self.fragment_types[fr] == 'Absent':
# continue
# if Nfr != 0:
# text += """--\n"""
# Nfr += 1
# text += """%d %d\n""" % (self.fragment_charges[fr], self.fragment_multiplicities[fr])
# for at in range(self.fragments[fr][0], self.fragments[fr][1] + 1):
# geom = self.full_atoms[at].compute()
# text += """%-3s %16.8f %16.8f %16.8f\n""" % \
# (("" if self.fZ(at) else "@") + self.full_atoms[at].symbol(), \
# geom[0], geom[1], geom[2])
# text += """units %s\n""" % (self.units().lower())
# return text
def format_molecule_for_psi4(self):
"""Returns string of molecule definition block."""
text = 'molecule mol {\n'
for line in self.create_psi4_string_from_molecule().splitlines():
text += ' ' + line + '\n'
text += '}\n'
return text
def format_molecule_for_qchem(self):
"""
"""
factor = 1.0 if self.PYunits == 'Angstrom' else psi_bohr2angstroms
text = ""
text += '$molecule\n'
text += '%d %d %s\n' % (self.molecular_charge(), self.multiplicity(), self.tagline)
for i in range(self.natom()):
[x, y, z] = self.atoms[i].compute()
text += '%2s %17.12f %17.12f %17.12f\n' % ((self.symbol(i) if self.Z(i) else "Gh"), \
x * factor, y * factor, z * factor)
text += '$end\n'
return text
pass
def format_molecule_for_molpro(self):
"""
"""
factor = 1.0 if self.PYunits == 'Angstrom' else psi_bohr2angstroms
# TODO keep fix_or?
self.fix_orientation(True)
self.PYmove_to_com = False
self.update_geometry()
text = ""
text += 'angstrom\n'
text += 'geometry={\n'
for fr in range(self.nfragments()):
if self.fragment_types[fr] == 'Absent':
pass
else:
for at in range(self.fragments[fr][0], self.fragments[fr][1] + 1):
[x, y, z] = self.atoms[at].compute()
text += '%2s %17.12f %17.12f %17.12f\n' % (self.symbol(at), \
x * factor, y * factor, z * factor)
text += '}\n\n'
text += 'SET,CHARGE=%d\n' % (self.molecular_charge())
text += 'SET,SPIN=%d\n' % (self.multiplicity() - 1) # Molpro wants (mult-1)
textDummy = "dummy"
for fr in range(self.nfragments()):
if self.fragment_types[fr] == 'Ghost':
for at in range(self.fragments[fr][0], self.fragments[fr][1] + 1):
textDummy += """,%d""" % (at + 1) # Molpro atom numbering is 1-indexed
textDummy += '\n'
if len(textDummy) > 6:
text += textDummy
return text
def format_molecule_for_cfour(self):
"""Function to print Molecule in a form readable by Cfour.
"""
self.update_geometry()
factor = 1.0 if self.PYunits == 'Angstrom' else psi_bohr2angstroms
#factor = 1.0 if self.PYunits == 'Bohr' else 1.0/psi_bohr2angstroms
text = 'auto-generated by qcdb from molecule %s\n' % (self.tagline)
# append atoms and coordentries
for fr in range(self.nfragments()):
if self.fragment_types[fr] == 'Absent':
pass
else:
for at in range(self.fragments[fr][0], self.fragments[fr][1] + 1):
[x, y, z] = self.atoms[at].compute()
text += '%-2s %17.12f %17.12f %17.12f\n' % ((self.symbol(at) if self.Z(at) else "GH"), \
x * factor, y * factor, z * factor)
text += '\n'
# prepare molecule keywords to be set as c-side keywords
options = defaultdict(lambda: defaultdict(dict))
options['CFOUR']['CFOUR_CHARGE']['value'] = self.molecular_charge()
options['CFOUR']['CFOUR_MULTIPLICITY']['value'] = self.multiplicity()
options['CFOUR']['CFOUR_UNITS']['value'] = 'ANGSTROM'
# options['CFOUR']['CFOUR_UNITS']['value'] = 'BOHR'
options['CFOUR']['CFOUR_COORDINATES']['value'] = 'CARTESIAN'
# options['CFOUR']['CFOUR_SUBGROUP']['value'] = self.symmetry_from_input().upper()
# print self.inertia_tensor()
# print self.inertial_system()
options['CFOUR']['CFOUR_CHARGE']['clobber'] = True
options['CFOUR']['CFOUR_MULTIPLICITY']['clobber'] = True
options['CFOUR']['CFOUR_UNITS']['clobber'] = True
options['CFOUR']['CFOUR_COORDINATES']['clobber'] = True
return text, options
def format_basis_for_cfour(self, puream):
"""Function to print the BASIS=SPECIAL block for Cfour according
to the active atoms in Molecule. Special short basis names
are used by Psi4 libmints GENBAS-writer in accordance with
Cfour constraints.
"""
text = ''
cr = 1
for fr in range(self.nfragments()):
if self.fragment_types[fr] == 'Absent':
pass
else:
for at in range(self.fragments[fr][0], self.fragments[fr][1] + 1):
text += """%s:P4_%d\n""" % (self.symbol(at).upper(), cr)
cr += 1
text += '\n'
options = defaultdict(lambda: defaultdict(dict))
options['CFOUR']['CFOUR_BASIS']['value'] = 'SPECIAL'
options['CFOUR']['CFOUR_SPHERICAL']['value'] = puream
options['CFOUR']['CFOUR_BASIS']['clobber'] = True
options['CFOUR']['CFOUR_SPHERICAL']['clobber'] = True
options['CFOUR']['CFOUR_BASIS']['superclobber'] = True
options['CFOUR']['CFOUR_SPHERICAL']['superclobber'] = True
return text, options
def format_molecule_for_cfour_old(self):
"""Function to print Molecule in a form readable by Cfour. This
version works as long as zmat is composed entirely of variables,
not internal values, while cartesian is all internal values,
no variables. Cutting off this line of development because,
with getting molecules after passing through libmints Molecule,
all zmats with dummies (Cfour's favorite kind) have already been
converted into cartesian. Next step, if this line was pursued
would be to shift any zmat internal values to external and any
cartesian external values to internal.
"""
text = ''
text += 'auto-generated by qcdb from molecule %s\n' % (self.tagline)
# # append units and any other non-default molecule keywords
# text += " units %-s\n" % ("Angstrom" if self.units() == 'Angstrom' else "Bohr")
# if not self.PYmove_to_com:
# text += " no_com\n"
# if self.PYfix_orientation:
# text += " no_reorient\n"
# append atoms and coordentries and fragment separators with charge and multiplicity
Pfr = 0
isZMat = False
isCart = False
for fr in range(self.nfragments()):
if self.fragment_types[fr] == 'Absent' and not self.has_zmatrix():
continue
# text += "%s %s%d %d\n" % (
# "" if Pfr == 0 else " --\n",
# "#" if self.fragment_types[fr] == 'Ghost' or self.fragment_types[fr] == 'Absent' else "",
# self.fragment_charges[fr], self.fragment_multiplicities[fr])
Pfr += 1
for at in range(self.fragments[fr][0], self.fragments[fr][1] + 1):
if type(self.full_atoms[at]) == ZMatrixEntry:
isZMat = True
elif type(self.full_atoms[at]) == CartesianEntry:
isCart = True
if self.fragment_types[fr] == 'Absent':
text += "%s" % ("X")
elif self.fZ(at) or self.fsymbol(at) == "X":
text += "%s" % (self.fsymbol(at))
else:
text += "%s" % ("GH") # atom info is lost + self.fsymbol(at) + ")")
text += "%s" % (self.full_atoms[at].print_in_input_format_cfour())
text += "\n"
# append any coordinate variables
if len(self.geometry_variables):
for vb, val in self.geometry_variables.items():
text += """%s=%.10f\n""" % (vb, val)
text += "\n"
# prepare molecule keywords to be set as c-side keywords
options = defaultdict(lambda: defaultdict(dict))
options['CFOUR']['CFOUR_CHARGE']['value'] = self.molecular_charge()
options['CFOUR']['CFOUR_MULTIPLICITY']['value'] = self.multiplicity()
options['CFOUR']['CFOUR_UNITS']['value'] = self.units()
if isZMat and not isCart:
options['CFOUR']['CFOUR_COORDINATES']['value'] = 'INTERNAL'
elif isCart and not isZMat:
options['CFOUR']['CFOUR_COORDINATES']['value'] = 'CARTESIAN'
else:
raise ValidationError("""Strange mix of Cartesian and ZMatrixEntries in molecule unsuitable for Cfour.""")
return text, options
def format_molecule_for_nwchem(self):
"""
"""
factor = 1.0 if self.PYunits == 'Angstrom' else psi_bohr2angstroms
text = ""
text += '%d %d %s\n' % (self.molecular_charge(), self.multiplicity(), self.tagline)
for i in range(self.natom()):
[x, y, z] = self.atoms[i].compute()
text += '%4s %17.12f %17.12f %17.12f\n' % (("" if self.Z(i) else 'Bq') + self.symbol(i), \
x * factor, y * factor, z * factor)
return text
pass
# if symm print M2OUT "nosym\nnoorient\n";
# print DIOUT "angstrom\ngeometry={\n";
def auto_fragments(self):
"""Detects fragments in an unfragmented molecule using BFS
algorithm. Returns a new Molecule in Cartesian, fixed-geom
(no variable values), no dummy-atom format. Any non-default
charge and multiplicity assigned to first fragment.
"""
if self.nfragments() != 1:
print 'Molecule already fragmented so no further action by auto_fragments().'
return self
flist = self.BFS()
# form new molecule through a string since self may contain
# dummies or zmatrix specs that mayn't be valid with atom shuffling
new_geom = '\n'
if self.PYcharge_specified or self.PYmultiplicity_specified:
new_geom = """\n %d %d\n""" % (self.molecular_charge(), self.multiplicity())
for fr in range(len(flist)):
new_geom += "" if fr == 0 else " --\n"
for at in flist[fr]:
geom = self.atoms[at].compute()
new_geom += """%-4s """ % (("" if self.Z(at) else "@") + self.symbol(at))
for j in range(3):
new_geom += """ %17.12f""" % (geom[j])
new_geom += "\n"
new_geom += " units %s\n" % (self.units())
if not self.PYmove_to_com:
new_geom += " no_com\n"
if self.orientation_fixed():
new_geom += " no_reorient\n"
subset = Molecule(new_geom)
subset.update_geometry()
return subset
def BFS(self):
"""Perform a breadth-first search (BFS) on the real atoms
in molecule, returning an array of atom indices of fragments.
Relies upon van der Waals radii and so faulty for close
(esp. hydrogen-bonded) fragments. Original code from
Michael S. Marshall.
"""
vdW_diameter = {
#'H': 1.001 / 1.5, # JMol
'HE': 1.012 / 1.5, # JMol
'LI': 0.825 / 1.5, # JMol
'BE': 1.408 / 1.5, # JMol
#'B': 1.485 / 1.5, # JMol
#'C': 1.452 / 1.5, # JMol
#'N': 1.397 / 1.5, # JMol
#'O': 1.342 / 1.5, # JMol
#'F': 1.287 / 1.5, # JMol
'NE': 1.243 / 1.5, # JMol
'NA': 1.144 / 1.5, # JMol
'MG': 1.364 / 1.5, # JMol
'AL': 1.639 / 1.5, # JMol
#'SI': 1.716 / 1.5, # JMol
#'P': 1.705 / 1.5, # JMol
#'S': 1.683 / 1.5, # JMol
#'CL': 1.639 / 1.5, # JMol
'AR': 1.595 / 1.5, # JMol
'H': 1.06 / 1.5, # Bondi JPC 68 441 (1964)
'B': 1.65 / 1.5, # Bondi JPC 68 441 (1964)
'C': 1.53 / 1.5, # Bondi JPC 68 441 (1964)
'N': 1.46 / 1.5, # Bondi JPC 68 441 (1964)
'O': 1.42 / 1.5, # Bondi JPC 68 441 (1964)
'F': 1.40 / 1.5, # Bondi JPC 68 441 (1964)
'SI': 1.93 / 1.5, # Bondi JPC 68 441 (1964)
'P': 1.86 / 1.5, # Bondi JPC 68 441 (1964)
'S': 1.80 / 1.5, # Bondi JPC 68 441 (1964)
'CL': 1.75 / 1.5, # Bondi JPC 68 441 (1964)
'GE': 1.98 / 1.5, # Bondi JPC 68 441 (1964)
'AS': 1.94 / 1.5, # Bondi JPC 68 441 (1964)
'SE': 1.90 / 1.5, # Bondi JPC 68 441 (1964)
'BR': 1.87 / 1.5, # Bondi JPC 68 441 (1964)
'SN': 2.16 / 1.5, # Bondi JPC 68 441 (1964)
'SB': 2.12 / 1.5, # Bondi JPC 68 441 (1964)
'TE': 2.08 / 1.5, # Bondi JPC 68 441 (1964)
'I': 2.04 / 1.5, # Bondi JPC 68 441 (1964)
'XE': 2.05 / 1.5} # Bondi JPC 68 441 (1964)
Queue = []
White = range(self.natom()) # untouched
Black = [] # touched and all edges discovered
Fragment = [] # stores fragments
start = 0 # starts with the first atom in the list
Queue.append(start)
White.remove(start)
# Simply start with the first atom, do a BFS when done, go to any
# untouched atom and start again iterate until all atoms belong
# to a fragment group
while len(White) > 0 or len(Queue) > 0: # Iterates to the next fragment
Fragment.append([])
while len(Queue) > 0: # BFS within a fragment
for u in Queue: # find all (still white) nearest neighbors to vertex u
for i in White:
dist = distance(self.xyz(i), self.xyz(u)) * psi_bohr2angstroms
if dist < vdW_diameter[self.symbol(u)] + vdW_diameter[self.symbol(i)]:
Queue.append(i) # if you find you, put in the queue
White.remove(i) # and remove it from the untouched list
Queue.remove(u) # remove focus from Queue
Black.append(u)
Fragment[-1].append(int(u)) # add to group (0-indexed)
Fragment[-1].sort() # preserve original atom ordering
if len(White) != 0: # can't move White -> Queue if no more exist
Queue.append(White[0])
White.remove(White[0])
return Fragment
def inertia_tensor(self, masswt=True, zero=ZERO):
"""Compute inertia tensor.
>>> print H2OH2O.inertia_tensor()
[[8.704574864178731, -8.828375721817082, 0.0], [-8.828375721817082, 280.82861714077666, 0.0], [0.0, 0.0, 281.249500988553]]
"""
return self.inertia_tensor_partial(range(self.natom()), masswt, zero)
def inertia_tensor_partial(self, part, masswt=True, zero=ZERO):
"""Compute inertia tensor based on atoms in *part*.
"""
tensor = [[0, 0, 0], [0, 0, 0], [0, 0, 0]]
for i in part:
if masswt:
# I(alpha, alpha)
tensor[0][0] += self.mass(i) * (self.y(i) * self.y(i) + self.z(i) * self.z(i))
tensor[1][1] += self.mass(i) * (self.x(i) * self.x(i) + self.z(i) * self.z(i))
tensor[2][2] += self.mass(i) * (self.x(i) * self.x(i) + self.y(i) * self.y(i))
# I(alpha, beta)
tensor[0][1] -= self.mass(i) * self.x(i) * self.y(i)
tensor[0][2] -= self.mass(i) * self.x(i) * self.z(i)
tensor[1][2] -= self.mass(i) * self.y(i) * self.z(i)
else:
# I(alpha, alpha)
tensor[0][0] += self.y(i) * self.y(i) + self.z(i) * self.z(i)
tensor[1][1] += self.x(i) * self.x(i) + self.z(i) * self.z(i)
tensor[2][2] += self.x(i) * self.x(i) + self.y(i) * self.y(i)
# I(alpha, beta)
tensor[0][1] -= self.x(i) * self.y(i)
tensor[0][2] -= self.x(i) * self.z(i)
tensor[1][2] -= self.y(i) * self.z(i)
# mirror
tensor[1][0] = tensor[0][1]
tensor[2][0] = tensor[0][2]
tensor[2][1] = tensor[1][2]
# Check the elements for zero and make them a hard zero.
for i in range(3):
for j in range(3):
if math.fabs(tensor[i][j]) < zero:
tensor[i][j] = 0.0
return tensor
def inertial_system_partial(self, part, masswt=True, zero=ZERO):
"""Solve inertial system based on atoms in *part*"""
return diagonalize3x3symmat(self.inertia_tensor_partial(part, masswt, zero))
def inertial_system(self, masswt=True, zero=ZERO):
"""Solve inertial system"""
return diagonalize3x3symmat(self.inertia_tensor(masswt, zero))
def print_ring_planes(self, entity1, entity2, entity3=None, entity4=None):
"""(reals only, 1-indexed)
"""
pass
# TODO allow handle lines
text = ""
summ = []
#for entity in [entity1, entity2, entity3, entity4]:
for item in [entity1, entity2]:
text += """\n ==> Entity %s <==\n\n""" % (item)
# convert plain atoms into list and move from 1-indexed to 0-indexed
entity = []
try:
for idx in item:
entity.append(idx - 1)
except TypeError:
entity = [item - 1]
if len(entity) == 1:
dim = 'point'
elif len(entity) == 2:
dim = 'line'
else:
dim = 'plane'
# compute centroid
cent = [0.0, 0.0, 0.0]
for at in entity:
cent = add(cent, self.xyz(at))
cent = scale(cent, 1.0 / len(entity))
text += ' Centroid: %14.8f %14.8f %14.8f [Angstrom]\n' % \
(cent[0] * psi_bohr2angstroms, \
cent[1] * psi_bohr2angstroms, \
cent[2] * psi_bohr2angstroms)
text += ' Centroid: %14.8f %14.8f %14.8f [Bohr]\n' % \
(cent[0], cent[1], cent[2])
if dim == 'point':
summ.append({'dim': dim, 'geo': cent, 'cent': cent})
# TODO: figure out if should be using mass-weighted
self.translate(scale(cent, -1))
evals, evecs = self.inertial_system_partial(entity, masswt=False)
midx = evals.index(max(evals))
text += ' Normal Vector: %14.8f %14.8f %14.8f [unit]\n' % \
(evecs[0][midx], evecs[1][midx], evecs[2][midx])
text += ' Normal Vector: %14.8f %14.8f %14.8f [unit]\n' % \
(evecs[0][midx] + cent[0], evecs[1][midx] + cent[1], evecs[2][midx] + cent[2])
xplane = [evecs[0][midx], evecs[1][midx], evecs[2][midx], \
-1.0 * (evecs[0][midx] * cent[0] + evecs[1][midx] * cent[1] + evecs[2][midx] * cent[2])]
text += ' Eqn. of Plane: %14.8f %14.8f %14.8f %14.8f [Ai + Bj + Ck + D = 0]\n' % \
(xplane[0], xplane[1], xplane[2], xplane[3])
dtemp = math.sqrt(evecs[0][midx] * evecs[0][midx] + evecs[1][midx] * evecs[1][midx] + evecs[2][midx] * evecs[2][midx])
print 'denom', dtemp
hessplane = [evecs[0][midx] / dtemp, evecs[1][midx] / dtemp, evecs[2][midx] / dtemp, xplane[3] / dtemp]
hessplane2 = [xplane[0] / dtemp, xplane[1] / dtemp, xplane[2] / dtemp, xplane[3] / dtemp]
text += ' Eqn. of Plane: %14.8f %14.8f %14.8f %14.8f [Ai + Bj + Ck + D = 0] H\n' % \
(hessplane[0], hessplane[1], hessplane[2], hessplane[3])
text += ' Eqn. of Plane: %14.8f %14.8f %14.8f %14.8f [Ai + Bj + Ck + D = 0] H2\n' % \
(hessplane2[0], hessplane2[1], hessplane2[2], hessplane2[3])
self.translate(cent)
if dim == 'plane':
summ.append({'dim': dim, 'geo': xplane, 'cent': cent})
#print summ
text += """\n ==> 1 (%s) vs. 2 (%s) <==\n\n""" % (summ[0]['dim'], summ[1]['dim'])
# if summ[0]['dim'] == 'plane' and summ[1]['dim'] == 'point':
# cent = summ[1]['geo']
# plane = summ[0]['geo']
# print cent, plane
#
# D = math.fabs(plane[0] * cent[0] + plane[1] * cent[1] + plane[2] * cent[2] + plane[3]) / \
# math.sqrt(plane[0] * plane[0] + plane[1] * plane[1] + plane[2] * plane[2])
# text += ' Pt to Plane: %14.8f [Angstrom]\n' % (D * psi_bohr2angstroms)
#if summ[0]['dim'] == 'plane' and summ[1]['dim'] == 'plane':
if summ[0]['dim'] == 'plane' and (summ[1]['dim'] == 'plane' or summ[1]['dim'] == 'point'):
cent1 = summ[0]['cent']
cent2 = summ[1]['cent']
plane1 = summ[0]['geo']
#plane2 = summ[1]['geo']
distCC = distance(cent1, cent2)
text += ' Distance from Center of %s to Center of %s: %14.8f [Angstrom]\n' % \
('2', '1', distCC * psi_bohr2angstroms)
distCP = math.fabs(plane1[0] * cent2[0] + plane1[1] * cent2[1] + plane1[2] * cent2[2] + plane1[3])
# distCP expression has a denominator that's one since plane constructed from unit vector
text += ' Distance from Center of %s to Plane of %s: %14.8f [Angstrom]\n' % \
('2', '1', distCP * psi_bohr2angstroms)
distCPC = math.sqrt(distCC * distCC - distCP * distCP)
text += ' Distance from Center of %s to Center of %s along Plane of %s: %14.8f [Angstrom]\n' % \
('2', '1', '1', distCPC * psi_bohr2angstroms)
print text
# text = " Interatomic Distances (Angstroms)\n\n"
# for i in range(self.natom()):
# for j in range(i + 1, self.natom()):
# eij = sub(self.xyz(j), self.xyz(i))
# dist = norm(eij) * psi_bohr2angstroms
# text += " Distance %d to %d %-8.3lf\n" % (i + 1, j + 1, dist)
# text += "\n\n"
# return text
def rotor_type(self, tol=FULL_PG_TOL):
"""Returns the rotor type.
>>> H2OH2O.rotor_type()
RT_ASYMMETRIC_TOP
"""
evals, evecs = diagonalize3x3symmat(self.inertia_tensor())
evals = sorted(evals)
rot_const = [1.0 / evals[0] if evals[0] > 1.0e-6 else 0.0,
1.0 / evals[1] if evals[1] > 1.0e-6 else 0.0,
1.0 / evals[2] if evals[2] > 1.0e-6 else 0.0]
# Determine degeneracy of rotational constants.
degen = 0
for i in range(2):
for j in range(i + 1, 3):
if degen >= 2:
continue
rabs = math.fabs(rot_const[i] - rot_const[j])
tmp = rot_const[i] if rot_const[i] > rot_const[j] else rot_const[j]
if rabs > ZERO:
rel = rabs / tmp
else:
rel = 0.0
if rel < tol:
degen += 1
#print "\tDegeneracy is %d\n" % (degen)
# Determine rotor type
if self.natom() == 1:
rotor_type = 'RT_ATOM'
elif rot_const[0] == 0.0:
rotor_type = 'RT_LINEAR' # 0 < IB == IC inf > B == C
elif degen == 2:
rotor_type = 'RT_SPHERICAL_TOP' # IA == IB == IC A == B == C
elif degen == 1:
if (rot_const[1] - rot_const[2]) < 1.0e-6:
rotor_type = 'RT_PROLATE_SYMMETRIC_TOP' # IA < IB == IC A > B == C
elif (rot_const[0] - rot_const[1]) < 1.0e-6:
rotor_type = 'RT_OBLATE_SYMMETRIC_TOP' # IA == IB < IC A == B > C
else:
rotor_type = 'RT_ASYMMETRIC_TOP' # IA < IB < IC A > B > C
return rotor_type
def center_of_charge(self):
"""Computes center of charge of molecule (does not translate molecule).
>>> H2OH2O.center_of_charge()
[-0.073339893272065401, 0.002959783555632145, 0.0]
"""
ret = [0.0, 0.0, 0.0]
total_c = 0.0
for at in range(self.natom()):
c = self.charge(at)
ret = add(ret, scale(self.xyz(at), c))
total_c += c
ret = scale(ret, 1.0 / total_c)
return ret
def move_to_coc(self):
"""Moves molecule to center of charge
"""
coc = scale(self.center_of_charge(), -1.0)
self.translate(coc)
# Attach method to qcdb.Molecule class
from interface_dftd3 import run_dftd3 as _dftd3_qcdb_yo
Molecule.run_dftd3 = _dftd3_qcdb_yo
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