Changes for page The FLASH HDF5 structure
Last modified by sndueste on 2026-01-19 14:35
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... ... @@ -1,3 +1,6 @@ 1 +{{layout}} 2 +{{layout-section ac:type="single"}} 3 +{{layout-cell}} 1 1 == Contents == 2 2 3 3 ... ... @@ -5,20 +5,10 @@ 5 5 {{toc/}} 6 6 7 7 8 -== General information about HDF5 and how to look on it==11 +== General information about HDF5 == 9 9 10 10 HDF5 is a data format maintained by the HDF group. For detailed general information see [[here>>url:https://portal.hdfgroup.org/display/support||shape="rect"]] 11 11 12 -The easiest way to look at the HDF5 files from your beamtime is to use the Jupyter notebook interface to Maxwell: [[https:~~/~~/max-jhub.desy.de/>>https://max-jhub.desy.de/]] 13 - 14 - The file content can be browsed by doubbelclicking on the file. 15 - 16 -Typically the Jupyter notebook starts at your home directory and you have to create a (soft) link to your beamtime folder: open a terminal window (File->New-> Terminal) nad create the link via: 17 - 18 -{{code language="none"}} 19 -> silx view 20 -{{/code}} 21 - 22 22 To download the HDF5 Viewer click [[here>>url:https://portal.hdfgroup.org/display/support/Download+HDFView||shape="rect"]] 23 23 24 24 For use on the DESY Maxwell or PAL (max-fsc or pal) **hdfview** is available in the xray module : ... ... @@ -68,17 +68,25 @@ 68 68 {{/expand}} 69 69 70 70 === HDF examples: === 64 +{{/layout-cell}} 65 +{{/layout-section}} 71 71 67 +{{layout-section ac:type="three_equal"}} 68 +{{layout-cell}} 72 72 * ADC data as example for **fast** **data** (10 Hz): 73 73 74 74 [[image:attach:image2020-11-16_15-26-28.png||height="250"]] 72 +{{/layout-cell}} 75 75 74 +{{layout-cell}} 76 76 * The //average// FEL pulse energy as example for the **slow** **data**. Here the data is not saved with 10 Hz - thus not for every FEL pulse train. The data is typically saved with 1 Hz if the values are changing (like the FEL energy) and every about 20 sec if there is no change for longer time ( e.g. motor set values). Thus to use the data together with the "fast" one, one has to interpolate the data as explained in the examples in the repos below show (e.g. {{code language="none"}}df['GMD_T_average'] = df['GMD_T_average'].interpolate(method='linear'){{/code}}) 77 77 78 78 ( as example only every 10th train ID is listed in the HDF group "index") 79 79 80 80 [[image:attach:image2020-11-16_15-31-45.png||height="250"]] 80 +{{/layout-cell}} 81 81 82 +{{layout-cell}} 82 82 * ((( 83 83 //zraw// group contains the **original DAQ (DOOCS) names** 84 84 ))) ... ... @@ -87,7 +87,11 @@ 87 87 88 88 89 89 [[image:attach:image2020-11-16_16-26-3.png||height="400"]] 91 +{{/layout-cell}} 92 +{{/layout-section}} 90 90 94 +{{layout-section ac:type="single"}} 95 +{{layout-cell}} 91 91 {{info}} 92 92 === There are different options that help you to work with the FLASH HDF5 data in Python === 93 93 ... ... @@ -94,8 +94,11 @@ 94 94 * The currently developed option for large data sets: [[the FAB package>>url:https://hasfcpkg.desy.de/fab/fab.html||shape="rect"]] ... see below 95 95 * and for smaller projects: (% class="Object" %)[[https:~~/~~/gitlab.desy.de/christopher.passow/flash-daq-hdf>>url:https://gitlab.desy.de/christopher.passow/flash-daq-hdf||shape="rect"]] 96 96 97 -(% class="Object" %)See also the collection of Demo data and sample scripts : [[ Collection ofHDF5sampledatafrom differentbeamlines>>doc:FLASHUSER.Offline data analysis (DAQ).Collection of HDF5 sample data from different beamlines.WebHome]] and [[DEMO - Working with FLASHdata>>doc:FLASHUSER.Offline data analysis (DAQ).DEMO - Working with FLASH data.WebHome]]102 +(% class="Object" %)See also the collection of Demo data and sample scripts : [[doc:FS-FLASH USER tmp.Data Acquisition and controls 1.DAQ and controls overview.Offline data analysis (DAQ).Collection of HDF5 sample data from different beamlines.WebHome]] and [[doc:FS-FLASH USER tmp.Data Acquisition and controls 1.DAQ and controls overview.Offline data analysis (DAQ).DEMO - Working with FLASH data.WebHome]] 98 98 {{/info}} 104 +{{/layout-cell}} 105 +{{/layout-section}} 106 +{{/layout}} 99 99 100 100 101 101 ... ... @@ -103,7 +103,7 @@ 103 103 104 104 The complete list for the relation between DOOCS names and HDF5 names for the recordable parameters can be found in [[DESY's Repository>>url:https://stash.desy.de/projects/CS/repos/pah/browse/src/camp/data/channel2HdfName.dat||shape="rect"]]. 105 105 106 -== Most popular FLASH parameters and their names in HDF5, DOOCS and ( .raw) DAQ ==114 +== Most popular FLASH parameters and their names in HDF5, DOOCS and (raw) DAQ == 107 107 108 108 {{id name="DOOCSparameters"/}} 109 109 ... ... @@ -115,7 +115,7 @@ 115 115 116 116 The previously used naming scheme (2024 and before) can be found here: 117 117 118 -{{expand expanded="false" title="FLASH1 naming scheme used until 2024"}}126 +{{expand expanded="false" title="FLASH1 Naming scheme used until 2024"}} 119 119 ==== (% id="cke_bm_8853497S" style="display:none" %) (%%)Beamline info (FLASH1) ==== 120 120 121 121 {{code language="none"}}/FL1/Beamlines/Attenuator/pressure{{/code}} ... ... @@ -869,23 +869,6 @@ 869 869 desc : The bunch number of the bunch used for the wavelength calculation 870 870 units : 871 871 872 -{{expand expanded="false" title="More detailed info on OPIS properties"}} 873 -FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL370,'%','relative width of photoline in percent of the FEL photon energy ROI1, rising flank' 874 -FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL375,'%','relative width of photoline in percent of the FEL photon energy ROI1, tailing flank' 875 -FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL470,'%','relative width of photoline in percent of the FEL photon energy ROI1, mean' 876 -FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL371,'%','relative width of photoline in percent of the FEL photon energy ROI2, rising flank' 877 -FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL376,'%','relative width of photoline in percent of the FEL photon energy ROI2, tailing flank' 878 -FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL471,'%','relative width of photoline in percent of the FEL photon energy ROI2, mean' 879 -FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL372,'%','relative width of photoline in percent of the FEL photon energy ROI3, rising flank' 880 -FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL377,'%','relative width of photoline in percent of the FEL photon energy ROI3, tailing flank' 881 -FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL472,'%','relative width of photoline in percent of the FEL photon energy ROI3, mean' 882 -FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL373,'%','relative width of photoline in percent of the FEL photon energy ROI4, rising flank' 883 -FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL378,'%','relative width of photoline in percent of the FEL photon energy ROI4, tailing flank' 884 -FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL473,'%','relative width of photoline in percent of the FEL photon energy ROI4, mean' 885 -FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL374,'%','relative width of photoline in percent of the FEL photon energy ROI5, rising flank' 886 -FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL379,'%','relative width of photoline in percent of the FEL photon energy ROI5, tailing flank' 887 -FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL474,'%','relative width of photoline in percent of the FEL photon energy ROI5, mean' 888 -{{/expand}} 889 889 890 890 If Opis is running typically on the the averaged data is saved. For several experiments it may make sense to save the information for each single bunch. This is up to now done by saving the complete ADC trace of the TOF setup. This is a huge amount of data and needs processing. This has to be performed after the beamtime in close contact to [[Markus Braune>>mailto:markus.braune@desy.de||shape="rect"]] ( responsible for [[OPIS>>url:http://photon-science.desy.de/facilities/flash/photon_diagnostics/opis_spectrometer/index_eng.html||shape="rect"]]) 891 891 ... ... @@ -1214,7 +1214,7 @@ 1214 1214 1215 1215 {{view-file att--filename="FSLADAQ-DAQParameterlistFL24-2.pdf"}}{{/view-file}} 1216 1216 1217 - internallink to parameter list: [[FS-LA DAQ - XWiki>>url:https://xwiki.desy.de/xwiki/bin/view/FSLADAQ/]]1208 + 1218 1218 {{/info}} 1219 1219 1220 1220 {{expand title="Laser parameters used until 2023"}}