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author | Thomas White <taw@physics.org> | 2011-06-16 17:53:28 +0200 |
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committer | Thomas White <taw@physics.org> | 2012-02-22 15:27:28 +0100 |
commit | 34b21127ea75e6a714a6c04a09f226180b2eb541 (patch) | |
tree | db5d75b4365cbbda4728f0d512d24abcdd3ece88 /doc/man | |
parent | aa4d05d94275baa8c87acc6343a23d16f1877b24 (diff) |
Move documentation to manpages
Diffstat (limited to 'doc/man')
-rw-r--r-- | doc/man/crystfel_geometry.1 | 123 | ||||
-rw-r--r-- | doc/man/indexamajig.1 | 220 | ||||
-rw-r--r-- | doc/man/pattern_sim.1 | 36 | ||||
-rw-r--r-- | doc/man/process_hkl.1 | 51 |
4 files changed, 430 insertions, 0 deletions
diff --git a/doc/man/crystfel_geometry.1 b/doc/man/crystfel_geometry.1 new file mode 100644 index 00000000..0deb058e --- /dev/null +++ b/doc/man/crystfel_geometry.1 @@ -0,0 +1,123 @@ +.\" +.\" Geometry man page +.\" +.\" (c) 2009-2011 Thomas White <taw@physics.org> +.\" +.\" Part of CrystFEL - crystallography with a FEL +.\" + +.TH CRYSTFEL\_GEOMETRY 1 +.SH NAME +CrystFEL detector geometry files + +.SH OVERVIEW + +The detector geometry is taken from a text file rather than hardcoded into the +program. Programs which care about the geometry (particularly indexamajig, +pattern_sim and powder_plot) take an argument "--geometry=<file>" +(or "-g <file>"), where <file> contains the geometry. + +A flexible (and pedantic) representation of the detector has been developed to +avoid all possible sources of ambiguity. CrystFEL's representation of a +detector is broken down into one or more "panels", each of which has its own +camera length, geometry, resolution and so on. Each panel fits into the overall +image taken from the HDF5 file, defined by minimum and maximum coordinates in +the "fast scan" and "slow scan" directions. "Fast scan" refers to the direction +whose coordinate changes most quickly as the bytes in the HDF5 file are moved +through. The coordinates are specified inclusively, meaning that a minimum of 0 +and a maximum of 9 results in a width of ten pixels. Counting begins from zero. +All pixels in the image must be assigned to a panel - gaps are not permitted. + +In the current version, panels are assumed to be perpendicular to the incident +beam and to have their edges parallel. Within these limitations, any geometry +can be constructed. + +The job of the geometry file is to establish a relationship between the array +of pixel values in the HDF5 file, defined in terms only of the "fast scan" and +"slow scan" directions, and the laboratory coordinate system defined as follows: + ++z is the beam direction, and points along the beam (i.e. away from the source) ++y points towards the zenith (ceiling). ++x completes the right-handed coordinate system. + +Naively speaking, this means that CrystFEL at the images from the "into the +beam" perspective, but please avoid thinking of things in this way. It's much +better to consider the precise way in which the coordinates are mapped. + +The syntax for a simple geometry might include several entires of the following +form: + +; Lines which should be ignored start with a semicolon. + +; The name before the slash indicates which panel is referred to. You can use +; any name as long as it doesn't start with "bad" (see below). +; The range of pixels in the HDF5 file which correspond to a panel are given: +panel0/min_fs = 0 +panel0/min_ss = 0 +panel0/max_fs = 193 +panel0/max_ss = 184 + +; The readout direction (x, y or 0). If more than three peaks are found in +; the same readout region, they are all discarded. This helps to avoid +; problems due to streaks appearing along the readout direction. +; If the badrow direction is '-', then the culling described above will not +; be performed for this panel. +panel0/badrow_direction = - + +; The resolution (in pixels per metre) for this panel +panel0/res = 9090.91 + +; The characteristic peak separation in pixels. The peak detection will assume +; that genuine peaks are separated by at least this amount. +panel0/peak_sep = 6.0 + +; You need to specify the peak integration radius, which should be a little +; larger than the actual radii of the peaks in pixels +panel0/integr_radius = 2.0 + +; The camera length (in metres) for this panel +; You can also specify the HDF path to a scalar floating point value containing +; the camera length in millimetres. +panel0/clen = /LCLS/detectorPosition + +; For this panel, the fast and slow scan directions correspond to the given +; directions in the lab coordinate system described above, measured in pixels. +panel0/fs = +y +panel0/ss = -x + +; The corner of this panel, defined as the first point in the panel to appear in +; the HDF5 file, is now given a position in the lab coordinate system. +; Note that "first point in the panel" is a conceptual simplification. We refer +; to that corner, and to the very corner of the pixel - NOT, for example, to the +; centre of the first pixel to appear. +panel0/corner_x = 429.39 +panel0/corner_y = -17.30 + +; You can suppress indexing for this panel if required, by setting "no_index" to +; "true" or "1". +panel0/no_index = 0 + +; You can also specify bad regions. Peaks with centroid locations within such +; a region will not be integrated nor indexed. Bad regions are specified in +; pixel units, but in the lab coordinate system (i.e. "y" points at the ceiling, +; "z" is the beam direction and "x" completes the right-handed system). +badregionA/min_x = -20.0 +badregionA/max_x = +20.0 +badregionA/min_y = -100.0 +badregionA/max_y = +100.0 + +; If you have a bad pixel mask, you can include it in the HDF5 file as an +; unsigned 16-bit integer array of the same size as the data. You need to +; give its path within each HDF5 file, and two bitmasks. The pixel is +; considered good if all of the bits which are set in "mask_good" are set, AND +; if none of the bits which are set in "mask_bad" are set. +mask = /processing/hitfinder/masks +mask_good = 0x27 +mask_bad = 0x00 + +; Any of the per-panel values can be given without a panel prefix, for example: +peak_sep = 6.0 +; in which case the value will be used for all *subsequent* panels. + + +See the "examples" folder for some examples (look at the ones ending in .geom). diff --git a/doc/man/indexamajig.1 b/doc/man/indexamajig.1 new file mode 100644 index 00000000..fcb1afc4 --- /dev/null +++ b/doc/man/indexamajig.1 @@ -0,0 +1,220 @@ +.\" +.\" indexamajig man page +.\" +.\" (c) 2009-2011 Thomas White <taw@physics.org> +.\" +.\" Part of CrystFEL - crystallography with a FEL +.\" + +.TH INDEXAMAJIG 1 +.SH NAME +indexamajig \- bulk indexing and data reduction program +.SH SYNOPSIS +.PP +.B indexamajig +[options] + +.SH DESCRIPTION + +The "indexamajig" program 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 in the form "h k l I", with some extra +information about the locations of the peaks. + +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: + +indexamajig -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 + +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 +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>). + +You can include a table of saturation values for in the HDF5 file, if you have +a method for estimating the intensities of saturated peaks. It goes in +/processing/hitfinder/peakinfo_saturated, and should be an n*3 two dimensional +array, where the first two columns contain fast scan and slow scan coordinates +(in that order) and the third contains the value which should belong in a peak +at the given location. The value will be spread in a small cross centred on +that location. + +See doc/geometry for information about how to create a geometry description +file. + +You can control what information is included in the output stream using +' --record=<flags>'. Possible flags are: + + pixels Include a list of sums of pixel values within the + integration domain, correcting for individual pixel + solid angles. + + integrated Include a list of reflection intensities, produced by + integrating around predicted peak locations. + + peaks Include peak locations and intensities from the peak + search. + + peaksifindexed As 'peaks', but only if the pattern could be indexed. + + peaksifnotindexed As 'peaks', but only if the pattern could NOT be indexed. + +So, if you just want the integrated intensities of indexed peaks, use +"--record=integrated". If you just want to check that the peak detection is +working, used "--record=peaks". 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 +"--record=integrated,peaksifnotindexed" and then use "check-peak-detection" from +the "scripts" folder to visualise the results of the peak detection. + +.SH PEAK DETECTION + +You can control the peak detection on the command line. Firstly, you can choose +the peak detection method using "--peaks=<method>". Currently, two possible +values for "method" are available. "hdf5" will take the peak locations from the +HDF5 file. It expects a two dimensional array at /processing/hitfinder/peakinfo +where size in the first dimension is the number of peaks and the size in the +second dimension is three. The first two columns contain the x and y +coordinate (see the "Note about data orientation" in geometry.txt for details), +the third contains the intensity. However, the intensity will be ignored since +the pattern will always be re-integrated using the unit cell provided by the +indexer on the basis of the peaks. + +The "zaef" method uses a simple gradient search after Zaefferer (2000). You can +control the overall threshold and minimum gradient for finding a peak using the +"--threshold" and "--min-gradient" options. Both of these have units of "ADU" +(i.e. units of intensity according to the contents of the HDF5 file). + +A minimum peak separation can also be provided in the geometry description file +(see geometry.txt 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 "by proximity". + +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: + + dirax : invoke DirAx + mosflm : invoke MOSFLM (DPS) + +Depending on what you have installed. For "dirax" and "mosflm", you need to +have the dirax or ipmosflm binaries in your PATH. + +Example: --indexing=dirax,mosflm + +.SH CELL REDUCTION + +You can choose from various options for cell reduction with the +"--cell-reduction=" option. The choices are "none", "reduce" and "compare". +This choice is important because all autoindexing methods produce an "ab +initio" estimate of the unit cell (nine parameters), rather than just finding +the orientation of the target cell (three parameters). It's clear that this is +not optimal, and will hopefully be fixed in future versions. + +With "none", 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 some kind of histogram +of the resulting parameters from the output stream to see which are the most +popular. If you're lucky, this will reveal the true unit cell. + +With "reduce", 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, but might produce spurious results in many cases. The predicted peaks +are always checked to verify that at least 10% of the predicted peaks are close +to peaks located by the peak search. If not, the next candidate unit cell is +tried until there are no more options. + +The "compare" method is like "reduce", but linear combinations are not taken. +That means that the cell must either match or match after 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 +"reduce", there is a possibility that the axes might be confused in this +situation. This happens for lysozyme (1VDS), so watch out. + +The tolerance for matching with "reduce" and "compare" is hardcoded as 5% in +the reciprocal axis lengths and 1.5 degrees in the (reciprocal) angles. Cells +from these reduction routines are further constrained to be right-handed. The +unmatched raw cell might be left-handed: CrystFEL doesn't check this for you. +Always using a right-handed cell means that the Bijvoet pairs can be told +apart. + +If the unit cell is centered (i.e. if the space group begins with I, R, C, A or +F), 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. + + +.SH TUNING CPU AFFINITIES FOR NUMA HARDWARE + +If you are running indexamajig on a NUMA (non-uniform memory architecture) +machine, a performance gain can sometimes be made by preventing the kernel from +allowing a process or thread to run on a CPU which is distant from the one on +which it started. Distance, in this context, might mean that the CPU is able to +access all the memory visible to the original CPU, but perhaps only relatively +slowly via a cable link. In many cases a group of CPUs will have direct access +to a certain region of memory, and so the process may be scheduled on any CPU in +that group without any penalty. However, scheduling the process to any CPU +outside the group may be slow. When running under Linux, indexamajig is able to +avoid such sub-optimal process scheduling by setting CPU affinities for its +threads. The CPU affinities are also inherited by subprocesses (e.g. MOSFLM or +DirAx). + +To do this usefully, you need to give indexamajig some information about your +hardware's architecture. Specify the size of the CPU groups using +"--cpugroup=<n>". You also need to specify the overall number of CPUs, so that +the program knows when to 'wrap around'. Using "--cpuoffset=<n>", where "n" is +a group number (not a CPU number), allows you to manually skip a few CPUs, which +may be useful if you do not want to use all the available CPUs but want to avoid +running all your jobs on the same ones. + +Note that specifying the above options is NOT the same thing as giving the +number of analyses to run in parallel (the 'number of threads'), which is done +with "-j <n>". The CPU tuning options provide information to indexamajig about +how to set the CPU affinities for its threads, but it does not specify how many +threads to use. + +Example: 72-core Altix UV 100 machine at the author's institution + +This machine consists of six blades, each containing two 6-core CPUs and some +local memory. Any CPU on any blade can access the memory on any other blade, +but the access will be slow compared to accessing memory on the same blade. +When running two instances of indexamajig, a sensible choice of parameters might +be: + +1: --cpus=72 --cpugroup=12 --cpuoffset=0 -j 36 +2: --cpus=72 --cpugroup=12 --cpuoffset=36 -j 36 + +This would dedicate half of the CPUs to one instance, and the other half to the +other. + + +.SH A NOTE ABOUT UNIT CELL SETTINGS + +CrystFEL's core symmetry module only knows about one setting for each unit cell. +You must use the same setting. That means that the unique axis (for cells which +have one) must be "c". + + +.SH KNOWN BUGS + +Don't run more than one indexamajig jobs simultaneously in the same working +directory - they'll overwrite each other's DirAx or MOSFLM files, causing subtle +problems which can't easily be detected. diff --git a/doc/man/pattern_sim.1 b/doc/man/pattern_sim.1 new file mode 100644 index 00000000..d53aeae5 --- /dev/null +++ b/doc/man/pattern_sim.1 @@ -0,0 +1,36 @@ +.\" +.\" pattern_sim man page +.\" +.\" (c) 2009-2011 Thomas White <taw@physics.org> +.\" +.\" Part of CrystFEL - crystallography with a FEL +.\" + +.TH PATTERN\_SIM 1 +.SH NAME +pattern\_sim \- Simulation of nanocrystallographic diffraction patterns +.SH SYNOPSIS +.PP +.B pattern\_sim +[options] + +.SH DESCRIPTION + +pattern_sim does not know about symmetry, so your input reflection list +(give with "-i") must be expanded. You can do this with: + +$ get_hkl -i myfile.hkl -o output.hkl -y mypointgroup -e 1 + +get_hkl does not currently understand symmetry, which means you'll have to +expand any molecular model (the PDB) out to P1 to get the correct results. You +can achieve that, for example, by loading it into Mercury, turning on "Packing" +and re-saving. Alternatively, you can do this using CCP4 with a command like: + +$ echo symgen P63 | pdbset xyzin model.pdb xyzout model-P1.pdb + +While on this subject, you might also want to include hydrogens in the model +using something like: +$ echo HYDROGENS APPEND | hgen xyzin model.pdb xyzout model-with-H.pdb + +Please be sure to read the "Note about Unit Cell Settings" in the documentation +for indexamajig. diff --git a/doc/man/process_hkl.1 b/doc/man/process_hkl.1 new file mode 100644 index 00000000..6c626e31 --- /dev/null +++ b/doc/man/process_hkl.1 @@ -0,0 +1,51 @@ +.\" +.\" process_hkl man page +.\" +.\" (c) 2009-2011 Thomas White <taw@physics.org> +.\" +.\" Part of CrystFEL - crystallography with a FEL +.\" + +.TH PROCESS\_HKL 1 +.SH NAME +process\_hkl \- Monte Carlo merging program +.SH SYNOPSIS +.PP +.B process\_hkl +-i mypatterns.stream -o mydata.hkl -y mypointgroup [options] + +.SH DESCRIPTION + +This program takes as input the data stream from "indexamajig". It merges the +many individual intensities together to form a single list of reflection +intensities which are useful for crystallography. + +Typical usage is of the form: + +$ process_hkl -i mypatterns.stream -o mydata.hkl -y mypointgroup + +.SH CHOICE OF POINT GROUP FOR MERGING + +One of the main features of serial crystallography is that the orientations of +individual crystals are random. That means that the orientation of each +crystal must be determined independently, with no information about its +relationship to the orientation of crystals in other patterns (as would be the +case for a rotation series of patterns). + +Some Laue classes are merohedral. This means that the orientation will have an +ambiguity, but this time more serious. The two (or more) possible +orientations could be called "twins", but the mechanism of their formation is +somewhat different to the conventional use of the term. In these cases, you +will need to merge according to the point group corresponding holohedral Laue +class. + +You can also tell process_hkl the "apparent" symmetry, which is the symmetry as +far as whatever produced the stream was concerned. In the case of most indexing +algorithms, this will be the corresponding holohedral point group (not the +Laue class nor the holohedral Laue class). If you use the "-a" option to give +this information, process_hkl will try to resolve the remaining orientational +ambiguities to get from the apparent symmetry to the true symmetry (given with +"-y"). Currently, it won't do a very good job of it. + +The document twin-calculator.pdf contains more detailed information about this +issue, as well as tables which contain all the required information. |