source: branches/pixel-map-branch/docs/intro.tex @ 1441

Last change on this file since 1441 was 255, checked in by Matthew Whiting, 17 years ago
  • Mostly Guide changes, thanks to the xspace package. Some alteration of the statistics calculation description, thanks to the new statsec parameter.
  • Also changed the default value of the reconDim parameter -- now default is 1-dimensional.
File size: 10.1 KB
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1\secA{Introduction and getting going quickly}
2
3This document provides a user's guide to \duchamp, an object-finder
4for use on spectral-line data cubes. The basic execution of \duchamp
5is to read in a FITS data cube, find sources in the cube, and produce
6a text file of positions, velocities and fluxes of the detections, as
7well as a postscript file of the spectra of each detection.
8
9\secB{What to do}
10
11So, you have a FITS cube, and you want to find the sources in it. What
12do you do? First, you need to get \duchamp: there are instructions in
13Appendix~\ref{app-install} for obtaining and installing it. Once you
14have it running, the first step is to make an input file that contains
15the list of parameters. Brief and detailed examples are shown in
16Appendix~\ref{app-input}. This file provides the input file name, the
17various output files, and defines various parameters that control the
18execution.
19
20The standard way to run \duchamp is by the command
21\begin{quote}
22\texttt{Duchamp -p [parameter file]}
23\end{quote}
24replacing \texttt{[parameter file]} with the name of the file listing
25the parameters.
26
27An even easier way is to use the default values for all parameters
28(these are given in Appendix~\ref{app-param} and in the file
29\texttt{InputComplete} included in the distribution directory) and use
30the syntax
31\begin{quote}
32\texttt{Duchamp -f [FITS file]}
33\end{quote}
34where \texttt{[FITS file]} is the file you wish to search.
35
36In either case, the program will then work away and give you the list
37of detections and their spectra. The program execution is summarised
38below, and detailed in \S\ref{sec-flow}. Information on inputs is in
39\S\ref{sec-param} and Appendix~\ref{app-param}, and descriptions of
40the output is in \S\ref{sec-output}.
41
42\secB{Guide to terminology and conventions}
43
44First, a brief note on the use of terminology in this guide. \duchamp
45is designed to work on FITS ``cubes''. These are FITS\footnote{FITS is
46the Flexible Image Transport System -- see \citet{hanisch01} or
47websites such as
48\href{http://fits.cv.nrao.edu/FITS.html}{http://fits.cv.nrao.edu/FITS.html}
49for details.} image arrays with (at least) three dimensions. They
50are assumed to have the following form: the first two dimensions
51(referred to as $x$ and $y$) are spatial directions (that is, relating
52to the position on the sky -- often, but not necessarily,
53corresponding to Equatorial or Galactic coordinates), while the third
54dimension, $z$, is the spectral direction, which can correspond to
55frequency, wavelength, or velocity. The three dimensional analogue of
56pixels are ``voxels'', or volume cells -- a voxel is defined by a
57unique $(x,y,z)$ location and has a unique value of flux, intensity
58or brightness (or something equivalent) associated with it.
59
60Note that it is possible for the FITS file to have more than three
61dimensions (for instance, there could be a fourth dimension
62representing a Stokes parameter). Only the two spatial dimensions and
63the spectral dimension are read into the array of pixel values that is
64searched for objects. All other dimensions are ignored\footnote{This
65actually means that the first pixel only of that axis is used, and the
66array is read by the \texttt{fits\_read\_subsetnull} command from the
67\textsc{cfitsio} library.}. Herein, we discuss the data in terms of
68the three basic dimensions, but you should be aware it is possible for
69the FITS file to have more than three. Note that the order of the
70dimensions in the FITS file does not matter.
71
72With this setup, each spatial pixel (a given $(x,y)$ coordinate) can
73be said to be a single spectrum, while a slice through the cube
74perpendicular to the spectral direction at a given $z$-value is a
75single channel (the 2-D image is a channel map).
76
77Detection involves locating a contiguous group of voxels with fluxes
78above a certain threshold. \duchamp makes no assumptions as to the
79size or shape of the detected features, other than having
80user-selected minimum size criteria. Features that are detected are
81assumed to be positive. The user can choose to search for negative
82features by setting an input parameter -- this inverts the cube prior
83to the search (see \S\ref{sec-detection} for details).
84
85Finally, note that it is possible to run \duchamp on a
86two-dimensional image (\ie one with no frequency or velocity
87information), or indeed a one-dimensional array, and many of the
88features of the program will work fine. The focus, however, is on
89object detection in three dimensions, one of which is a spectral
90dimension.
91
92\secB{A summary of the execution steps}
93
94The basic flow of the program is summarised here -- all steps are
95discussed in more detail in the following sections.
96\begin{enumerate}
97\item The necessary parameters are recorded.
98
99  How this is done depends on the way the program is run from the
100  command line. If the \texttt{-p} option is used, the parameter file
101  given on the command line is read in, and the parameters therein are
102  read. All other parameters are given their default values (listed in
103  Appendix~\ref{app-param}).
104
105  If the \texttt{-f} option is used, all parameters are assigned their
106  default values.
107
108\item The FITS image is located and read in to memory.
109
110  The file given is assumed to be a valid FITS file. As discussed
111  above, it can have any number of dimensions, but \duchamp only
112  reads in the two spatial and the one spectral dimensions. A subset
113  of the FITS array can be given (see \S\ref{sec-input} for details).
114
115\item If requested, a FITS file containing a previously reconstructed
116  or smoothed array is read in.
117
118  When a cube is either Hanning-smoothed or reconstructed with the
119  \atrous wavelet method, the result can be saved to a FITS file, so
120  that subsequent runs of \duchamp can read it in to save having to
121  re-do the reconstruction (as it can be relatively time-intensive).
122
123\item \label{step-blank} If requested, BLANK pixels are trimmed from
124  the edges, and the baseline of each spectrum is removed.
125
126  When BLANK pixels are present, they can adversely affect the
127  reconstruction algorithms, as well as increasing the size in memory
128  of the array. This step trims them from the spatial edges, recording
129  the amount trimmed so that they can be added back in later.
130
131  A spectral baseline can be removed at this point as well. This may
132  be necessary if there is a ripple or other large-scale feature
133  present that will hinder detection of faint sources.
134
135\item If the reconstruction method is requested, and the reconstructed
136  array has not been read in at Step 3 above, the cube is
137  reconstructed using the \atrous wavelet method.
138
139  This step uses the \atrous method to determine the amount of
140  structure present at various scales. A simple thresholding technique
141  then removes random noise from the cube, leaving the significant
142  signal. This process can greatly reduce the noise level in the cube,
143  enhancing the detectability of sources.
144
145\item Alternatively (and if requested), the each spectral channel is
146  Hanning-smoothed by a desired amount.
147
148  This step considers each spectrum individually, and convolves it
149  with a Hanning filter (with width chosen by the user). This can help
150  to reduce the amount of noise visible in the cube.
151
152\item A threshold for the cube is then calculated, based on the pixel
153  statistics (unless a threshold is manually specified by the user).
154
155  The threshold can either be chosen as a simple $n\sigma$ threshold
156  (\ie so many standard deviations above the mean), or calculated via
157  the ``False Discovery Rate'' method. Alternatively, the threshold
158  can be specified as a simple flux value, without care as to the
159  statistical significance (\eg ``I want every source brighter than
160  10mJy'').
161
162\item Searching for objects then takes place, using the requested
163  thresholding method.
164
165  The cube is searched in the following manner: each 1-D spectrum is
166  searched, followed by each 2-D image. Any objects detected in each
167  search are added to a master list, or combined with objects already
168  in that list.
169
170\item The list of objects is condensed by merging neighbouring objects
171  and removing those deemed unacceptable.
172
173  There are certain criteria the user can specify that objects must
174  meet: minimum numbers of spatial pixels and spectral channels, and
175  minimum separations between neighbouring objects. Those that do not
176  meet these criteria are either deleted from the list, or merged with
177  their nearby neighbours.
178
179\item The baselines and trimmed pixels are replaced prior to output.
180
181  This is just the inverse of step~\#\ref{step-blank}.
182
183\item The details of the detections are written to screen and to the
184  requested output file.
185
186  Crucial properties of each detection are provided, showing its
187  location, extent, and flux. These are presented in both pixel
188  coordinates and world coordinates (\eg sky position and
189  velocity). Any warning flags are also printed, showing detections to
190  be wary of.
191
192\item Maps showing the spatial location of the detections are written.
193
194  These are 2-dimensional maps, showing where each detection lies on
195  the spatial coverage of the cube. This is provided as an aid to the
196  user so that a quick idea of the distribution of object positions
197  can be gained \eg are all the detections on the edge?
198
199  Two maps are provided: one is a 0th moment map, showing the 0th
200  moment of each detection in its appropriate position, while the
201  second is a ``detection map'', showing the number of times each
202  spatial pixel was detected in the searching routines.
203
204  These maps are written to postscript files, and the 0th moment map
205  can also be displayed in a PGPLOT X-window.
206
207\item The integrated or peak spectra of each detection are written to a
208  postscript file.
209
210  The spectral equivalent of the maps -- what is the spectral profile
211  of each detection? Also provided here are basic information for each
212  object (a summary of the information in the results file), as well
213  as a 0th moment map of the detection.
214
215\item If requested, the reconstructed or smoothed array can be written
216  to a new FITS file.
217
218  If either of these procedures were done, the resulting array can be
219  saved as a FITS file for later use. The FITS header will be the same
220  as the input file, with a few additional keywords to identify the
221  file.
222
223\end{enumerate}
224
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