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authorThomas White <taw@physics.org>2013-02-08 12:35:30 -0800
committerThomas White <taw@physics.org>2013-02-08 12:35:30 -0800
commitdac436f21df140b6bf0796f6f9cbb6fcb6c03e2d (patch)
treecdbe1bfb5038be2d58ea3fc359311c5f8ab1b372 /doc/man/indexamajig.1
parentdf22900f8dba733e8c563704f2686f0e315655f4 (diff)
Update docs, comments etc
Diffstat (limited to 'doc/man/indexamajig.1')
-rw-r--r--doc/man/indexamajig.1101
1 files changed, 25 insertions, 76 deletions
diff --git a/doc/man/indexamajig.1 b/doc/man/indexamajig.1
index 9933627c..7f44605f 100644
--- a/doc/man/indexamajig.1
+++ b/doc/man/indexamajig.1
@@ -1,7 +1,8 @@
.\"
.\" indexamajig man page
.\"
-.\" Copyright © 2012 Thomas White <taw@physics.org>
+.\" Copyright © 2012-2013 Deutsches Elektronen-Synchrotron DESY,
+ * a research centre of the Helmholtz Association.
.\"
.\" Part of CrystFEL - crystallography with a FEL
.\"
@@ -12,25 +13,23 @@ indexamajig \- bulk indexing and data reduction program
.SH SYNOPSIS
.PP
.BR indexamajig
-\fB-i\fR \fIfilename\fR \fB-o\fR \fIoutput.stream\fR \fB-g\fR \fIdetector.geom\fR \fB-b\fR \fIbeamline.beam\fR \fB--peaks=\fR\fImethod\fR \fB--indexing=\fR\fImethod\fR \fB--cell-reduction=\fR\fImethod\fR
+\fB-i\fR \fIfilename\fR \fB-o\fR \fIoutput.stream\fR \fB-g\fR \fIdetector.geom\fR \fB-b\fR \fIbeamline.beam\fR \fB--peaks=\fR\fImethod\fR \fB--indexing=\fR\fImethod\fR
[\fBoptions\fR] \fB...\fR
.PP
\fBindexamajig --help\fR
.SH DESCRIPTION
-indexamajig takes as input a list of diffraction image files, currently in HDF5 format. For each image, it attempts to find peaks and then index the pattern. If successful, it will measure the intensities of the peaks at Bragg locations and produce a list of integrated peaks and intensities (and so on) in an output text file known as a "stream".
+\fBindexamajig\fR takes a list of diffraction snapshots from crystals in random orientations and attempts to find peaks, index and integrate each one. The input is a list of diffraction image files in HDF5 format and some auxiliary files and parameters. The output is a long text file ('stream') containing the results from each image in turn.
-For minimal basic use, you need to provide the list of diffraction patterns, the method which will be used to index, a file describing the geometry of the detector, a PDB file which contains the unit cell which will be used for the indexing, and that you'd like the program to output a list of intensities for each successfully indexed pattern. Here is what the minimal use might look like on the command line:
+For minimal basic use, you need to provide the list of diffraction patterns, the method which will be used to index, a file describing the geometry of the detector, and a PDB file which contains the unit cell which will be used for the indexing. Here is what the minimal use might look like on the command line:
.IP \fBindexamajig\fR
.PD
--i mypatterns.lst -j 10 -g mygeometry.geom --indexing=mosflm,dirax --peaks=hdf5 --cell-reduction=reduce -b myxfel.beam -o test.stream -p mycell.pdb --record=integrated
+-i mypatterns.lst -j 10 -g mygeometry.geom --indexing=mosflm,dirax --peaks=hdf5 -b myxfel.beam -o test.stream -p mycell.pdb
.PP
-More typical use includes all the above, but might also include a noise or
-common mode filter (--filter-noise or --filter-cm respectively) if detector
-noise causes problems for the peak detection. The HDF5 files might be in some
+More typical use includes all the above, but might also include extra parameters to modify the behaviour. The HDF5 files might be in some
folder a long way from the current directory, so you might want to specify a
full pathname to be added in front of each filename. You'll probably want to
run more than one indexing job at a time (-j <n>).
@@ -43,33 +42,7 @@ array, where the first two columns contain fast scan and slow scan coordinates
at the given location. The value will be spread in a small cross centred on
that location.
-See \fBman crystfel_geometry\fR for information about how to create a geometry description file.
-
-You can control what information is included in the output stream using
-\fB--record\fR=\fIflags\fR. Possible flags are:
-
-.IP \fBintegrated\fR
-.PD
-Include a list of reflection intensities, produced by integrating around predicted peak locations.
-
-.IP \fBpeaks\fR
-.PD
-Include peak locations and intensities from the peak search.
-
-.IP \fBpeaksifindexed\fR
-.PD
-As 'peaks', but the peak information will be written only if the pattern could be indexed.
-
-.IP \fBpeaksifnotindexed\fR
-.PD
-As 'peaks', but the peak information will be written only if the pattern could \fInot\fR be indexed.
-
-.PP
-The default is \fB--record=integrated\fR.
-
-.PP
-If you just want the integrated intensities of indexed peaks, use \fB--record=integrated\fR. If you just want to check that the peak detection is working, used \fB--record=peaks\fR. If you want the integrated peaks for the indexable patterns, but also want to check the peak detection for the patterns
-which could not be indexed, you might use \fB--record=integrated,peaksifnotindexed\fR and then use \fBcheck-peak-detection\fR from the scripts folder to visualise the results of the peak detection.
+See \fBman crystfel_geometry\fR for information about how to create a geometry description file and a beam parameters file.
.SH PEAK DETECTION
@@ -77,63 +50,49 @@ You can control the peak detection on the command line. Firstly, you can choose
If you use \fB--peaks=zaef\fR, indexamajig will use a simple gradient search after Zaefferer (2000). You can control the overall threshold and minimum gradient for finding a peak using \fB--threshold\fR and \fB--min-gradient\fR. Both of these have arbitrary units matching the pixel values in the data.
-A minimum peak separation can also be provided in the geometry description file
-(see \fBman crystfel_geometry\fR for details). This number serves two purposes. Firstly, it is the maximum distance allowed between the peak summit and the foot point (where the gradient exceeds the minimum gradient). Secondly, it is the minimum distance allowed between one peak and another, before the later peak will be rejected.
+Peaks will be rejected if the 'foot point' is further away from the 'summit' of the peak by more than the inner integration radius (see below). They will also be rejected if the peak is closer than twice the inner integration radius from another peak.
You can suppress peak detection altogether for a panel in the geometry file by specifying the "no_index" value for the panel as non-zero.
.SH INDEXING METHODS
-You can choose between a variety of indexing methods. You can choose more than one method, in which case each method will be tried in turn until the later cell reduction step says that the cell is a "hit". Choose from:
-
-.IP \fBnone\fR
-.PD
-No indexing, peak detection only.
+You can choose between a variety of indexing methods. You can choose more than one method, in which case each method will be tried in turn until one of them reports that the pattern has been successfully indexed. Choose from:
.IP \fBdirax\fR
.PD
-DirAx will be executed. DirAx must be installed and in your PATH for this to work. Test by running \fBdirax\fR on the command line immediately before running \fBindexamajig\fR - you should see a welcome message. If not, refer to the installation instructions for DirAx.
+ Invoke DirAx, check linear combinations of the resulting cell axes for agreement with your cell, and then check that the cell accounts for at least half of the peaks from the peak search.
.IP \fBmosflm\fR
.PD
-MOSFLM will be executed. MOSFLM must be installed and in your PATH for this to work. Test by running \fBipmosflm\fR on the command line immediately before running \fBindexamajig\fR - you should see a welcome message. If not, refer to the installation instructions for CCP4.
+As \fBdirax\fR, but invoke MOSFLM instead. If you provide a PDB file (with \fB-p\fR), the lattice type and centering information will be passed to MOSFLM, which will then return solutions which match. Note that the lattice parameter information will \fBnot\fR be given to MOSFLM.
.IP \fBreax\fR
.PD
-An \fIexperimental\fR DPS-style algorithm will be used, which searches for a lattice with cell parameters close to those contained in the CRYST1 line of the PDB file given with \fB-p\fR or \fB--pdb\fR. If you use this option, you should also use \fB--cell-reduction=none\fR.
+Run the DPS algorithm, looking for the axes of your cell.
.PP
-The default is \fB--indexing=none\fR.
-
-
-.SH CELL REDUCTION
-Neither MOSFLM nor DirAx are currently able to simply search for the orientation of a known unit cell. Instead, they determine the unit cell parameters ab initio. To check if the parameters match the known unit cell, which you provide with \fB-p\fR \fIunitcell.pdb\fR or \fB--pdb=\fR\fIunitcell.pdb\fR. There is a choice of ways in which this comparison can be performed, which you can choose between using \fB--cell-reduction=\fR\fImethod\fR. The choices for \fImethod\fR are:
+You can add the following to the above indexing methods:
-.IP \fBnone\fR
+.IP \fB-raw\fR
.PD
-The raw cell from the autoindexer will be used. The cell probably won't match the target cell, but it'll still get used. Use this option to test whether the patterns are basically "indexable" or not, or if you don't know the cell parameters. In the latter case, you'll need to plot a histogram of the resulting parameters from the output stream to see which are the most popular.
+Do not check the resulting unit cell. This option is useful when you need to determine the unit cell ab initio. Use with 'dirax' and 'mosflm' - the other indexing methods need the unit cell as input in any case, and cannot determine the unit cell ab initio.
-.IP \fBreduce\fR
+.IP \fB-axes\fR
.PD
-Linear combinations of the raw cell will be checked against the target cell. If at least one candidate is found for each axis of the target cell, the angles will be checked to correspondence. If a match is found, this cell will be used for further processing. This option should generate the most matches.
+Check permutations of the axes for correspondence with your cell, but do not check linear combinations. This is useful to avoid a potential problem when one of the unit cell axis lengths is close to a multiple of one of the others. Use with \fBdirax\fR and \fBmosflm\fR.
-.IP \fBcompare\fR
-.PD
-The cell will be checked for correspondence after only a simple permutation of the axes. This is useful when the target cell is subject to reticular twinning, such as if one cell axis length is close to twice another. With \fB--cell-reduction=reduce\fR there would be a possibility that the axes might be confused in this situation. This happens for lysozyme (1VDS), so watch out.
+.IP \fB-bad\fR
+Do not check that the cell accounts for any of the peaks as described in \fBdirax\fR above. Might be useful to debug initial indexing problems, or if there are many multi-crystal patterns and the indexing method has no concept of multiple crystals per pattern (which, at the moment, means all of them). Can be used with any indexing method.
.PP
-The tolerance for matching with \fBreduce\fR and \fBcompare\fR can be set using \fB--tolerance=\fR\fIa,b,c,angl\fR \- see below for more details. Cells from these reduction routines are further constrained to be right-handed, but no such constraint will be applied if you use \fB--cell-reduction=none\fR. Always using a right-handed cell means that the Bijvoet pairs can be told apart.
+The default indexing method is 'none', which means no indexing will be done. This is useful if you just want to check that the peak detection is working properly.
-.PP
-If the unit cell is centered (i.e. if the space group begins with I, F, H, A, B, C), you should be careful when using "compare" for the cell reduction, since (for example) DirAx will always find a primitive unit cell, and this cell must be converted to the non-primitive conventional cell from the PDB.
+Examples of indexing methods: 'dirax,mosflm,reax', 'dirax-raw,mosflm-raw', 'dirax-raw-bad'.
-.PP
-The default is \fB--cell-reduction=none\fR.
.SH PEAK INTEGRATION
-If the pattern could be successfully indexed and the cell reduction gave a
-positive match, peaks will be predicted in the pattern and their intensities
+If the pattern could be successfully indexed, peaks will be predicted in the pattern and their intensities
measured. The peak integration relies on knowing an accurate radius to
integrate the peak within, and that the annulus used to estimate the background
level is not so big that that it covers neighbouring peaks. However,
@@ -179,11 +138,6 @@ Find peaks in the images using \fImethod\fR. See the second titled \fBPEAK DETE
Index the patterns using \fImethod\fR. See the section titled \fBINDEXING METHODS\fR (above) for more information.
.PD 0
-.IP \fB--cell-reduction=\fR\fImethod\fR
-.PD
-Use \fImethod\fR for unit cell reduction. See the section titled \fBCELL REDUCTION\fR (above) for more information.
-
-.PD 0
.IP "\fB-g\fR \fIfilename\fR"
.IP \fB--geometry=\fR\fIfilename\fR
.PD
@@ -235,7 +189,7 @@ When using \fB--peaks=hdf5\fR, read the peak locations from a table in the HDF5
.PD 0
.IP \fB--tolerance=\fR\fItol\fR
.PD
-Set the tolerances for unit cell comparison. \fItol\fR takes the form \fIa\fR,\fIb\fR,\fIc\fR,\fIang\fR. \fIa\fR, \fIb\fR and \fIc\fR are the tolerances, in percent, for the respective direct space axes when using \fBcompare\fR or \fBcompare_ab\fR for cell reduction (see above). \fIang\fR is the tolerance in degrees for the angles. They represent the respective \fIreciprocal\fR space parameters when using \fB--cell-reduction=reduce\fR.
+Set the tolerances for unit cell comparison. \fItol\fR takes the form \fIa\fR,\fIb\fR,\fIc\fR,\fIang\fR. \fIa\fR, \fIb\fR and \fIc\fR are the tolerances, in percent, for the respective direct space axes when using \fB-axes\fR in the indexing method (see below). \fIang\fR is the tolerance in degrees for the angles. When \fBnot\fR using \fB-axes\fR, they represent the respective \fIreciprocal\fR space parameters. Sorry for the horrifying inconsistency.
.PD
The default is \fB--tolerance=5,5,5,1.5\fR.
@@ -309,11 +263,6 @@ with old scripts because this option selects the behaviour which is now the
default.
.PD 0
-.IP \fB--insane\fR
-.PD
-Normally, indexamajig will check that the projected reciprocal space positions of peaks found by the peak detection are close to reciprocal lattice points. This option disables this check, and normally is \fInot\fR a good idea.
-
-.PD 0
.IP \fB--no-bg-sub\fR
.PD
Don't subtract local background estimates from integrated intensities. This is almost never useful, but might help to detect problems from troublesome background noise.
@@ -353,7 +302,7 @@ This page was written by Thomas White.
Report bugs to <taw@physics.org>, or visit <http://www.desy.de/~twhite/crystfel>.
.SH COPYRIGHT AND DISCLAIMER
-Copyright © 2012 Deutsches Elektronen-Synchrotron DESY, a research centre of the Helmholtz Association.
+Copyright © 2012-2013 Deutsches Elektronen-Synchrotron DESY, a research centre of the Helmholtz Association.
.P
indexamajig, and this manual, are part of CrystFEL.
.P