#!/usr/bin/env python
"""
    This seems to work for fcc and bcc and sc

    Things to figure out:
        * why multiply strain on right
        * why we can't use changing volumes
        * why diamond doesn't agree between cubic True and False

"""

import ase
from ase.structure import bulk
import numpy as np
import scipy.optimize as opt
import numdifftools as ndt
from kimcalculator import *
from scipy.optimize import fmin
import simplejson
import sys
import json
import jinja2

class ElasticConstants(object):
    """Determine the cubic elastic constants by numerically determining the Hessian"""

    def __init__(self, calc, element, potentialname, crystalstructure, latticeconst):
        self.calculator = calc
        self.element = element
        self.potentialname = potentialname
        self.crystalstructure = crystalstructure
        self.latticeconst = latticeconst
        self.slab = self.create_slab()
        self.o_cell = self.slab.get_cell()
        self.slab.set_calculator(self.calculator)
        self.o_volume = self.slab.get_volume()

    def create_slab(self):
        slab = bulk(self.element,a=self.latticeconst,crystalstructure=self.crystalstructure,cubic=True)
        return slab

    def voigt_to_matrix(self,voigt_vec):
        """Convert a voigt notation vector to a matrix """
        matrix = np.zeros((3,3))
        matrix[0,0] = voigt_vec[0]
        matrix[1,1] = voigt_vec[1]
        matrix[2,2] = voigt_vec[2]
        matrix[ [ [1,2], [2,1] ] ] = voigt_vec[3]
        matrix[ [ [0,2], [2,0] ] ] = voigt_vec[4]
        matrix[ [ [0,1], [1,0] ] ] = voigt_vec[5]

        return matrix

    def energy_from_strain(self,strain_vec):
        """ Apply a strain according to the strain_vec """
        # self.slab = self.o_slab.copy()
        # print strain_vec
        strain_mat = self.voigt_to_matrix(strain_vec)
        old_cell = self.o_cell
        new_cell = old_cell + np.dot(old_cell, strain_mat)
        # new_cell = old_cell + np.einsum('ij,aj->ai',strain_mat,old_cell)
        self.slab.set_cell(new_cell,scale_atoms=True)
        energy = self.slab.get_potential_energy()
        # volume = self.slab.get_volume()
        # n_of_atoms = self.slab.get_number_of_atoms()

        return (energy/self.o_volume)/ase.units.GPa

    def energy_from_scale(self,scale):
        # strain_mat = np.eye(3) * (scale)
        old_cell = self.o_cell
        # new_cell = old_cell + np.dot( strain_mat, old_cell)
        new_cell = old_cell * (1 + scale)
        self.slab.set_cell(new_cell,scale_atoms=True)
        energy = self.slab.get_potential_energy()
        # volume = self.slab.get_volume()
        # n_of_atoms = self.slab.get_number_of_atoms()
        return energy

    def results(self):
        """ Return the cubic elastic constants """
        #get the minimum
        self.minscale = float(fmin(self.energy_from_scale,0,xtol=0,ftol=1e-7))
        self.oo_cell = self.o_cell.copy()
        self.o_cell = self.o_cell * (1+self.minscale)

        func = self.energy_from_strain
        hess = ndt.Hessian(func)

        elastic_constants = hess(np.zeros(6))
        error_estimate = hess.error_estimate

        inds11 = [[0,1,2],[0,1,2]]
        C11 = elastic_constants[ inds11 ].mean()
        C11sig = np.sqrt( ((1./3*error_estimate[ inds11 ])**2).sum() )

        inds12 = [[1,2,2,0,0,1],[0,0,1,1,2,2]]
        C12 = ( elastic_constants[inds12].mean() )
        C12sig = np.sqrt( ((1./6*error_estimate[inds12])**2).sum() )

        inds44 = [[3,4,5],[3,4,5]]
        C44 = 1./4 * elastic_constants[inds44].mean()
        C44sig = 1./4 * np.sqrt( ((1./3*error_estimate[inds44])**2).sum() )

        B = 1./3 * ( C11 + 2 * C12 )
        Bsig = np.sqrt( ( 1./3 * C11sig )**2 + ( 2./3 * C12sig )**2 )

        excessinds = [[3,4,5,3,4,5,3,4,5,0,1,2,4,5,0,1,2,3,5,0,1,2,3,4],
                [0,0,0,1,1,1,2,2,2,3,3,3,3,3,4,4,4,4,4,5,5,5,5,5]]
        excess =(np.abs(elastic_constants[excessinds]).mean() )
        excess_sig = np.sqrt( ((1./24*error_estimate[excessinds])**2).sum() )

        results_dict = { 'C11': C11,
                         'C11_sig' : C11sig,
                         'C12' : C12,
                         'C12_sig' : C12sig,
                         'C44': C44,
                         'C44_sig' : C44sig,
                         'B' : B,
                         'B_sig' : Bsig,
                         'excess': excess,
                         'excess_sig' : excess_sig,
                         'units' : 'GPa',
                         "element": symbol,
                         "crystal_structure": lattice,
                         "space_group": space_groups[lattice],
                         "wyckoff_code": wyckoff_codes[lattice],
                         "lattice_constant": self.latticeconst,
                         "scale_discrepency": self.minscale,
                         }

        return results_dict

symbol  = raw_input()
lattice = raw_input()
model   = raw_input()
latticeconst_result = raw_input()
# symbol  = 'Fe'
# lattice = 'diamond'
# model   = 'EAM_Dynamo_Ackland_Bacon_Fe__MO_142799717516_000'
# latticeconst_result = 2.86652799316e-10

space_groups = {"fcc": "Fm-3m", "bcc": "Im-3m", "sc": "Pm-3m", "diamond": "Fd-3m"}
wyckoff_codes = {"fcc": "4a", "bcc": "2a", "sc": "1a", "diamond": "8a"}
normed_basis = { 
    lattice: json.dumps(bulk(symbol, lattice, a=1, cubic=True).positions.tolist(), separators=(' ', ' '))
    for lattice in space_groups.keys() 
}

latticeconst = float(latticeconst_result) * 1e10

print symbol, lattice, model, latticeconst

calc = KIMCalculator(model)
# import ase.calculators
# calc = ase.calculators.emt.EMT()
bulkmodulus = ElasticConstants(calc, symbol, model, lattice, latticeconst)
results = bulkmodulus.results()
results.update({"basis_coordinates": normed_basis[lattice]})

template_environment = jinja2.Environment(
    loader=jinja2.FileSystemLoader('/'),
    block_start_string='@[',
    block_end_string=']@',
    variable_start_string='@<',
    variable_end_string='>@',
    comment_start_string='@#',
    comment_end_string='#@',
    undefined=jinja2.StrictUndefined,
    )

#template the EDN output
with open(os.path.abspath("output/results.edn"), "w") as f:
    template = template_environment.get_template(os.path.abspath("results.edn.tpl"))
    f.write(template.render(**results))