INVERSION OF SYNTHETIC APERTUR,E R,ADAR (SAR) - MSpace ...
INVERSION OF SYNTHETIC APERTUR,E R,ADAR (SAR) - MSpace ...
INVERSION OF SYNTHETIC APERTUR,E R,ADAR (SAR) - MSpace ...
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4.3 Forward Formulation for <strong>SAR</strong> Configuration<br />
The plevious section clealtecl with horv the Born inversion can be appliecl<br />
to leflection seismology probler.r.rs. Iu the clerivation, the Boln (first) approximation<br />
used in Eq.(4.9) hacl trvo implicit assurnptions: (a) tlie inciclent<br />
rvavefield renains unafected, ancl (b) only the incidett rvavefield intelacts<br />
rvith the velocity perturbatiol,<br />
The fir'st condition is requirecl to folnulate the Boln invelsion because<br />
the incident wave is assurnecl to be governed by a Green's function for the<br />
constant refelence rneclium in Ec1.(4.10). Thus the transmission losses or<br />
refi'active efects on the incident \¡¿ave as it 1ti'opagates downwalcl ate not<br />
includec{.<br />
The seconcl assumption is in fact the main step of the Born (fit st) apploxirnation<br />
to ornit higher-older scattering caused by other than the incident<br />
'\¡r'ave.<br />
<strong>SAR</strong> specific features rnust be investigated to develop an invelsion method<br />
of <strong>SAR</strong> data using tire Born (first) approximation. Differences l¡etween <strong>SAR</strong><br />
configulation alcl leflection seismology a;:e summalizecl as follows:<br />
i) unlike in seismic applications, the refelence velocity is a constant, i.e.<br />
the velocity of light,<br />
2) the centel fi'equelcy of tlie ladal signal is rnuch higher than that of<br />
seismic g'aves,<br />
3) the soulce ancl receivel pails ale not ol tlie scatteling sulface, ancl<br />
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