import math

import numpy as np
import pandas as pd
from scipy import stats
from scipy import optimize
import emcee
import matplotlib.pyplot as plt
import seaborn as sns

%matplotlib inline
clr_plt = sns.color_palette()

"""
Explanation: Bayesian approach with emcee - Test case - 3 free parameters
An example of applying the Bayesian approach with 3 free parameters (erosion rate, time exposure and inheritance), using the emcee package.
For more info about the method used, see the notebook Inference_Notes.
This example (a test case) is based on a generic dataset of 10Be concentration vs. depth, which is drawn from a distribution with given "true" parameters.
This notebook has the following external dependencies:
End of explanation
"""


import models

"""
Explanation: The mathematical (deterministic, forward) model
An implementation of the mathematical model used for predicting profiles of 10Be concentrations is available in the models Python module (see the notebook Models). The 10Be model assumes that the soil density is constant along the depth profile and that the inheritance is the same for the whole sample of 10Be concentration vs. depth.
End of explanation
"""


# the true parameters 
eps_true = 5e-4
t_true = 3e5
rho_true = 2.
inh_true = 5e4

# depths and sample size
depth_minmax = [50, 500]
N = 8

# perturbations
err_magnitude = 20.
err_variability = 5.

"""
Explanation: The data
The dataset is generated using the following parameter values. eps is the erosion rate, t is the exposure time, rho is the soil density and inh is the inheritance.
End of explanation
"""


import gendata

profile_data = gendata.generate_dataset(
    models.C_10Be,
    (eps_true, t_true, rho_true, inh_true),
    zlimits=depth_minmax,
    n=N,
    err=(err_magnitude, err_variability)
)

"""
Explanation: The gendata Python module is used to generate the dataset (see the notebook Datasets).
End of explanation
"""


sns.set_context('notebook')

fig, ax = plt.subplots()

profile_data.plot(
    y='depth', x='C', xerr='std',
    kind="scatter", ax=ax, rot=45
)

ax.invert_yaxis()

"""
Explanation: Make a plot of the dataset
End of explanation
"""


param_names = 'erosion rate', 'time exposure', 'inheritance'

"""
Explanation: The statistical model used for computing the posterior probability density PPD
Here below we define a data model by the tuple m = (eps, t, inh). It correspond to a given location in the 3-d parameter space. The soil density is assumed known.

Define the parameter names. It is important to use the same order to further define the priors and bounds tuples!
End of explanation
"""


param_true = pd.Series((eps_true, t_true, inh_true), index=param_names)

"""
Explanation: Create a pd.Series with the true parameter values. It will be used for plotting purpose.
End of explanation
"""


eps_prior = stats.uniform(loc=0., scale=1e-3)
t_prior = stats.uniform(loc=0., scale=8e5)
inh_prior = stats.uniform(loc=0., scale=1.5e5)

priors = eps_prior, t_prior, inh_prior
param_priors = pd.Series(priors, index=param_names)

"""
Explanation: Define the prior probability distribution for each free parameter. Here the uniform distribution is used, with given bounds (loc and scale arguments of scipy.stats.uniform are the lower bound and the range, respectively)
End of explanation
"""


def get_bounds(f, lower_qtl=0., upper_qtl=1.):
    return f.ppf(lower_qtl), f.ppf(upper_qtl)

eps_bounds = get_bounds(eps_prior, 0, 1)
t_bounds = get_bounds(t_prior, 0, 1)
inh_bounds = get_bounds(inh_prior, 0, 1)

bounds = eps_bounds, t_bounds, inh_bounds
param_bounds = pd.DataFrame(
    np.array(bounds), columns=('min', 'max'), index=param_names
)

param_bounds

"""
Explanation: Define (min, max) bounds for each free parameter. It should be given by lower and upper quantiles (lower_qtl, upper_qtl) of the prior distribution. Choose the extreme quantiles (0, 1) if the distribution is uniform. It will be used for plotting purpose and also for constrained optimization (see below).
End of explanation
"""


fig, axes = plt.subplots(1, 3, figsize=(13, 3))

for ax, p, b, name in zip(axes.flatten(),
                          param_priors.values,
                          param_bounds.values,
                          param_names):
    xmin, xmax = b
    eps = 0.1 * (xmax - xmin)
    x = np.linspace(xmin - eps, xmax + eps, 200)
    d = p.pdf(x)
    ax.plot(x, d)
    ax.fill(x, d, alpha=0.4)
    plt.setp(ax.xaxis.get_majorticklabels(), rotation=45)
    plt.setp(ax, ylim=(0, None), yticklabels=[],
             xlabel=name)

plt.subplots_adjust()

"""
Explanation: Plot the prior probability density for each parameter.
End of explanation
"""


def lnprior(m):
    lps = [p.logpdf(v) for (p, v) in zip(priors, m)]
    if not np.all(np.isfinite(lps)):
        return -np.inf
    return np.sum(lps)

"""
Explanation: Define a function that returns the (logarithm of the) prior probability density for a given data model m.
End of explanation
"""


def lnlike(m):
    eps, t, inh = m
    
    mean = models.C_10Be(profile_data['depth'].values,
                         eps, t, rho_true, inh)
    var = profile_data['std']**2
    
    lngauss = -0.5 * np.sum(
        np.log(2. * np.pi * var) +
        (profile_data['C'] - mean)**2 / var
    )   
    
    return lngauss

"""
Explanation: Define a function that returns the log-likelihood. It is a $n$-dimensional Gaussian ($n$ nucleide concentrations sampled along the depth profile) with the mean given by the formard model and the variance given by the error estimated from the measurements of the nucleide concentration of each sample. This Gaussian implies that (1) the error on each measurement is random, (2) the sampled nucleide concentrations are measured independently of each other, (3) the forward model - i.e., the deterministic model that predicts the nucleide concentration profile - represents the real physics and (4) the values of the non-free parameters of the forward model - e.g., nucleide surface production rate, attenuation lengths... - are exactly known.
End of explanation
"""


def lnprob(m):
    lp = lnprior(m)
    if not np.isfinite(lp):
        return -np.inf
    return lp + lnlike(m)

"""
Explanation: Define a function that returns the log-posterior probability density, according to the Bayes's theorem.
End of explanation
"""


n_params, n_walkers = len(param_names), 100

# randomly choose initial guesses according to the prior
init_guesses = np.array(
    [p.rvs(size=n_walkers) for p in priors]
).T

# perform bounded non-linear optimization from each initial guess
op_lnlike = lambda *args: -lnlike(*args)
init_walkers = np.empty_like(init_guesses)

for i, g in enumerate(init_guesses):
    res = optimize.minimize(op_lnlike, g,
                            method='TNC',
                            bounds=bounds)
    init_walkers[i] = res['x']


"""
Explanation: Sampling the posterior probablility density using MCMC
In our case, the from of the PPD may be highly anisotropic ; it may present high (negative or positive) correlations between its parameters (erosion rate, exposure time, soil density, inheritance). Usually, these relationships are even non-linear.
It is therefore important to use a robust algorithm to sample this complex PPD. The Affine Invariant Markov chain Monte Carlo (MCMC) Ensemble sampler implemented in the emcee package will be more efficient in our case than the standard MCMC algorithms such as the Metropolis-Hasting method.
The emcee sampler allows to define multiple, independent walkers. This requires to first set the initial position of each walker in the parameter space. As shown in the emcee documentation, the author suggests initializing the walkers in a tiny Gaussian ball around the maximum likelihood result. We can obtain the maximum likelihood estimate by applying an optimization algorithm such as one of those implemented in the scipy.optimize module. Note that non-linear optimization usually requires to provide an initial guess.
Given our complex, non-linear, and potentially flat form of the PDD in some areas of the parameter space, we prefer to set the initial positions of the walkers as the maximum likelihood estimates resulting from randomly chosing initial guesses in the parameter space according to the prior probability density. Note that we use a constrained optimization algorithm to ensure that the initial positions are within the bounds defined above.
End of explanation
"""


df_init_guesses = pd.DataFrame(init_guesses, columns=param_names)
df_init_walkers = pd.DataFrame(init_walkers, columns=param_names)

def scatter_pos(xcol, ycol, ax):
    df_init_guesses.plot(
        kind='scatter', x=xcol, y=ycol,
        alpha=0.5, ax=ax, color=clr_plt[0], label='init guesses'
    )
    df_init_walkers.plot(
        kind='scatter', x=xcol, y=ycol,
        alpha=0.8, ax=ax, color=clr_plt[1], label='init walkers'
    )
    legend = ax.legend(frameon=True, loc='lower right')
    legend.get_frame().set_facecolor('w')
    plt.setp(ax, xlim=param_bounds.loc[xcol],
             ylim=param_bounds.loc[ycol])

fig, ax = plt.subplots(2, 2, figsize=(12,12))
scatter_pos('erosion rate', 'time exposure', ax[0][0])
scatter_pos('inheritance', 'time exposure', ax[0][1])
scatter_pos('erosion rate', 'inheritance', ax[1][0])

"""
Explanation: We show below the initial guesses and the initial positions of the walkers in a scatter plot.
End of explanation
"""


sampler = emcee.EnsembleSampler(n_walkers, n_params, lnprob)

n_steps = 500
sampler.run_mcmc(init_walkers, n_steps)

mcmc_samples = pd.DataFrame(sampler.flatchain,
                            columns=param_names)

"""
Explanation: We can then setup the emcee sampler and run the MCMC for n_steps iterations starting from the initial positions defined above.
End of explanation
"""


sample_plot_range = slice(None)

axes = mcmc_samples[sample_plot_range].plot(
    kind='line', subplots=True,
    figsize=(10, 8), color=clr_plt[0]
)

for i, ax in enumerate(axes):
    ax.axhline(param_true.iloc[i], color='r')

"""
Explanation: Let's plot the trace of the MCMC iterations. The red lines show the true values.
End of explanation
"""


nburn = 100

mcmc_kept_samples = pd.DataFrame(
    sampler.chain[:, nburn:, :].reshape((-1, n_params)),
    columns=param_names
)

"""
Explanation: Try plotting only the firsts samples (e.g., sample_plot_range = slice(0, 1000)). We see that thanks to the initial positions of the walkers, the emcee sampler quickly starts exploring the full posterior distribution. The “burn-in” period is small and we can therefore set a small value for nburn below.
End of explanation
"""


def jointplot_density(xcol, ycol):
    p = sns.jointplot(
        xcol, ycol,
        data=mcmc_kept_samples,
        xlim=(mcmc_kept_samples[xcol].min(),
              mcmc_kept_samples[xcol].max()),
        ylim=(mcmc_kept_samples[ycol].min(),
              mcmc_kept_samples[ycol].max()),
        joint_kws={'alpha': 0.02}
    )
    p.ax_joint.axhline(param_true.loc[ycol], color='r')
    p.ax_joint.axvline(param_true.loc[xcol], color='r')

jointplot_density('erosion rate', 'time exposure')
jointplot_density('inheritance', 'time exposure')
jointplot_density('erosion rate', 'inheritance')

"""
Explanation: We can visualize the sampled posterior propbability density by joint plots of the MCMC samples. The red lines show the true values.
End of explanation
"""


mcmc_kept_samples.mean()

"""
Explanation: Given the samples, it is straightforward to characterize the posterior porbability density and estimate its moments.

the PPD mean (if the PPD distribution is strictly gaussian, it also correspond to the MAP (Maximum A-Posterori) and therefore the most probable model)
End of explanation
"""


max_ppd = sampler.lnprobability[:, nburn:].reshape((-1)).argmax()
mcmc_kept_samples.iloc[max_ppd]

"""
Explanation: the sample which have the max PPD value (i.e., the most probable sampled model)
End of explanation
"""


percentiles = np.array([2.5, 5, 25, 50, 75, 95, 97.5])
mcmc_kept_samples.quantile(percentiles * 0.01)

"""
Explanation: the PPD quantiles (useful for delineating the Bayesian confidence intervals or credible intervals for each free parameter)
End of explanation
"""


fig, ax = plt.subplots()

# plot the profile data with error bars
profile_data.plot(
    y='depth', x='C', xerr='std',
    kind="scatter", ax=ax, rot=45
)

# plot 50 randomly chosen profiles from MCMC samples
depths = np.linspace(profile_data['depth'].min(),
                     profile_data['depth'].max(),
                     100)

for i in np.random.randint(len(mcmc_kept_samples), size=100):
    eps, t, inh = mcmc_kept_samples.iloc[i]
    c = models.C_10Be(depths, eps, t, rho_true, inh)
    ax.plot(c, depths, color='grey', alpha=0.1)

# plot the true profile
c_true = models.C_10Be(depths, eps_true, t_true,
                       rho_true, inh_true)
ax.plot(c_true, depths, color='r', label='true model')

ax.invert_yaxis()

"""
Explanation: We finally plot the nucleide concentration profiles (blue dots: data w/ error bars, red line: true profile, grey lines: randomly chosen profiles from MCMC samples).
End of explanation
"""


