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diff --git a/noao/twodspec/apextract/doc/apflatten.hlp b/noao/twodspec/apextract/doc/apflatten.hlp new file mode 100644 index 00000000..f7e1b8c0 --- /dev/null +++ b/noao/twodspec/apextract/doc/apflatten.hlp @@ -0,0 +1,304 @@ +.help apflatten Sep96 noao.twodspec.apextract +.ih +NAME +apflatten -- Create flat fields for fiber or narrow aperture spectra +.ih +USAGE +apflatten input output +.ih +PARAMETERS +.ls input +List of input flat field observations. +.le +.ls output = "" +List of output flat field images. If no output name is given then the +input name is used as a root with the extension ".flat". +.le +.ls apertures = "" +Apertures to recenter, resize, trace, and flatten. This only applies +to apertures read from the input or reference database. Any new +apertures defined with the automatic finding algorithm or interactively +are always selected. The syntax is a list comma separated ranges +where a range can be a single aperture number, a hyphen separated +range of aperture numbers, or a range with a step specified by "x<step>"; +for example, "1,3-5,9-12x2". +.le +.ls references = "" +List of reference images to be used to define apertures for the input +images. When a reference image is given it supersedes apertures +previously defined for the input image. The list may be null, "", or +any number of images less than or equal to the list of input images. +There are three special words which may be used in place of an image +name. The word "last" refers to the last set of apertures written to +the database. The word "OLD" requires that an entry exist +and the word "NEW" requires that the entry not exist for each input image. +.le + +.ls interactive = yes +Run this task interactively? If the task is not run interactively then +all user queries are suppressed and interactive aperture editing and trace +fitting are disabled. +.le +.ls find = yes +Find the spectra and define apertures automatically? In order for +spectra to be found automatically there must be no apertures for the +input image or reference image defined in the database. +.le +.ls recenter = yes +Recenter the apertures? +.le +.ls resize = yes +Resize the apertures? +.le +.ls edit = yes +Edit the apertures? The \fIinteractive\fR parameter must also be yes. +.le +.ls trace = yes +Trace the apertures? +.le +.ls fittrace = yes +Interactively fit the traced positions by a function? The \fIinteractive\fR +parameter must also be yes. +.le +.ls flatten = yes +Remove the profile shape and flat field spectrum leaving only +sensitivity variations? +.le +.ls fitspec = yes +Fit normalization spectrum interactively? The \fIinteractive\fR +parameter must also be yes. +.le + +.ls line = INDEF, nsum = 1 +The dispersion line (line or column perpendicular to the dispersion +axis) and number of adjacent lines (half before and half after unless +at the end of the image) used in finding, recentering, resizing, +and editing operations. For tracing this is the starting line and +the same number of lines are summed at each tracing point. A line of +INDEF selects the middle of the image along the dispersion axis. +A positive nsum sums the lines and a negative value takes the median. +However, for tracing only sums are allowed and the absolute value +is used. +.le +.ls threshold = 10. +Division threshold. If a pixel in the two dimensional normalization spectrum +is less than this value then a flat field value of 1 is output. +.le + +The following parameters control the profile and spectrum fitting. +.ls pfit = "fit1d" (fit1d|fit2d) +Profile fitting algorithm to use with variance weighting or cleaning. +When determining a profile the two dimensional spectrum is divided by +an estimate of the one dimensional spectrum to form a normalized two +dimensional spectrum profile. This profile is then smoothed by fitting +one dimensional functions, "fit1d", along the lines or columns most closely +corresponding to the dispersion axis or a special two dimensional +function, "fit2d", described by Marsh (see \fBapprofile\fR). +.le +.ls clean = no +Detect and replace deviant pixels? +.le +.ls saturation = INDEF +Saturation or nonlinearity level. During variance weighted extractions +wavelength points having any pixels above this value are excluded from the +profile determination. +.le +.ls readnoise = 0. +Read out noise in photons. This parameter defines the minimum noise +sigma. It is defined in terms of photons (or electrons) and scales +to the data values through the gain parameter. A image header keyword +(case insensitive) may be specified to get the value from the image. +.le +.ls gain = 1 +Detector gain or conversion factor between photons/electrons and +data values. It is specified as the number of photons per data value. +A image header keyword (case insensitive) may be specified to get the value +from the image. +.le +.ls lsigma = 3., usigma = 3. +Lower and upper rejection thresholds, given as a number of times the +estimated sigma of a pixel, for cleaning. +.le + +The following parameters are used to fit the normalization spectrum using +the ICFIT routine. +.ls function = "legendre" +Fitting function for the normalization spectra. The choices are "legendre" +polynomial, "chebyshev" polynomial, linear spline ("spline1"), and +cubic spline ("spline3"). +.le +.ls order = 1 +Number of polynomial terms or number of spline pieces for the fitting function. +.le +.ls sample = "*" +Sample regions for fitting points. Intervals are separated by "," and an +interval may be one point or a range separated by ":". +.le +.ls naverage = 1 +Number of points within a sample interval to be subaveraged or submedianed to +form fitting points. Positive values are for averages and negative points +for medians. +.le +.ls niterate = 0 +Number of sigma clipping rejection iterations. +.le +.ls low_reject = 3. , high_reject = 3. +Lower and upper sigma clipping rejection threshold in units of sigma determined +from the RMS sigma of the data to the fit. +.le +.ls grow = 0. +Growing radius for rejected points (in pixels). That is, any rejected point +also rejects other points within this distance of the rejected point. +.le +.ih +ADDITIONAL PARAMETERS +I/O parameters and the default dispersion axis are taken from the +package parameters, the default aperture parameters from +\fBapdefault\fR, automatic aperture finding parameters from +\fBapfind\fR, recentering parameters from \fBaprecenter\fR, resizing +parameters from \fBapresize\fR, parameters used for centering and +editing the apertures from \fBapedit\fR, and tracing parameters from +\fBaptrace\fR. +.ih +DESCRIPTION +It is sometimes the case that it is undesirable to simply divide +two dimensional format spectra taken through fibers, aperture masks +with small apertures such as holes and slitlets, or small slits in +echelle formats by a flat field observation of a lamp. This is due +to the sharp dropoff of the flat field and object profiles and +absence of signal outside of the profile. Slight shifts or changes +in profile shape introduce bad edge effects, unsightly "grass" is +produced where there is no signal (which may also confuse extraction +programs), and the division will also remove the characteristic +profile of the object which might be needed for tracking the +statistical significance, variance weighted extraction, and more. +A straight flat field division also has the problem of changing the +shape of the spectrum in wavelength, again compromising the +poisson statistics and artificially boosting low signal regions. + +There are three approaches to consider. First, the +flat field correction can be done after extraction to one dimension. +This is valid provided the flat field and object profiles don't shift +much. However, for extractions that depend on a smooth profile, +such as the variance weighting algorithms of this package, the sensitivity +corrections must remain small; i.e. no large fringes or other +small scale variations that greatly perturb the true photon profile. +The second approach is to divide out the overall spectral shape of +the flat field spectrum, fill regions outside of the signal with +one and leave the profile shape intact. This will still cause profile +division problems described earlier but is mentioned here since it +implemented in a related task called \fBapnormalize\fR. The last +approach is to model both the profile and overall spectrum shape and +remove it from the flat field leaving only the sensitivity variations. +This is what the task \fBapflatten\fR does. + +The two dimensional flat field spectra within the defined apertures of +the input images are fit by a model having the profile of the data and +a smooth spectral shape. This model is then divided into the flat +field image within the aperture, replacing points of low signal, set +with the \fIthreshold\fR parameter, within the aperture and all points +outside the aperture by one to produce an output sensitivity variation +only flat field image. + +A two dimensional normalized profile is computed by dividing the data +within the aperture by the one dimensional spectrum and smoothing with +low order function fits parallel to the dispersion axis if the aperture +is well aligned with the axis or parallel to the traced aperture center +if the trace is tilted relative to the dispersion axis. The smooth +profile is then used to improve the spectrum estimate using variance +weighting and to eliminate deviant or cosmic ray pixels by sigma +tests. The profile algorithm is described in detail in +\fBapprofiles\fR and the variance weighted spectrum is described in +\fBapvariance\fR. + +The process of determining the profile and variance weighted spectrum, +and hence the two dimensional spectrum model, is identical to that used +for variance weighted extraction of the one dimensional spectra in the +tasks \fBapall\fR or \fBapsum\fR and in making a two dimensional +spectrum model in the task \fBapfit\fR. Most of the parameters in +this task are the same in those tasks and so further information about +them may be found in their descriptions. In fact, up to this point the +task is the same as \fBapfit\fR and, if the flat field were normalized +by this model it would produce the "ratio" output of that task. + +This task deviates from \fBapfit\fR in that the final variance weighted +one dimensional spectrum of the flat field is subjected to a smoothing +operation. This is done by fitting a function to the spectrum using +the \fBicfit\fR routine. This may be done interactively or +noninteractively depending on the \fBinteractive\fR parameter. The +default fitting parameters are part of this task. The goal of the +fitting is to follow the general spectral shape of the flat field light +(usually a lamp) but not the small bumps and wiggles which are the one +dimensional projection of sensitivity variations. When the fitted +function is multiplied into the normalize profile and then the two +dimensional model divided into the data the sensitivity variations not +part of the fitted spectrum are what is left in the final output flat +field. + +The remainder of this description covers the basic steps defining the +apertures to be used. These steps and parameter are much the same as +in any of the other \fBapextract\fR tasks. + +Aperture definitions may be inherited from those of other images by +specifying a reference image with the \fBreferences\fR parameter. +Images in the reference list are matched with those in the input list +in order. If the reference image list is shorter than the number of +input images, the last reference image is used for all remaining input +images. Thus, a single reference image may be given for all the input +images or different reference images may be given for each input +image. The special reference name "last" may be used to select the +last set apertures used in any of the \fBapextract\fR tasks. + +If an aperture reference image is not specified or no apertures are +found for the specified reference image, previously defined apertures +for the input image are sought in the aperture database. Note that +reference apertures supersede apertures for the input image. If no +apertures are defined they may be created automatically, the \fIfind\fR +option, or interactively in the aperture editor, if the +\fIinteractive\fR and \fIedit\fR options are set. + +The functions performed by the task are selected by a set of flag +parameters. The functions are an automatic spectrum finding and +aperture defining algorithm (see \fBapfind\fR) which is ignored if +apertures are already defined, automatic recentering and resizing +algorithms (see \fBaprecenter\fR and \fBapresize\fR), an interactive +aperture editing function (see \fBapedit\fR), a spectrum position tracing +and trace function fit (see \fBaptrace\fR), and the main function of +this task, the flat field profile and spectral shape modeling and removal. + +Each function selection will produce a query for each input spectrum if +the \fIinteractive\fR parameter is set. The queries are answered by +"yes", "no", "YES", or "NO", where the upper case responses suppress +the query for following images. There are other queries associated +with tracing which first ask whether the operation is to be done +interactively and, if yes, lead to queries for each aperture. If the +\fIinteractive\fR parameter is not set then aperture editing +interactive trace fitting, and interactive spectrum shape fitting are ignored. +.ih +REVISIONS +.ls APFLATTEN V2.11 +The "apertures" parameter can be used to select apertures for resizing, +recentering, tracing, and extraction. This parameter name was previously +used for selecting apertures in the recentering algorithm. The new +parameter name for this is now "aprecenter". +.le +.ih +EXAMPLES +1. To make a two dimensional flat field from a lamp observation: + +.nf + cl> apflatten fiber1 flat read=3 gain=1 back=fit + Yes find + No resize + No edit + Yes trace + Yes trace interactively + NO + Yes flatten + Yes fit interactively +.fi +.ih +SEE ALSO +apbackground, approfile, apvariance, apfit, icfit, +apdefault, apfind, aprecenter, apresize, apedit, aptrace, apsum +.endhelp |