import io
from itertools import chain

import matplotlib.pyplot as plt
import numpy as np
from ase.io import read
from ase.optimize import FIRE
from ase.vibrations import Vibrations
from ase.vibrations.franck_condon import FranckCondon

from gpaw import GPAW
from gpaw.mpi import world
from gpaw.utilities.adjust_cell import adjust_cell
from gpaw.utilities.folder import Folder

butadiene = u"""10

C       3.649801161546418      5.442281389577507      3.863313703750026
C       5.051651240044169      5.368220758269772      4.162165876906096
C       5.750174626862403      4.162261915959347      4.240449977068684
C       7.150130182125531      4.155384186721486      4.537328602062397
H       3.218154657585170      4.565210696328925      3.522601038049320
H       3.077656122062729      6.375092902842770      3.826039498180272
H       5.478464901706067      6.370680001794822      4.422235395756437
H       5.320549047980879      3.220584852467720      3.974551561510350
H       7.723359150977955      3.224855971783890      4.574146712279462
H       7.580803493981530      5.034479218283977      4.877211530909463
"""

h = 0.3
atoms = read(io.StringIO(butadiene), format='xyz')
adjust_cell(atoms, 3.0, h)
atoms.calc = GPAW(mode='fd', h=h)
if 0:
    dyn = FIRE(atoms)
    dyn.run(fmax=0.05)
    atoms.write('butadiene.xyz')

vibname = 'fcvib'
vib = Vibrations(atoms, name=vibname)
vib.run()

# Modul
a = FranckCondon(atoms, vibname, minfreq=250)

# excited state forces
F = np.array([[-2.11413, 0.07317, -0.91682],
              [3.23569, -0.74520, 0.76758],
              [-3.44847, 0.63846, -0.81080],
              [2.77345, 0.01272, 0.74811],
              [-0.06544, -0.01078, -0.03209],
              [-0.01245, -0.01123, -0.00040],
              [0.00186, -0.05864, -0.00371],
              [-0.00151, 0.05815, 0.00141],
              [0.01625, 0.00781, -0.00202],
              [0.06253, 0.00902, 0.03381]])

# Huang-Rhys factors
S, fq = a.get_Huang_Rhys_factors(F)

# Temperature and #quanta taken into account
T = 300
n = 10

colors = ['red', 'blue', 'green']
labels = ['normal modes with #quanta=1,-1 and the 0-0 transition',
          'normal modes with #quanta>1,<-1',
          'combination of two normal modes']

S = np.append(1, S)
fq = np.append(0, fq)
if world.rank == 0:
    plt.vlines(fq, 0, S, color='darkblue',
               label='Huang-Rhys factors', linewidth=2.0)

    plt.legend(loc='upper right')
    plt.axis([-1000, 6000, 0, 1.05])
    plt.ylabel('HR factors [a.u.]')
    plt.xlabel('frequency [cm-1]')
    plt.show()

# Plot Franck-Condon factors
FC, f = a.get_Franck_Condon_factors(T, F, order=n)
for l in range(len(FC)):
    plt.vlines(f[l], 0, FC[l], color=colors[l], label=labels[l], linewidth=2.0)

# Fold the spectrum with a gaussian function
width = 300
folding = 'Gauss'
x = [j for j in chain(*f)]
y = [j for j in chain(*FC)]

if world.rank == 0:
    X, Y = Folder(width, folding).fold(x, y)
    plt.plot(X, Y * 750, color='black', linewidth=2.0,
             label='Temperature=' + str(T) + 'K, #quanta=' + str(n) +
             ', width of gaussian=' + str(width) + 'cm^-1',
             linestyle='dashed')

    plt.legend(loc='upper right')
    plt.axis([-1000, 6000, 0, 0.6])
    plt.ylabel('FC factors [a.u.]')
    plt.xlabel('frequency [cm-1]')
    plt.show()
