Phase to Displacement

Phase to Displacement Operator

In case that some of the point scatterers on the ground slightly change their relative position in the time interval between two SAR observations (as, for example, in the event of subsidence, landslide, earthquake, etc.), then the following additive phase term, independent of the baseline, appears in the interferometric phase:

where λ is the transmitted wavelength and d is the relative scatterer displacement projected on the slant range direction. The interferometric phase variation can be split into three contributions:
  1. A phase variation proportional to the relative terrain altitude, referred to a horizontal reference plane;
  2. A phase variation proportional to the slant range difference of the point targets; and
  3. A phase variation proportional to the relative scatterer displacement.
If a digital elevation model (DEM) is available, the first phase term (i.e. the altitude contribution) can be subtracted from the interferometric phase. This operation is known as topographic phase removal.
If precise orbital data is available, the second phase term can also be computed and subtracted from the interferometric phase. This operation is called interferogram flattening or flat-Earth phase removal.
As a result of the above two operations, it generates a phase map proportional only to the relative terrain displacement which can be computed by


This operator converts interferometric phase to displacement map.

Input and Output


Reference: 

[1] Ferretti A., Massonet D., Monti Guarnieri A., Prati C., Rocca F., 2007, InSAR Principles: Guidelines for SAR Interferometry Processing and Interpretation, ESA TM-19