“…Finally, the image on the roof-shaped stepped micromirror enters the rear imaging system through the beam splitter and is finally imaged on the detector. From this, we can obtain the polarization interference image array for the target object and the three-dimensional polarization interference intensity datasets I 0 (x,y,∆(m,n)), I 45 (x,y,∆(m,n)), I 90 (x,y,∆(m,n)) and I 135 (x,y,∆(m,n)) for the four polarization directions of the target by segmenting and registering the polarization interference image array [19,20]. ∆(m,n) is the optical path difference modulated by the phase modulation unit (m,n): ∆(m,n) = 2(Nn−m)d. Here, m and n are the position coordinates of the corresponding phase modulation unit, taking the center of the whole modulation unit as the zero point and increasing accordingly in the horizontal and vertical directions.…”