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authorDavid Luevano <55825613+luevano@users.noreply.github.com>2019-12-08 21:54:19 -0700
committerDavid Luevano <55825613+luevano@users.noreply.github.com>2019-12-08 21:54:19 -0700
commit7c8b391dddd65ff58417df80dfc79cadddf4f4e6 (patch)
tree0bad908f5b40848addc3307de4307b1dae4c6e7e /lj_matrix.py
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+import math
+import numpy as np
+from numpy.linalg import eig
+
+
+def lj_matrix(mol_data,
+ nc_data,
+ max_len=25,
+ as_eig=False,
+ bohr_radius_units=False):
+ """
+ Creates the coulomb matrix from the molecule data given.
+ mol_data: molecule data, matrix of atom coordinates.
+ nc_data: nuclear charge data, array of atom data.
+ max_len: maximum amount of atoms in molecule.
+ as_eig: if data should be returned as matrix or array of eigenvalues.
+ bohr_radius_units: if units should be in bohr's radius units.
+ """
+ if bohr_radius_units:
+ conversion_rate = 0.52917721067
+ else:
+ conversion_rate = 1
+
+ mol_n = len(mol_data)
+ mol_nr = range(mol_n)
+
+ if not mol_n == len(nc_data):
+ print(''.join(['Error. Molecule matrix dimension is different ',
+ 'than the nuclear charge array dimension.']))
+ else:
+ if max_len < mol_n:
+ print(''.join(['Error. Molecule matrix dimension (mol_n) is ',
+ 'greater than max_len. Using mol_n.']))
+ max_len = None
+
+ if max_len:
+ lj = np.zeros((max_len, max_len))
+ ml_r = range(max_len)
+
+ # Actual calculation of the coulomb matrix.
+ for i in ml_r:
+ if i < mol_n:
+ x_i = mol_data[i, 0]
+ y_i = mol_data[i, 1]
+ z_i = mol_data[i, 2]
+ Z_i = nc_data[i]
+ else:
+ break
+
+ for j in ml_r:
+ if j < mol_n:
+ x_j = mol_data[j, 0]
+ y_j = mol_data[j, 1]
+ z_j = mol_data[j, 2]
+
+ x = (x_i-x_j)**2
+ y = (y_i-y_j)**2
+ z = (z_i-z_j)**2
+
+ if i == j:
+ lj[i, j] = (0.5*Z_i**2.4)
+ else:
+ # Calculations are done after i==j is checked
+ # so no division by zero is done.
+
+ # A little play with r exponents
+ # so no square root is calculated.
+ # Conversion factor is included in r^2.
+
+ # 1/r^2
+ r_2 = 1/(conversion_rate**2*(x + y + z))
+
+ r_6 = math.pow(r_2, 3)
+ r_12 = math.pow(r_6, 2)
+ lj[i, j] = (4*(r_12 - r_6))
+ else:
+ break
+
+ # Now the value will be returned.
+ if as_eig:
+ lj_sorted = np.sort(eig(lj)[0])[::-1]
+ # Thanks to SO for the following lines of code.
+ # https://stackoverflow.com/a/43011036
+
+ # Keep zeros at the end.
+ mask = lj_sorted != 0.
+ f_mask = mask.sum(0, keepdims=1) >\
+ np.arange(lj_sorted.shape[0]-1, -1, -1)
+
+ f_mask = f_mask[::-1]
+ lj_sorted[f_mask] = lj_sorted[mask]
+ lj_sorted[~f_mask] = 0.
+
+ return lj_sorted
+
+ else:
+ return lj
+
+ else:
+ lj_temp = []
+ # Actual calculation of the coulomb matrix.
+ for i in mol_nr:
+ x_i = mol_data[i, 0]
+ y_i = mol_data[i, 1]
+ z_i = mol_data[i, 2]
+ Z_i = nc_data[i]
+
+ lj_row = []
+ for j in mol_nr:
+ x_j = mol_data[j, 0]
+ y_j = mol_data[j, 1]
+ z_j = mol_data[j, 2]
+
+ x = (x_i-x_j)**2
+ y = (y_i-y_j)**2
+ z = (z_i-z_j)**2
+
+ if i == j:
+ lj_row.append(0.5*Z_i**2.4)
+ else:
+ # Calculations are done after i==j is checked
+ # so no division by zero is done.
+
+ # A little play with r exponents
+ # so no square root is calculated.
+ # Conversion factor is included in r^2.
+
+ # 1/r^2
+ r_2 = 1/(conversion_rate**2*(x + y + z))
+
+ r_6 = math.pow(r_2, 3)
+ r_12 = math.pow(r_6, 2)
+ lj_row.append(4*(r_12 - r_6))
+
+ lj_temp.append(np.array(lj_row))
+
+ lj = np.array(lj_temp)
+ # Now the value will be returned.
+ if as_eig:
+ return np.sort(eig(lj)[0])[::-1]
+ else:
+ return lj