diff --git a/BP_Fawad_v1.py b/BP_Fawad_v1.py
new file mode 100644
index 0000000..70c36ae
--- /dev/null
+++ b/BP_Fawad_v1.py
@@ -0,0 +1,325 @@
+#!/usr/bin/env python
+
+""" ============================================
+    SRP: SAR Raw data Processor (:mod:`srp`)
+    ============================================
+
+    Script to process SAR RAW data
+
+    **Arguments**
+        * -c, --cfg_file: Configuration file
+        * -r, --raw_file: Raw data file
+        * -o, --output_file: Output file
+
+"""
+
+import os
+import time
+import argparse
+
+import numpy as np
+from matplotlib import pyplot as plt
+
+from oceansar.utils import geometry as geo
+from oceansar import utils
+from back_projection_func import back_projection
+from oceansar import ocs_io as tpio
+from oceansar import constants as const
+from oceansar.radarsim.antenna import sinc_1tx_nrx, sinc_bp
+
+
+def sar_focus(cfg_file, raw_output_file, output_file):
+
+    ###################
+    # INITIALIZATIONS #
+    ###################
+
+    print('-------------------------------------------------------------------')
+    print(time.strftime("- OCEANSAR SAR Processor: %Y-%m-%d %H:%M:%S", time.localtime()))
+    print('-------------------------------------------------------------------')
+
+    # CONFIGURATION FILE
+    cfg = tpio.ConfigFile(cfg_file)
+
+    # PROCESSING
+    az_weighting = cfg.processing.az_weighting
+    doppler_bw = cfg.processing.doppler_bw
+    plot_format = cfg.processing.plot_format
+    plot_tex = cfg.processing.plot_tex
+    plot_save = cfg.processing.plot_save
+    plot_path = cfg.processing.plot_path
+    plot_raw = cfg.processing.plot_raw
+    plot_rcmc_dopp = cfg.processing.plot_rcmc_dopp
+    plot_rcmc_time = cfg.processing.plot_rcmc_time
+    plot_image_valid = cfg.processing.plot_image_valid
+
+    # SAR
+    f0 = cfg.sar.f0
+    prf = cfg.sar.prf
+    num_ch = cfg.sar.num_ch
+    alt = cfg.sar.alt
+    v_ground = cfg.sar.v_ground
+    rg_bw = cfg.sar.rg_bw
+    over_fs = cfg.sar.over_fs
+
+    # CALCULATE PARAMETERS
+    l0 = const.c / f0
+    if v_ground == 'auto':
+        v_ground = geo.orbit_to_vel(alt, ground=True)
+    rg_sampling = rg_bw * over_fs
+
+    # RAW DATA
+    raw_file = tpio.RawFile(raw_output_file, 'r')
+    raw_data = raw_file.get('raw_data*')
+    sr0 = raw_file.get('sr0')
+    inc_angle = raw_file.get('inc_angle')
+    b_ati = raw_file.get('b_ati')
+    b_xti = raw_file.get('b_xti')
+    raw_file.close()
+
+    
+    # OTHER INITIALIZATIONS
+    # Create plots directory
+    plot_path = os.path.dirname(output_file) + os.sep + plot_path
+    if plot_save:
+        if not os.path.exists(plot_path):
+            os.makedirs(plot_path)
+
+    slc = []
+    BP = 1
+    ########################
+    # PROCESSING MAIN LOOP #
+    ########################
+    for ch in np.arange(num_ch):
+
+        if plot_raw:
+            plt.figure()
+            plt.imshow(np.real(raw_data[0, ch]),
+                       vmin=-np.max(np.abs(raw_data[0, ch])),
+                       vmax=np.max(np.abs(raw_data[0, ch])), cmap='gray')
+            plt.savefig(plot_path + os.sep + ('plot_raw_real_%d.%s' % (ch, plot_format)))
+            plt.close()
+            
+        if BP ==1:
+                    # Getting each channel data
+            az_size_orig, rg_size_orig = raw_data[0, 0].shape
+            backscatter = np.zeros((num_ch, az_size_orig, rg_size_orig)) 
+            az_size_orig, rg_size_orig = raw_data[0, ch].shape  # az 142 and rg 97
+            data = np.zeros((az_size_orig, rg_size_orig), dtype=complex)  #Initialization 2D, ( az, rg)
+            data = raw_data[0, ch, :, :]    
+            backscatter[ch, :, :] = back_projection(data, prf, f0, v_ground, sr0, rg_sampling)
+            
+            # Removal of non valid samples
+            n_val_az_2 = np.floor(
+            doppler_bw / 2. / (2. * v_ground**2. / l0 / sr0) * prf / 2.) * 2.
+            reduced = backscatter[ch, int(n_val_az_2):int(az_size_orig - n_val_az_2 - 1), :]
+            print(reduced.shape)
+        
+            idx_reduced_azi = np.sum(np.abs(reduced), axis=1)
+            intensity_BP = np.abs((reduced[np.argmax(idx_reduced_azi), :]))  #Sliced at Max Azimuth
+            plt.figure()
+            plt.imshow(np.abs(reduced), origin='lower', vmin=0, vmax=np.max(np.abs(reduced)),
+                       aspect=float(rg_size_orig) / float(az_size_orig),
+                       cmap='gray')
+            plt.xlabel("Range")
+            plt.title("Reduced BP")
+            plt.ylabel("Azimuth")
+            
+           
+           
+
+        # Optimize matrix sizes
+        az_size_orig, rg_size_orig = raw_data[0, ch].shape
+        optsize = utils.optimize_fftsize(raw_data[0, ch].shape)
+        optsize = [raw_data.shape[0], optsize[0], optsize[1]]
+        data = np.zeros(optsize, dtype=complex)
+        data[:, :raw_data[0, ch].shape[0],
+       :raw_data[0, ch].shape[1]] = raw_data[:, ch, :, :]
+        az_size, rg_size = data.shape[1:]
+   
+                         
+        # RCMC Correction
+        print('Applying RCMC correction... [Channel %d/%d]' % (ch + 1, num_ch))
+ 
+        fr = np.fft.fftfreq(rg_size, 1/rg_sampling)
+        fa = np.fft.fftfreq(az_size, 1/prf)
+        ## Compensation of ANTENNA PATTERN
+        ## FIXME this will not work for a long separation betwen Tx and Rx!!!
+        sin_az = fa * l0 / (2 * v_ground)
+        if hasattr(cfg.sar, 'ant_L'):
+            ant_L = cfg.sar.ant_L
+            if cfg.sar.L_total:
+                beam_pattern = sinc_1tx_nrx(sin_az, ant_L * num_ch, f0, num_ch, field=True)
+            else:
+                beam_pattern = sinc_1tx_nrx(sin_az, ant_L, f0, 1, field=True)
+        else:
+            ant_l_tx = cfg.sar.ant_L_tx
+            ant_l_rx = cfg.sar.ant_L_rx
+            beam_pattern = (sinc_bp(sin_az, ant_l_tx, f0, field=True)
+                            * sinc_bp(sin_az, ant_l_rx, f0, field=True))
+
+
+        #fa[az_size/2:] = fa[az_size/2:] - prf
+        rcmc_fa = sr0 / np.sqrt(1 - (fa * (l0 / 2.) / v_ground)**2.) - sr0
+        data = np.fft.fft(np.fft.fft(data, axis=-1), axis=-2)
+       
+#        for i in np.arange(az_size):
+#            data[i,:] *= np.exp(1j*2*np.pi*2*rcmc_fa[i]/const.c*fr)
+        data = (data * np.exp(4j * np.pi * rcmc_fa.reshape((1, az_size, 1)) /
+                              const.c * fr.reshape((1, 1, rg_size))))
+    
+        data = np.fft.ifft(data, axis=2)
+       
+        if plot_rcmc_dopp:
+            plt.figure()
+            plt.imshow(np.fft.fftshift(np.abs(data[0]), axes=0), vmax=np.max(np.abs(data)), cmap='gray',
+                       origin='lower')
+            plt.savefig(plot_path + os.sep + ('plot_rcmc_dopp_%d.%s' % (ch, plot_format)))
+            plt.close()
+
+        if plot_rcmc_time:
+            rcmc_time = np.fft.ifft(data[0], axis=0)[
+                :az_size_orig, :rg_size_orig]
+            rcmc_time_max = np.max(np.abs(rcmc_time))
+            plt.figure()
+            plt.imshow(np.real(rcmc_time), vmin=-rcmc_time_max, vmax=rcmc_time_max, cmap='gray',
+                       origin='lower')
+            plt.savefig(plot_path + os.sep + ('plot_rcmc_time_real_%d.%s' % (ch, plot_format)))
+            plt.close()
+
+        # Azimuth compression
+        print(
+            'Applying azimuth compression... [Channel %d/%d]' % (ch + 1, num_ch))
+
+        n_samp = 2 * (int(doppler_bw / (fa[1] - fa[0])) / 2)
+        weighting = (az_weighting -
+                     (1. - az_weighting) * np.cos(2 * np.pi * np.linspace(0, 1., int(n_samp))))
+        # Compensate amplitude loss
+
+        L_win = np.sum(np.abs(weighting)**2) / weighting.size
+        weighting /= np.sqrt(L_win)
+        if fa.size > n_samp:
+            zeros = np.zeros(az_size)
+            zeros[0:int(n_samp)] = weighting
+            weighting = np.roll(zeros, int(-n_samp / 2))
+        weighting = np.where(np.abs(beam_pattern) > 0, weighting/beam_pattern, 0)
+        ph_ac = 4. * np.pi / l0 * sr0 * \
+            (np.sqrt(1. - (fa * l0 / 2. / v_ground)**2.) - 1.)
+  
+        data = data * (np.exp(1j * ph_ac) * weighting).reshape((1, az_size, 1))
+  
+        #=====================================
+        data = np.fft.ifft(data, axis=1)
+        
+        print(data.shape)
+        
+        print('Finishing... [Channel %d/%d]' % (ch + 1, num_ch))
+
+
+        # Reduce to initial dimension
+        data = data[:, :int(az_size_orig), :int(rg_size_orig)]
+        print(data.shape)
+        # Removal of non valid samples
+        n_val_az_2 = np.floor(
+            doppler_bw / 2. / (2. * v_ground**2. / l0 / sr0) * prf / 2.) * 2.
+        # data = raw_data[ch, n_val_az_2:(az_size_orig - n_val_az_2 - 1), :]
+        data = data[:, int(n_val_az_2):int(az_size_orig - n_val_az_2 - 1), :]
+        
+        
+        print(ch)
+        print(data.shape)
+        if plot_image_valid:
+            plt.figure()
+            plt.imshow(np.abs(data[0]), origin='lower', vmin=0, vmax=np.max(np.abs(data)),
+                       aspect=float(rg_size_orig) / float(az_size_orig),
+                       cmap='gray')
+            plt.xlabel("Range")
+            plt.ylabel("Azimuth")
+            plt.savefig(os.path.join(
+            plot_path, ('plot_image_valid_%d.%s' % (ch, plot_format)))) 
+            
+            
+            
+            
+            
+        ##### INTENSITY PLOT at MAX Azimuth Position
+        range_resolution = const.c / (2 * rg_sampling)
+        azimuth_resolution = v_ground/prf
+        print (range_resolution)
+        print (azimuth_resolution)
+        
+        intensity_grid = np.abs(data[0]) #for frequency based
+        azimuth_intensity_sum = np.sum(intensity_grid, axis=1)
+        intensity_Freqbased = (intensity_grid[np.argmax(azimuth_intensity_sum), :])
+        
+        plt.figure(figsize=(10, 5))
+        plt.plot(np.abs(intensity_Freqbased), label='Frequency-Based Intensity')
+        plt.plot(np.abs(intensity_BP), label='Back-Projection Intensity')
+        plt.xlabel('Range Bin')
+        plt.ylabel('Magnitude')
+        plt.grid()
+        plt.legend()  # Place this before plt.show()
+        
+          
+
+        # IN dB and X axis in Meters
+        range_bins = np.arange(intensity_BP.size)
+        range_resolution = const.c / (2 * rg_sampling)
+        range_distances = range_bins * range_resolution
+        intensity_Freqbased_dB = 10 * np.log10(np.abs(intensity_Freqbased) + 1e-6)
+        intensity_BP_dB = 10 * np.log10(np.abs(intensity_BP) + 1e-6)
+                
+        plt.figure(figsize=(10, 6))
+        plt.plot(range_distances, intensity_Freqbased_dB, label="Freq. Based Algo.")
+        plt.plot(range_distances, intensity_BP_dB, label="BP Algo.")
+        plt.title("Intensity Across Range Distances at Maximum Intensity Azimuth Index")
+        plt.xlabel("Range Distance (meters)")
+        plt.ylabel("Intensity (dB)")
+        plt.legend()
+        plt.grid()
+        plt.show()
+        
+        ####
+      
+        
+        
+        slc.append(data)
+    
+    
+
+    # Save processed data
+    slc = np.array(slc, dtype=complex)
+    print("Shape of SLC: " + str(slc.shape), flush=True)
+   
+    proc_file = tpio.ProcFile(output_file, 'w', slc.shape)
+    proc_file.set('slc*', slc)
+    proc_file.set('inc_angle', inc_angle)
+    proc_file.set('f0', f0)
+    proc_file.set('num_ch', num_ch)
+    proc_file.set('ant_L', ant_l_tx)
+    proc_file.set('prf', prf)
+    proc_file.set('v_ground', v_ground)
+    proc_file.set('orbit_alt', alt)
+    proc_file.set('sr0', sr0)
+    proc_file.set('rg_sampling', rg_bw*over_fs)
+    proc_file.set('rg_bw', rg_bw)
+    proc_file.set('b_ati', b_ati)
+    proc_file.set('b_xti', b_xti)
+    proc_file.close()
+
+    print('-----------------------------------------')
+    print(time.strftime(
+        "Processing finished [%Y-%m-%d %H:%M:%S]", time.localtime()))
+    print('-----------------------------------------')
+
+
+if __name__ == '__main__':
+
+    # INPUT ARGUMENTS
+    parser = argparse.ArgumentParser()
+    parser.add_argument('-c', '--cfg_file')
+    parser.add_argument('-r', '--raw_file')
+    parser.add_argument('-o', '--output_file')
+    args = parser.parse_args()
+
+    sar_focus(args.cfg_file, args.raw_file, args.output_file)
diff --git a/back_projection_func.py b/back_projection_func.py
new file mode 100644
index 0000000..d01a29c
--- /dev/null
+++ b/back_projection_func.py
@@ -0,0 +1,63 @@
+import numpy as np
+import matplotlib.pyplot as plt
+from scipy import interpolate
+from scipy import stats
+
+def filter_on_peak(size, peak_index, alpha=4):
+    x = np.arange(size) - peak_index
+    sinc_filter = np.sinc(x / alpha)
+    return sinc_filter
+
+def back_projection(data, prf, f0, v_ground, sr0, rg_sampling):
+    c = 3e8
+    az_size, rg_size = data.shape
+    wavelength = c / f0
+    kr = 2 * np.pi / wavelength
+    epsilon = 1e-6
+
+    image_grid = np.zeros((az_size, rg_size), dtype=complex)  
+    peak_range_idx = np.bincount(np.argmax(np.abs(data), axis=1)).argmax() 
+    sinc_filter_window = filter_on_peak(rg_size, peak_range_idx)
+    print(peak_range_idx)
+    middle_azimuth_idx = (az_size // 2)+1 
+    ##### MAIN LOOP ####
+    for az_idx in range(az_size):
+        range_vector = data[az_idx, :] * sinc_filter_window
+        range_vector *= np.max(np.abs(data[az_idx, :])) / np.max(np.abs(range_vector)) #Amp. compensation
+        azimuth_time = az_idx / prf 
+
+        d_az = v_ground * azimuth_time #Azi displace.
+
+        for y in range(rg_size):
+            range_distance = sr0 + y * rg_sampling
+            slant_range = np.sqrt(d_az**2 + range_distance**2)
+            # Note: Since d_az is very small that makes range and slant range almost equal. 
+            # Increasing v_ground or azimuth_time will make impact, To verify i have added epsilon
+            #slant_range = np.sqrt(d_az**2 + range_distance**2) +epsilon
+            rg_bin_float = (slant_range - sr0) / rg_sampling
+            rg_bin = int(np.floor(rg_bin_float))
+            weight = rg_bin_float - rg_bin
+            if 0 <= rg_bin < rg_size - 1:
+                interpolated_value = (
+                    (1 - weight) * range_vector[rg_bin] + weight * range_vector[rg_bin + 1]
+                )
+                
+                phase_correction = np.exp(1j * kr * (slant_range - range_distance))
+                contribution = interpolated_value * phase_correction
+                """print("Contribution:", contribution)
+                print("Range Vector Value:", range_vector[rg_bin])
+                print("Difference (slant_range - range_distance):", slant_range - range_distance)
+                print("Phase of Contribution:", np.angle(contribution))
+                print("Phase of Range Vector Value:", np.angle(range_vector[rg_bin]))
+                print("Phase Difference:", np.angle(contribution) - np.angle(range_vector[rg_bin]))"""                
+                image_grid[middle_azimuth_idx, y] += contribution
+
+    """plt.plot(np.abs(data[:, peak_range_idx]))
+    plt.plot(np.abs(image_grid[middle_azimuth_idx, :])) 
+    plt.xlabel('Range Index')
+    plt.ylabel('Magnitude')
+    plt.title('Accumulated Magnitude at Middle Azimuth Row')
+    plt.grid(True)
+    plt.show()"""
+
+    return image_grid
diff --git a/oceansar/radarsim/BP_Fawad_v1.py b/oceansar/radarsim/BP_Fawad_v1.py
new file mode 100644
index 0000000..70c36ae
--- /dev/null
+++ b/oceansar/radarsim/BP_Fawad_v1.py
@@ -0,0 +1,325 @@
+#!/usr/bin/env python
+
+""" ============================================
+    SRP: SAR Raw data Processor (:mod:`srp`)
+    ============================================
+
+    Script to process SAR RAW data
+
+    **Arguments**
+        * -c, --cfg_file: Configuration file
+        * -r, --raw_file: Raw data file
+        * -o, --output_file: Output file
+
+"""
+
+import os
+import time
+import argparse
+
+import numpy as np
+from matplotlib import pyplot as plt
+
+from oceansar.utils import geometry as geo
+from oceansar import utils
+from back_projection_func import back_projection
+from oceansar import ocs_io as tpio
+from oceansar import constants as const
+from oceansar.radarsim.antenna import sinc_1tx_nrx, sinc_bp
+
+
+def sar_focus(cfg_file, raw_output_file, output_file):
+
+    ###################
+    # INITIALIZATIONS #
+    ###################
+
+    print('-------------------------------------------------------------------')
+    print(time.strftime("- OCEANSAR SAR Processor: %Y-%m-%d %H:%M:%S", time.localtime()))
+    print('-------------------------------------------------------------------')
+
+    # CONFIGURATION FILE
+    cfg = tpio.ConfigFile(cfg_file)
+
+    # PROCESSING
+    az_weighting = cfg.processing.az_weighting
+    doppler_bw = cfg.processing.doppler_bw
+    plot_format = cfg.processing.plot_format
+    plot_tex = cfg.processing.plot_tex
+    plot_save = cfg.processing.plot_save
+    plot_path = cfg.processing.plot_path
+    plot_raw = cfg.processing.plot_raw
+    plot_rcmc_dopp = cfg.processing.plot_rcmc_dopp
+    plot_rcmc_time = cfg.processing.plot_rcmc_time
+    plot_image_valid = cfg.processing.plot_image_valid
+
+    # SAR
+    f0 = cfg.sar.f0
+    prf = cfg.sar.prf
+    num_ch = cfg.sar.num_ch
+    alt = cfg.sar.alt
+    v_ground = cfg.sar.v_ground
+    rg_bw = cfg.sar.rg_bw
+    over_fs = cfg.sar.over_fs
+
+    # CALCULATE PARAMETERS
+    l0 = const.c / f0
+    if v_ground == 'auto':
+        v_ground = geo.orbit_to_vel(alt, ground=True)
+    rg_sampling = rg_bw * over_fs
+
+    # RAW DATA
+    raw_file = tpio.RawFile(raw_output_file, 'r')
+    raw_data = raw_file.get('raw_data*')
+    sr0 = raw_file.get('sr0')
+    inc_angle = raw_file.get('inc_angle')
+    b_ati = raw_file.get('b_ati')
+    b_xti = raw_file.get('b_xti')
+    raw_file.close()
+
+    
+    # OTHER INITIALIZATIONS
+    # Create plots directory
+    plot_path = os.path.dirname(output_file) + os.sep + plot_path
+    if plot_save:
+        if not os.path.exists(plot_path):
+            os.makedirs(plot_path)
+
+    slc = []
+    BP = 1
+    ########################
+    # PROCESSING MAIN LOOP #
+    ########################
+    for ch in np.arange(num_ch):
+
+        if plot_raw:
+            plt.figure()
+            plt.imshow(np.real(raw_data[0, ch]),
+                       vmin=-np.max(np.abs(raw_data[0, ch])),
+                       vmax=np.max(np.abs(raw_data[0, ch])), cmap='gray')
+            plt.savefig(plot_path + os.sep + ('plot_raw_real_%d.%s' % (ch, plot_format)))
+            plt.close()
+            
+        if BP ==1:
+                    # Getting each channel data
+            az_size_orig, rg_size_orig = raw_data[0, 0].shape
+            backscatter = np.zeros((num_ch, az_size_orig, rg_size_orig)) 
+            az_size_orig, rg_size_orig = raw_data[0, ch].shape  # az 142 and rg 97
+            data = np.zeros((az_size_orig, rg_size_orig), dtype=complex)  #Initialization 2D, ( az, rg)
+            data = raw_data[0, ch, :, :]    
+            backscatter[ch, :, :] = back_projection(data, prf, f0, v_ground, sr0, rg_sampling)
+            
+            # Removal of non valid samples
+            n_val_az_2 = np.floor(
+            doppler_bw / 2. / (2. * v_ground**2. / l0 / sr0) * prf / 2.) * 2.
+            reduced = backscatter[ch, int(n_val_az_2):int(az_size_orig - n_val_az_2 - 1), :]
+            print(reduced.shape)
+        
+            idx_reduced_azi = np.sum(np.abs(reduced), axis=1)
+            intensity_BP = np.abs((reduced[np.argmax(idx_reduced_azi), :]))  #Sliced at Max Azimuth
+            plt.figure()
+            plt.imshow(np.abs(reduced), origin='lower', vmin=0, vmax=np.max(np.abs(reduced)),
+                       aspect=float(rg_size_orig) / float(az_size_orig),
+                       cmap='gray')
+            plt.xlabel("Range")
+            plt.title("Reduced BP")
+            plt.ylabel("Azimuth")
+            
+           
+           
+
+        # Optimize matrix sizes
+        az_size_orig, rg_size_orig = raw_data[0, ch].shape
+        optsize = utils.optimize_fftsize(raw_data[0, ch].shape)
+        optsize = [raw_data.shape[0], optsize[0], optsize[1]]
+        data = np.zeros(optsize, dtype=complex)
+        data[:, :raw_data[0, ch].shape[0],
+       :raw_data[0, ch].shape[1]] = raw_data[:, ch, :, :]
+        az_size, rg_size = data.shape[1:]
+   
+                         
+        # RCMC Correction
+        print('Applying RCMC correction... [Channel %d/%d]' % (ch + 1, num_ch))
+ 
+        fr = np.fft.fftfreq(rg_size, 1/rg_sampling)
+        fa = np.fft.fftfreq(az_size, 1/prf)
+        ## Compensation of ANTENNA PATTERN
+        ## FIXME this will not work for a long separation betwen Tx and Rx!!!
+        sin_az = fa * l0 / (2 * v_ground)
+        if hasattr(cfg.sar, 'ant_L'):
+            ant_L = cfg.sar.ant_L
+            if cfg.sar.L_total:
+                beam_pattern = sinc_1tx_nrx(sin_az, ant_L * num_ch, f0, num_ch, field=True)
+            else:
+                beam_pattern = sinc_1tx_nrx(sin_az, ant_L, f0, 1, field=True)
+        else:
+            ant_l_tx = cfg.sar.ant_L_tx
+            ant_l_rx = cfg.sar.ant_L_rx
+            beam_pattern = (sinc_bp(sin_az, ant_l_tx, f0, field=True)
+                            * sinc_bp(sin_az, ant_l_rx, f0, field=True))
+
+
+        #fa[az_size/2:] = fa[az_size/2:] - prf
+        rcmc_fa = sr0 / np.sqrt(1 - (fa * (l0 / 2.) / v_ground)**2.) - sr0
+        data = np.fft.fft(np.fft.fft(data, axis=-1), axis=-2)
+       
+#        for i in np.arange(az_size):
+#            data[i,:] *= np.exp(1j*2*np.pi*2*rcmc_fa[i]/const.c*fr)
+        data = (data * np.exp(4j * np.pi * rcmc_fa.reshape((1, az_size, 1)) /
+                              const.c * fr.reshape((1, 1, rg_size))))
+    
+        data = np.fft.ifft(data, axis=2)
+       
+        if plot_rcmc_dopp:
+            plt.figure()
+            plt.imshow(np.fft.fftshift(np.abs(data[0]), axes=0), vmax=np.max(np.abs(data)), cmap='gray',
+                       origin='lower')
+            plt.savefig(plot_path + os.sep + ('plot_rcmc_dopp_%d.%s' % (ch, plot_format)))
+            plt.close()
+
+        if plot_rcmc_time:
+            rcmc_time = np.fft.ifft(data[0], axis=0)[
+                :az_size_orig, :rg_size_orig]
+            rcmc_time_max = np.max(np.abs(rcmc_time))
+            plt.figure()
+            plt.imshow(np.real(rcmc_time), vmin=-rcmc_time_max, vmax=rcmc_time_max, cmap='gray',
+                       origin='lower')
+            plt.savefig(plot_path + os.sep + ('plot_rcmc_time_real_%d.%s' % (ch, plot_format)))
+            plt.close()
+
+        # Azimuth compression
+        print(
+            'Applying azimuth compression... [Channel %d/%d]' % (ch + 1, num_ch))
+
+        n_samp = 2 * (int(doppler_bw / (fa[1] - fa[0])) / 2)
+        weighting = (az_weighting -
+                     (1. - az_weighting) * np.cos(2 * np.pi * np.linspace(0, 1., int(n_samp))))
+        # Compensate amplitude loss
+
+        L_win = np.sum(np.abs(weighting)**2) / weighting.size
+        weighting /= np.sqrt(L_win)
+        if fa.size > n_samp:
+            zeros = np.zeros(az_size)
+            zeros[0:int(n_samp)] = weighting
+            weighting = np.roll(zeros, int(-n_samp / 2))
+        weighting = np.where(np.abs(beam_pattern) > 0, weighting/beam_pattern, 0)
+        ph_ac = 4. * np.pi / l0 * sr0 * \
+            (np.sqrt(1. - (fa * l0 / 2. / v_ground)**2.) - 1.)
+  
+        data = data * (np.exp(1j * ph_ac) * weighting).reshape((1, az_size, 1))
+  
+        #=====================================
+        data = np.fft.ifft(data, axis=1)
+        
+        print(data.shape)
+        
+        print('Finishing... [Channel %d/%d]' % (ch + 1, num_ch))
+
+
+        # Reduce to initial dimension
+        data = data[:, :int(az_size_orig), :int(rg_size_orig)]
+        print(data.shape)
+        # Removal of non valid samples
+        n_val_az_2 = np.floor(
+            doppler_bw / 2. / (2. * v_ground**2. / l0 / sr0) * prf / 2.) * 2.
+        # data = raw_data[ch, n_val_az_2:(az_size_orig - n_val_az_2 - 1), :]
+        data = data[:, int(n_val_az_2):int(az_size_orig - n_val_az_2 - 1), :]
+        
+        
+        print(ch)
+        print(data.shape)
+        if plot_image_valid:
+            plt.figure()
+            plt.imshow(np.abs(data[0]), origin='lower', vmin=0, vmax=np.max(np.abs(data)),
+                       aspect=float(rg_size_orig) / float(az_size_orig),
+                       cmap='gray')
+            plt.xlabel("Range")
+            plt.ylabel("Azimuth")
+            plt.savefig(os.path.join(
+            plot_path, ('plot_image_valid_%d.%s' % (ch, plot_format)))) 
+            
+            
+            
+            
+            
+        ##### INTENSITY PLOT at MAX Azimuth Position
+        range_resolution = const.c / (2 * rg_sampling)
+        azimuth_resolution = v_ground/prf
+        print (range_resolution)
+        print (azimuth_resolution)
+        
+        intensity_grid = np.abs(data[0]) #for frequency based
+        azimuth_intensity_sum = np.sum(intensity_grid, axis=1)
+        intensity_Freqbased = (intensity_grid[np.argmax(azimuth_intensity_sum), :])
+        
+        plt.figure(figsize=(10, 5))
+        plt.plot(np.abs(intensity_Freqbased), label='Frequency-Based Intensity')
+        plt.plot(np.abs(intensity_BP), label='Back-Projection Intensity')
+        plt.xlabel('Range Bin')
+        plt.ylabel('Magnitude')
+        plt.grid()
+        plt.legend()  # Place this before plt.show()
+        
+          
+
+        # IN dB and X axis in Meters
+        range_bins = np.arange(intensity_BP.size)
+        range_resolution = const.c / (2 * rg_sampling)
+        range_distances = range_bins * range_resolution
+        intensity_Freqbased_dB = 10 * np.log10(np.abs(intensity_Freqbased) + 1e-6)
+        intensity_BP_dB = 10 * np.log10(np.abs(intensity_BP) + 1e-6)
+                
+        plt.figure(figsize=(10, 6))
+        plt.plot(range_distances, intensity_Freqbased_dB, label="Freq. Based Algo.")
+        plt.plot(range_distances, intensity_BP_dB, label="BP Algo.")
+        plt.title("Intensity Across Range Distances at Maximum Intensity Azimuth Index")
+        plt.xlabel("Range Distance (meters)")
+        plt.ylabel("Intensity (dB)")
+        plt.legend()
+        plt.grid()
+        plt.show()
+        
+        ####
+      
+        
+        
+        slc.append(data)
+    
+    
+
+    # Save processed data
+    slc = np.array(slc, dtype=complex)
+    print("Shape of SLC: " + str(slc.shape), flush=True)
+   
+    proc_file = tpio.ProcFile(output_file, 'w', slc.shape)
+    proc_file.set('slc*', slc)
+    proc_file.set('inc_angle', inc_angle)
+    proc_file.set('f0', f0)
+    proc_file.set('num_ch', num_ch)
+    proc_file.set('ant_L', ant_l_tx)
+    proc_file.set('prf', prf)
+    proc_file.set('v_ground', v_ground)
+    proc_file.set('orbit_alt', alt)
+    proc_file.set('sr0', sr0)
+    proc_file.set('rg_sampling', rg_bw*over_fs)
+    proc_file.set('rg_bw', rg_bw)
+    proc_file.set('b_ati', b_ati)
+    proc_file.set('b_xti', b_xti)
+    proc_file.close()
+
+    print('-----------------------------------------')
+    print(time.strftime(
+        "Processing finished [%Y-%m-%d %H:%M:%S]", time.localtime()))
+    print('-----------------------------------------')
+
+
+if __name__ == '__main__':
+
+    # INPUT ARGUMENTS
+    parser = argparse.ArgumentParser()
+    parser.add_argument('-c', '--cfg_file')
+    parser.add_argument('-r', '--raw_file')
+    parser.add_argument('-o', '--output_file')
+    args = parser.parse_args()
+
+    sar_focus(args.cfg_file, args.raw_file, args.output_file)
diff --git a/oceansar/radarsim/back_projection_func.py b/oceansar/radarsim/back_projection_func.py
new file mode 100644
index 0000000..d01a29c
--- /dev/null
+++ b/oceansar/radarsim/back_projection_func.py
@@ -0,0 +1,63 @@
+import numpy as np
+import matplotlib.pyplot as plt
+from scipy import interpolate
+from scipy import stats
+
+def filter_on_peak(size, peak_index, alpha=4):
+    x = np.arange(size) - peak_index
+    sinc_filter = np.sinc(x / alpha)
+    return sinc_filter
+
+def back_projection(data, prf, f0, v_ground, sr0, rg_sampling):
+    c = 3e8
+    az_size, rg_size = data.shape
+    wavelength = c / f0
+    kr = 2 * np.pi / wavelength
+    epsilon = 1e-6
+
+    image_grid = np.zeros((az_size, rg_size), dtype=complex)  
+    peak_range_idx = np.bincount(np.argmax(np.abs(data), axis=1)).argmax() 
+    sinc_filter_window = filter_on_peak(rg_size, peak_range_idx)
+    print(peak_range_idx)
+    middle_azimuth_idx = (az_size // 2)+1 
+    ##### MAIN LOOP ####
+    for az_idx in range(az_size):
+        range_vector = data[az_idx, :] * sinc_filter_window
+        range_vector *= np.max(np.abs(data[az_idx, :])) / np.max(np.abs(range_vector)) #Amp. compensation
+        azimuth_time = az_idx / prf 
+
+        d_az = v_ground * azimuth_time #Azi displace.
+
+        for y in range(rg_size):
+            range_distance = sr0 + y * rg_sampling
+            slant_range = np.sqrt(d_az**2 + range_distance**2)
+            # Note: Since d_az is very small that makes range and slant range almost equal. 
+            # Increasing v_ground or azimuth_time will make impact, To verify i have added epsilon
+            #slant_range = np.sqrt(d_az**2 + range_distance**2) +epsilon
+            rg_bin_float = (slant_range - sr0) / rg_sampling
+            rg_bin = int(np.floor(rg_bin_float))
+            weight = rg_bin_float - rg_bin
+            if 0 <= rg_bin < rg_size - 1:
+                interpolated_value = (
+                    (1 - weight) * range_vector[rg_bin] + weight * range_vector[rg_bin + 1]
+                )
+                
+                phase_correction = np.exp(1j * kr * (slant_range - range_distance))
+                contribution = interpolated_value * phase_correction
+                """print("Contribution:", contribution)
+                print("Range Vector Value:", range_vector[rg_bin])
+                print("Difference (slant_range - range_distance):", slant_range - range_distance)
+                print("Phase of Contribution:", np.angle(contribution))
+                print("Phase of Range Vector Value:", np.angle(range_vector[rg_bin]))
+                print("Phase Difference:", np.angle(contribution) - np.angle(range_vector[rg_bin]))"""                
+                image_grid[middle_azimuth_idx, y] += contribution
+
+    """plt.plot(np.abs(data[:, peak_range_idx]))
+    plt.plot(np.abs(image_grid[middle_azimuth_idx, :])) 
+    plt.xlabel('Range Index')
+    plt.ylabel('Magnitude')
+    plt.title('Accumulated Magnitude at Middle Azimuth Row')
+    plt.grid(True)
+    plt.show()"""
+
+    return image_grid