|
Beamtime |
Beamtime is assigned competitively |
|
Detector |
|
TiB |
Tebibyte |
unit of data storage equal to 2^40 or 1,099,511,627,776 bytes |
TB |
Terabyte |
unit of data storage equal to 10^12 or 1,000,000,000,000 bytes. It is often imprecisely used to refer to tebibytes, most egregiously by operating system software, leading to common incorrect usage |
GiB |
Gibibyte |
unit of data storage equal to 2^30 bytes |
GB |
Gigabyte |
unit of data storage equal to 10^9 or 1,000,000,000 bytes. It is often imprecisely used to refer to gibibytes, most egregiously by operating system software, leading to common incorrect usage |
MiB |
Mebibyte |
unit of data storage equal to 2^20 bytes |
MB |
Megabyte |
unit of data storage equal to 10^6 or 1,000,000 bytes. It is often imprecisely used to refer to mebibytes, most egregiously by operating system software, leading to common incorrect usage |
BIDS |
Brain imaging data structure |
a metadata standard for neuroimaging data of multiple modalities |
SHA256 |
Secure Hash Algorithm 256 |
Cryptographic hash function computed with eight 32-bit words. In this project, this algorithm is used to calculate checksums that allow for identifying changes in data such as data corruption. |
|
Checksum |
A checksum is a small-sized block of data derived from another block of digital data for the purpose of detecting errors that may have been introduced during its transmission or storage. By themselves, checksums are often used to verify data integrity but are not relied upon to verify data authenticity. |
|
Synchrotron |
Particle accelerator for electrons, used to generate X-rays with very high photon flux and spatial and temporal coherence. |
SRµCT |
synchrotron radiation computed mictrotomography |
Computed microtomography using synchrotron radiation as X-ray source |
ANSTO |
Australian Nuclear Science & Technology Organisation |
Umbrella organization running particle accelerators and nuclear reactors in Australia |
AS |
Australian Synchrotron |
Synchrotron in Melbourne, Victoria, Australia |
CLS |
Canadian Light Source |
Synchrotron in Saskatoon, Saskatchewan, Canada |
DESY |
Deutsches Elektronen-Synchrotron |
Umbrella organization running synchrotrons in Germany. Historically, the name referred to a specific synchrotron that is no longer in operation. Colloquially, this name is used to refer to the PETRA III synchrotron. |
PETRA III |
Positron–Electron Tandem Ring Accelerator |
Synchrotron in Hamburg, Germany |
DLS |
Diamond Light Source |
Synchrotron in Didcot, Oxfordshire, United Kingdom |
ESRF |
European Synchrotron Radiation Facility |
Synchrotron in Grenoble, France |
PSI |
Paul Scherrer Institut |
Umbrella organization running the Swiss Light Source and other particle accelerators in Switzerland. Colloquially, this name is sometimes used to refer to the SLS synchrotron. |
SLS |
Swiss Light Source |
Synchrotron in Villigen, Aargau, Switzerland |
SOLEIL |
Source optimisée de lumière d’énergie intermédiaire du LURE (Laboratoire pour l’utilisation du rayonnement électromagnétique) |
Synchrotron in Gif-sur-Yvette, Île-de-France, France |
SPring-8 |
Super Photon Ring – 8 GeV |
Synchrotron in Sayō, Hyōgo, Japan |
BL |
Beamline |
Experimental endstation making use of synchrotron radiation coming from a storage ring. Multiple beamlines can be built for a single storage ring, allowing for multiple, highly varied experiments with a single synchrotron particle accelerator |
IMBL |
Imaging and Medical Beam Line |
Computed microtomography beamline at the Australian Synchrotron. |
BMIT |
Biomedical Imaging and Therapy |
Computed microtomography beamline at the Canadian Light Source |
P05 |
P05 - Imaging Beamline |
Computed microtomography beamline at the Deutsches Elektronen Synchrotron, for lower photon energies < 50 keV |
P07 |
P07 - The High Energy Materials Science Beamline of Helmholtz-Zentrum Hereon and DESY |
Computed microtomography beamline at the Deutsches Elektronen Synchrotron, for higher photon energies > 50 keV |
I13-2 |
The Diamond Manchester Imaging Branchline |
Computed microtomography beamline at the Diamond Light Source |
ID17 |
ID17 - Biomedical Beamline |
Computed microtomography beamline at the European Synchrotron Radiation Facility. Permanently closed down for computed microtomography experiments since July 2022. |
ID19 |
ID19 - Microtomography beamline |
Computed microtomography beamline at the European Synchrotron Radiation Facility |
TOMCAT |
Beamline for TOmographic Microscopy and Coherent rAdiology experimentTs |
Computed microtomography beamline at the Swiss Light Source |
ANATOMIX |
Advanced Nanotomography and Imaging with coherent X rays |
Computed microtomography beamline at the Source optimisée de lumière d’énergie intermédiaire du LURE |
BL20B2 |
BL20B2 Medical and Imaging I beamline |
Computed microtomography beamline at the Super Photon Ring – 8 GeV |
|
Beamtime |
Access to synchrotrons for experiments is given to researchers for a specific amount of time during specific, pre-assigned dates. Both the duration and the specific time slots may be referred to as beamtime |
|
Beamtime proposal |
Access to synchrotrons for experiments is limited due to the demand for beamtime exceeding the available supply. Unpaid, scientific access to synchrotrons is therefore assigned competitively based on experimental proposals, which are typically evaluated by a scientific committee and assigned beamtime based on their relative ranking. |
|
Beamtime proposal number |
Experimental proposals to receive beamtime at a synchrotron are always assigned an internal number by the respective synchrotron for their internal tracking. This number is frequently also used in the Synchrotron file system or databases |
|
User |
Term used to refer to researchers who are external to a synchrotron facility, but have received beamtime and are performing experiments there. |