"""
Convolution
===========
This example shows how to use the :py:class:`pylops.signalprocessing.Convolve1D`,
:py:class:`pylops.signalprocessing.Convolve2D` and
:py:class:`pylops.signalprocessing.ConvolveND` operators to perform convolution
between two signals.

Such operators can be used in the forward model of several common application
in signal processing that require filtering of an input signal for the
instrument response. Similarly, removing the effect of the instrument
response from signal is equivalent to solving linear system of equations
based on Convolve1D, Convolve2D or ConvolveND operators.
This problem is generally referred to as *Deconvolution*.

A very practical example of deconvolution can be found in the geophysical
processing of seismic data where the effect of the source response
(i.e., airgun or vibroseis) should be removed from the recorded signal
to be able to better interpret the response of the subsurface. Similar examples
can be found in telecommunication and speech analysis.

"""
import matplotlib.pyplot as plt
import numpy as np
from scipy.sparse.linalg import lsqr

import pylops
from pylops.utils.wavelets import ricker

plt.close("all")

###############################################################################
# We will start by creating a zero signal of lenght :math:`nt` and we will
# place a unitary spike at its center. We also create our filter to be
# applied by means of :py:class:`pylops.signalprocessing.Convolve1D` operator.
# Following the seismic example mentioned above, the filter is a
# `Ricker wavelet <http://subsurfwiki.org/wiki/Ricker_wavelet>`_
# with dominant frequency :math:`f_0 = 30 Hz`.
nt = 1001
dt = 0.004
t = np.arange(nt) * dt
x = np.zeros(nt)
x[int(nt / 2)] = 1
h, th, hcenter = ricker(t[:101], f0=30)

Cop = pylops.signalprocessing.Convolve1D(nt, h=h, offset=hcenter, dtype="float32")
y = Cop * x

xinv = Cop / y

fig, ax = plt.subplots(1, 1, figsize=(10, 3))
ax.plot(t, x, "k", lw=2, label=r"$x$")
ax.plot(t, y, "r", lw=2, label=r"$y=Ax$")
ax.plot(t, xinv, "--g", lw=2, label=r"$x_{ext}$")
ax.set_title("Convolve 1d data", fontsize=14, fontweight="bold")
ax.legend()
ax.set_xlim(1.9, 2.1)
plt.tight_layout()

###############################################################################
# We show now that also a filter with mixed phase (i.e., not centered
# around zero) can be applied and inverted for using the
# :py:class:`pylops.signalprocessing.Convolve1D`
# operator.
Cop = pylops.signalprocessing.Convolve1D(nt, h=h, offset=hcenter - 3, dtype="float32")
y = Cop * x
y1 = Cop.H * x
xinv = Cop / y

fig, ax = plt.subplots(1, 1, figsize=(10, 3))
ax.plot(t, x, "k", lw=2, label=r"$x$")
ax.plot(t, y, "r", lw=2, label=r"$y=Ax$")
ax.plot(t, y1, "b", lw=2, label=r"$y=A^Hx$")
ax.plot(t, xinv, "--g", lw=2, label=r"$x_{ext}$")
ax.set_title(
    "Convolve 1d data with non-zero phase filter", fontsize=14, fontweight="bold"
)
ax.set_xlim(1.9, 2.1)
ax.legend()
plt.tight_layout()

###############################################################################
# We repeat a similar exercise but using two dimensional signals and
# filters taking advantage of the
# :py:class:`pylops.signalprocessing.Convolve2D` operator.
nt = 51
nx = 81
dt = 0.004
t = np.arange(nt) * dt
x = np.zeros((nt, nx))
x[int(nt / 2), int(nx / 2)] = 1

nh = [11, 5]
h = np.ones((nh[0], nh[1]))

Cop = pylops.signalprocessing.Convolve2D(
    (nt, nx),
    h=h,
    offset=(int(nh[0]) / 2, int(nh[1]) / 2),
    dtype="float32",
)
y = Cop * x
xinv = (Cop / y.ravel()).reshape(Cop.dims)

fig, axs = plt.subplots(1, 3, figsize=(10, 3))
fig.suptitle("Convolve 2d data", fontsize=14, fontweight="bold", y=0.95)
axs[0].imshow(x, cmap="gray", vmin=-1, vmax=1)
axs[1].imshow(y, cmap="gray", vmin=-1, vmax=1)
axs[2].imshow(xinv, cmap="gray", vmin=-1, vmax=1)
axs[0].set_title("x")
axs[0].axis("tight")
axs[1].set_title("y")
axs[1].axis("tight")
axs[2].set_title("xlsqr")
axs[2].axis("tight")
plt.tight_layout()
plt.subplots_adjust(top=0.8)

fig, ax = plt.subplots(1, 2, figsize=(10, 3))
fig.suptitle("Convolve in 2d data - traces", fontsize=14, fontweight="bold", y=0.95)
ax[0].plot(x[int(nt / 2), :], "k", lw=2, label=r"$x$")
ax[0].plot(y[int(nt / 2), :], "r", lw=2, label=r"$y=Ax$")
ax[0].plot(xinv[int(nt / 2), :], "--g", lw=2, label=r"$x_{ext}$")
ax[1].plot(x[:, int(nx / 2)], "k", lw=2, label=r"$x$")
ax[1].plot(y[:, int(nx / 2)], "r", lw=2, label=r"$y=Ax$")
ax[1].plot(xinv[:, int(nx / 2)], "--g", lw=2, label=r"$x_{ext}$")
ax[0].legend()
ax[0].set_xlim(30, 50)
ax[1].legend()
ax[1].set_xlim(10, 40)
plt.tight_layout()
plt.subplots_adjust(top=0.8)

###############################################################################
# Finally we do the same using three dimensional signals and
# filters taking advantage of the
# :py:class:`pylops.signalprocessing.ConvolveND` operator.
ny, nx, nz = 13, 10, 7
x = np.zeros((ny, nx, nz))
x[ny // 3, nx // 2, nz // 4] = 1
h = np.ones((3, 5, 3))
offset = [1, 2, 1]

Cop = pylops.signalprocessing.ConvolveND(
    dims=(ny, nx, nz), h=h, offset=offset, axes=(0, 1, 2), dtype="float32"
)
y = Cop * x
xlsqr = lsqr(Cop, y.ravel(), damp=0, iter_lim=300, show=0)[0]
xlsqr = xlsqr.reshape(Cop.dims)

fig, axs = plt.subplots(3, 3, figsize=(10, 12))
fig.suptitle("Convolve 3d data", y=0.95, fontsize=14, fontweight="bold")
axs[0][0].imshow(x[ny // 3], cmap="gray", vmin=-1, vmax=1)
axs[0][1].imshow(y[ny // 3], cmap="gray", vmin=-1, vmax=1)
axs[0][2].imshow(xlsqr[ny // 3], cmap="gray", vmin=-1, vmax=1)
axs[0][0].set_title("x")
axs[0][0].axis("tight")
axs[0][1].set_title("y")
axs[0][1].axis("tight")
axs[0][2].set_title("xlsqr")
axs[0][2].axis("tight")
axs[1][0].imshow(x[:, nx // 2], cmap="gray", vmin=-1, vmax=1)
axs[1][1].imshow(y[:, nx // 2], cmap="gray", vmin=-1, vmax=1)
axs[1][2].imshow(xlsqr[:, nx // 2], cmap="gray", vmin=-1, vmax=1)
axs[1][0].axis("tight")
axs[1][1].axis("tight")
axs[1][2].axis("tight")
axs[2][0].imshow(x[..., nz // 4], cmap="gray", vmin=-1, vmax=1)
axs[2][1].imshow(y[..., nz // 4], cmap="gray", vmin=-1, vmax=1)
axs[2][2].imshow(xlsqr[..., nz // 4], cmap="gray", vmin=-1, vmax=1)
axs[2][0].axis("tight")
axs[2][1].axis("tight")
axs[2][2].axis("tight")
plt.tight_layout()