import os
import numpy as np
from polsartools.utils.proc_utils import process_chunks_parallel
from polsartools.utils.utils import conv2d,time_it
from .cp_infiles import cpc2files
[docs]
@time_it
def mf3cc(in_dir, chi=45, psi=0, win=1, fmt="tif", cog=False,
ovr = [2, 4, 8, 16], comp=False,
max_workers=None,block_size=(512, 512),
progress_callback=None # for QGIS plugin
):
"""Perform Model-Free 3-Component Decomposition for compact-pol SAR data.
This function implements the model-free three-component decomposition for
compact-polarimetric SAR data, decomposing the total backscattered power into
surface (Ps), double-bounce (Pd), and volume (Pv) scattering components, along
with the scattering-type parameter (Theta_CP).
Examples
--------
>>> # Basic usage with default parameters
>>> mf3cc("/path/to/cp_data")
>>> # Advanced usage with custom parameters
>>> mf3cc(
... in_dir="/path/to/cp_data",
... chi=-45,
... win=5,
... fmt="tif",
... cog=True,
... block_size=(1024, 1024)
... )
Parameters
----------
in_dir : str
Path to the input folder containing compact-pol C2 matrix files.
chi : float, default=45
Ellipticity angle chi of the transmitted wave in degrees.
For circular polarization, chi = 45° (right circular) or -45° (left circular).
psi : float, default=0
Orientation angle psi of the transmitted wave in degrees.
For circular polarization, typically 0°.
win : int, default=1
Size of the spatial averaging window. Larger windows reduce speckle noise
but decrease spatial resolution.
fmt : {'tif', 'bin'}, default='tif'
Output file format:
- 'tif': GeoTIFF format with georeferencing information
- 'bin': Raw binary format
cog : bool, default=False
If True, creates Cloud Optimized GeoTIFF (COG) outputs with internal tiling
and overviews for efficient web access.
ovr : list[int], default=[2, 4, 8, 16]
Overview levels for COG creation. Each number represents the
decimation factor for that overview level.
comp : bool, default=False
If True, applies LZW compression to the output GeoTIFF files.
max_workers : int | None, default=None
Maximum number of parallel processing workers. If None, uses
CPU count - 1 workers.
block_size : tuple[int, int], default=(512, 512)
Size of processing blocks (rows, cols) for parallel computation.
Larger blocks use more memory but may be more efficient.
Returns
-------
None
Writes four output files to disk:
1. Ps_mf3cc: Surface scattering power component
2. Pd_mf3cc: Double-bounce scattering power component
3. Pv_mf3cc: Volume scattering power component
4. Theta_CP_mf3cc: Scattering-type parameter
"""
write_flag=True
input_filepaths = cpc2files(in_dir)
output_filepaths = []
if fmt == "bin":
output_filepaths.append(os.path.join(in_dir, "Ps_mf3cc.bin"))
output_filepaths.append(os.path.join(in_dir, "Pd_mf3cc.bin"))
output_filepaths.append(os.path.join(in_dir, "Pv_mf3cc.bin"))
output_filepaths.append(os.path.join(in_dir, "Theta_CP_mf3cc.bin"))
else:
output_filepaths.append(os.path.join(in_dir, "Ps_mf3cc.tif"))
output_filepaths.append(os.path.join(in_dir, "Pd_mf3cc.tif"))
output_filepaths.append(os.path.join(in_dir, "Pv_mf3cc.tif"))
output_filepaths.append(os.path.join(in_dir, "Theta_CP_mf3cc.tif"))
process_chunks_parallel(input_filepaths, list(output_filepaths),
win,
write_flag,
process_chunk_mf3cc,
*[chi, psi],
block_size=block_size,
max_workers=max_workers,
num_outputs=len(output_filepaths),
cog=cog, ovr=ovr, comp=comp,
progress_callback=progress_callback
)
def process_chunk_mf3cc(chunks, window_size, *args, **kwargs):
chi=args[-2]
psi=args[-1]
# print(chi,psi):
kernel = np.ones((window_size,window_size),np.float32)/(window_size*window_size)
c11_T1 = np.array(chunks[0])
c12_T1 = np.array(chunks[1])+1j*np.array(chunks[2])
c21_T1 = np.conj(c12_T1)
c22_T1 = np.array(chunks[3])
ncols,nrows = np.shape(c11_T1)
if window_size>1:
c11_T1 = conv2d(np.real(c11_T1),kernel)+1j*conv2d(np.imag(c11_T1),kernel)
c12_T1 = conv2d(np.real(c12_T1),kernel)+1j*conv2d(np.imag(c12_T1),kernel)
c21_T1 = conv2d(np.real(c21_T1),kernel)+1j*conv2d(np.imag(c21_T1),kernel)
c22_T1 = conv2d(np.real(c22_T1),kernel)+1j*conv2d(np.imag(c22_T1),kernel)
c2_det = (c11_T1*c22_T1-c12_T1*c21_T1)
c2_trace = c11_T1+c22_T1
# t2_span = t11s*t22s
m1 = np.real(np.sqrt(1.0-(4.0*c2_det/np.power(c2_trace,2))))
# Compute Stokes parameters
s0 = c11_T1 + c22_T1
s1 = c11_T1 - c22_T1
s2 = np.real(c12_T1 + c21_T1)
s3 = np.where(chi >= 0, 1j * (c12_T1 - c21_T1), -1j * (c12_T1 - c21_T1))
s3 = np.real(s3)
SC = ((s0)-(s3))/2;
OC = ((s0)+(s3))/2;
h = (OC-SC)
# span = c11s + c22s
val = ((m1*s0*h))/((SC*OC + (m1**2)*(s0**2)))
thet = np.real(np.arctan(val))
theta_CP = np.rad2deg(thet)
Ps_CP= (((m1*(c2_trace)*(1.0+np.sin(2*thet))/2)))
Pd_CP= (((m1*(c2_trace)*(1.0-np.sin(2*thet))/2)))
Pv_CP= (c2_trace*(1.0-m1))
return Ps_CP.astype(np.float32), Pd_CP.astype(np.float32), Pv_CP.astype(np.float32), theta_CP.astype(np.float32)
