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authorThomas White <taw@physics.org>2017-07-24 14:58:50 +0200
committerThomas White <taw@physics.org>2017-07-24 14:58:58 +0200
commit6a25a919a8a886f446089bd67e26132dbf46627e (patch)
tree571354a7802bf31c9a27b26fc692a015114d8407 /libcrystfel/src/image.h
parentc9dee7dba94cdd314d2769d30695d995d491b9cb (diff)
Update docs
Diffstat (limited to 'libcrystfel/src/image.h')
-rw-r--r--libcrystfel/src/image.h8
1 files changed, 1 insertions, 7 deletions
diff --git a/libcrystfel/src/image.h b/libcrystfel/src/image.h
index 9719bb59..d7884e4c 100644
--- a/libcrystfel/src/image.h
+++ b/libcrystfel/src/image.h
@@ -173,13 +173,7 @@ struct beam_params
* The field <structfield>data</structfield> contains the raw image data, if it
* is currently available. The data might be available throughout the
* processing of an experimental pattern, but it might not be available when
- * simulating, scaling or merging patterns. Similarly,
- * <structfield>flags</structfield> contains an array of the same dimensions
- * as <structfield>data</structfield> to contain the bad pixel flags.
- * <structfield>twotheta</structfield> likewise contains an array of 2*theta
- * (scattering angle) values in radians, since these values are generated as a
- * by-product of the scattering vector calculation and can be used later for
- * calculating intensities from differential scattering cross sections.
+ * simulating, scaling or merging patterns.
*
* <structfield>crystals</structfield> is an array of %Crystal directly
* returned by the low-level indexing system. <structfield>n_crystals</structfield>