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are masked out. Parameters for this option can be set in theconfiguration file. The connected component file is composedof unsigned characters, with all pixels of the same valuebelonging to the same connected component and zerocorresponding to masked pixels.</td></table><p><table width="100%" border=0 rules="none" frame="void" cols="2" cellspacing="0" cellpadding="0"><tr valign="top" align="left"><td width="10%"></td><td width="90%"><b>-G</b> <i>maskfile</i></td></table><p><table width="100%" border=0 rules="none" frame="void" cols="2" cellspacing="0" cellpadding="0"><tr valign="top" align="left"><td width="21%"></td><td width="79%">Grow a connected component mask (see the <b>-g</b> option)for the input data array, assuming that it is alreadyunwrapped, and write the mask to the file <i>maskfile</i>.Statistical cost functions are computed for forming themask, but a new unwrapped solution is notcomputed.</td></table><p><table width="100%" border=0 rules="none" frame="void" cols="2" cellspacing="0" cellpadding="0"><tr valign="top" align="left"><td width="10%"></td><td width="90%"><b>-h</b></td></table><p><table width="100%" border=0 rules="none" frame="void" cols="2" cellspacing="0" cellpadding="0"><tr valign="top" align="left"><td width="21%"></td><td width="79%">Print a help message summarizing command-line options andexit.</td></table><p><table width="100%" border=0 rules="none" frame="void" cols="2" cellspacing="0" cellpadding="0"><tr valign="top" align="left"><td width="10%"></td><td width="90%"><b>-i</b></td></table><p><table width="100%" border=0 rules="none" frame="void" cols="2" cellspacing="0" cellpadding="0"><tr valign="top" align="left"><td width="21%"></td><td width="79%">Run in initialize-only mode. Normally, <b>snaphu</b> useseither an approximate minimum spanning tree (MST) algorithmor a minimum cost flow (MCF) algorithm for generating theinitialization to its iterative, modified network-simplexsolver. If <b>-i</b> is given, the initialization is writtento the output and the program exits without running theiterative solver.</td></table><p><table width="100%" border=0 rules="none" frame="void" cols="2" cellspacing="0" cellpadding="0"><tr valign="top" align="left"><td width="10%"></td><td width="90%"><b>-l</b> <i>logfile</i></td></table><p><table width="100%" border=0 rules="none" frame="void" cols="2" cellspacing="0" cellpadding="0"><tr valign="top" align="left"><td width="21%"></td><td width="79%">Log all runtime parameters and some other environmentinformation into the specified file. The log file is a textfile in the same format as a configurationfile.</td></table><p><table width="100%" border=0 rules="none" frame="void" cols="2" cellspacing="0" cellpadding="0"><tr valign="top" align="left"><td width="10%"></td><td width="90%"><b>-m</b> <i>magfile</i></td></table><p><table width="100%" border=0 rules="none" frame="void" cols="2" cellspacing="0" cellpadding="0"><tr valign="top" align="left"><td width="21%"></td><td width="79%">Read interferogram magnitude data from the specified file.This option is useful mainly if the wrapped-phase input fileis given as a set of real phase values rather than complexinterferogram values. The interferogram magnitude is used toform a coherence estimate if appropriate amplitude data aregiven as well. The default file format is FLOAT_DATA. If theformats ALT_LINE_DATA or ALT_SAMPLE_DATA are used, themagnitude should be in the first data channel of the file;the second channel is ignored. If the COMPLEX_DATA format isused, the phase information is ignored.</td></table><p><table width="100%" border=0 rules="none" frame="void" cols="2" cellspacing="0" cellpadding="0"><tr valign="top" align="left"><td width="10%"></td><td width="90%"><b>-n</b></td></table><p><table width="100%" border=0 rules="none" frame="void" cols="2" cellspacing="0" cellpadding="0"><tr valign="top" align="left"><td width="21%"></td><td width="79%">Run in no-statistical-costs mode. If the <b>-i</b> or<b>-p</b> options are given, <b>snaphu</b> will not usestatistical costs. Information from a weight file (<b>-w</b>option) will still be used if given.</td></table><p><table width="100%" border=0 rules="none" frame="void" cols="2" cellspacing="0" cellpadding="0"><tr valign="top" align="left"><td width="10%"></td><td width="90%"><b>-o</b> <i>outfile</i></td></table><p><table width="100%" border=0 rules="none" frame="void" cols="2" cellspacing="0" cellpadding="0"><tr valign="top" align="left"><td width="21%"></td><td width="79%">Write the unwrapped output to file called <i>outfile</i>. Ifthe file formats ALT_LINE_DATA (default) or ALT_SAMPLE_DATAare used, the unwrapped phase is written into the seconddata channel, while the interferogram magnitude is writteninto the first channel. The format FLOAT_DATA may also beused.</td></table><p><table width="100%" border=0 rules="none" frame="void" cols="2" cellspacing="0" cellpadding="0"><tr valign="top" align="left"><td width="10%"></td><td width="90%"><b>-p</b> <i>value</i></td></table><p><table width="100%" border=0 rules="none" frame="void" cols="2" cellspacing="0" cellpadding="0"><tr valign="top" align="left"><td width="21%"></td><td width="79%">Run in Lp-norm mode with p=<i>value</i>, where <i>value</i>is a nonnegative decimal. Instead of statistical costfunctions, the program uses Lp cost functions withstatistically based weights (unless <b>-n</b> is alsogiven). Solutions are still always congruent. Moreover,congruence is enforced within the solver routine, not as apost-optimization processing step. Therefore, if p=2, forexample, least-squares cost functions are used, but thesolution will probably be more accurate than one generatedfrom a transform-based least-squares algorithm.</td></table><p><table width="100%" border=0 rules="none" frame="void" cols="2" cellspacing="0" cellpadding="0"><tr valign="top" align="left"><td width="10%"></td><td width="90%"><b>-q</b></td></table><p><table width="100%" border=0 rules="none" frame="void" cols="2" cellspacing="0" cellpadding="0"><tr valign="top" align="left"><td width="21%"></td><td width="79%">Run in quantify-only mode. The input data are assumed to beunwrapped already, and the total cost of this solution iscalculated and printed. The unwrapped phase is wrappedassuming congruence for the cost calculation. Round-offerrors may limit the precision of the quantified cost. Seethe <b>-u</b> option for allowable fileformats.</td></table><p><table width="100%" border=0 rules="none" frame="void" cols="2" cellspacing="0" cellpadding="0"><tr valign="top" align="left"><td width="10%"></td><td width="90%"><b>-s</b></td></table><p><table width="100%" border=0 rules="none" frame="void" cols="2" cellspacing="0" cellpadding="0"><tr valign="top" align="left"><td width="21%"></td><td width="79%">Run in smooth-solution mode. The problem statistics andresulting cost functions are based on the assumption thatthe true unwrapped phase represents a generic surface withno discontinuities. This is the same as deformation modewith the DEFOMAX parameter set to zero.</td></table><p><table width="100%" border=0 rules="none" frame="void" cols="2" cellspacing="0" cellpadding="0"><tr valign="top" align="left"><td width="10%"></td><td width="90%"><b>-t</b></td></table><p><table width="100%" border=0 rules="none" frame="void" cols="2" cellspacing="0" cellpadding="0"><tr valign="top" align="left"><td width="21%"></td><td width="79%">Run in topography mode. The problem statistics and resultingcost functions are based on the assumption that the trueunwrapped phase represents surface elevation. This is thedefault.</td></table><p><table width="100%" border=0 rules="none" frame="void" cols="2" cellspacing="0" cellpadding="0"><tr valign="top" align="left"><td width="10%"></td><td width="90%"><b>-u</b></td></table><p><table width="100%" border=0 rules="none" frame="void" cols="2" cellspacing="0" cellpadding="0"><tr valign="top" align="left"><td width="21%"></td><td width="79%">Assume that the input file is unwrapped rather than wrapped.The algorithm makes iterative improvements to this solutioninstead of using an initialization routine. The input filemay be in the formats ALT_LINE_DATA (default) orALT_SAMPLE_DATA; the interferogram magnitude should be inthe first data channel and the unwrapped phase should be inthe second data channel. The format FLOAT_DATA may also beused.</td></table><p><table width="100%" border=0 rules="none" frame="void" cols="2" cellspacing="0" cellpadding="0"><tr valign="top" align="left"><td width="10%"></td><td width="90%"><b>-v</b></td></table><p><table width="100%" border=0 rules="none" frame="void" cols="2" cellspacing="0" cellpadding="0"><tr valign="top" align="left"><td width="21%"></td><td width="79%">Run in verbose mode. Extra information on the algorithm'sprogress is printed to the standard output.</td></table><p><table width="100%" border=0 rules="none" frame="void" cols="2" cellspacing="0" cellpadding="0"><tr valign="top" align="left"><td width="10%"></td><td width="90%"><b>-w</b> <i>weightfile</i></td></table><p><table width="100%" border=0 rules="none" frame="void" cols="2" cellspacing="0" cellpadding="0"><tr valign="top" align="left"><td width="21%"></td><td width="79%">Read external, scalar weights from file <i>weightfile</i>.The weights, which should be positive short integers, areapplied to whichever cost functions are used. There is oneweight value for each arc in the network, so<i>weightfile</i> should be the concatenation of rasterhorizontal-flow and vertical-flow arc weights. Thus, for anN row by M column interferogram, <i>weightfile</i> wouldconsist of a rasterized (N-1) by M array followed by arasterized N by (M-1) array of short integer data. Thisoption is not well tested.</td></table><p><table width="100%" border=0 rules="none" frame="void" cols="2" cellspacing="0" cellpadding="0"><tr valign="top" align="left"><td width="10%"></td><td width="90%"><b>--aa</b> <i>ampfile1 ampfile2</i></td></table><p><table width="100%" border=0 rules="none" frame="void" cols="2" cellspacing="0" cellpadding="0"><tr valign="top" align="left"><td width="21%"></td><td width="79%">Amplitude data are read from the files specified. The datafrom the two individual SAR images forming the interferogramare assumed to be separately stored in files <i>ampfile1</i>and <i>ampfile2</i>. These files should be in the formatFLOAT_DATA. This option is similar to the <b>-a</b>option.</td></table><p><table width="100%" border=0 rules="none" frame="void" cols="2" cellspacing="0" cellpadding="0"><tr valign="top" align="left"><td width="10%"></td><td width="90%"><b>--AA</b> <i>pwrfile1 pwrfile2</i></td></table><p><table width="100%" border=0 rules="none" frame="void" cols="2" cellspacing="0" cellpadding="0"><tr valign="top" align="left"><td width="21%"></td><td width="79%">Similar to the <b>--aa</b> option, but power data are readfrom the specified files.</td></table><p><table width="100%" border=0 rules="none" frame="void" cols="2" cellspacing="0" cellpadding="0"><tr valign="top" align="left"><td width="10%"></td><td width="90%"><b>--assemble</b> <i>dirname</i></td></table><p><table width="100%" border=0 rules="none" frame="void"
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