Changes for page The FLASH HDF5 structure
Last modified by sndueste on 2025/02/06 10:55
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... ... @@ -19,18 +19,14 @@ 19 19 {{code language="none"}}> module load xray{{/code}} 20 20 {{code language="none"}}> hdfview{{/code}} 21 21 22 -o r youcanuse22 +[[Contents>>doc:||anchor="Contents"]] 23 23 24 - {{codelanguage="none"}}>silxview{{/code}}24 +== The new (starting 2021) HDF5 format == 25 25 26 26 \\ 27 27 28 -[[Contents >>doc:||anchor="Contents"]]28 +FLASH provides a conversion of its data acquisition (DAQ) to the commonly used [[HDF5>>url:https://www.hdfgroup.org/solutions/hdf5/||shape="rect"]] format. Correlated data are mapped by a primary index called **train ID**. Every data set has an individual index of train IDs to identify the data even when data are missing or deviate in update rate.If the data set of choice contains gaps, users have to decide how to treat missing values. DAQ channels are spread across various files with one file name pattern for each DAQ. This means users have to assemble data from different files if necessary. 29 29 30 -== The FLASH HDF5 format == 31 - 32 -FLASH provides a conversion of its data acquisition (DAQ) to the commonly used [[HDF5>>url:https://www.hdfgroup.org/solutions/hdf5/||shape="rect"]] format. Correlated data are mapped by a primary index called **train ID**. Every data set has an individual index of train IDs to identify the data even when data are missing or deviate in update rate. If the data set of choice contains gaps, users have to decide how to treat missing values. DAQ channels are spread across various files with one file name pattern for each DAQ. This means users have to assemble data from different files if necessary. 33 - 34 34 The hierarchy is realized using a human readable named HDF tree with each DAQ channel containing the data sets "//value//" and "//index//". Additionally, the HDF group //zraw// contains a tree of the original DAQ channel names. 35 35 36 36 Reference implementation, which follows the concept of Python libraries like Pandas, Xarray, or Dask, is given below. ... ... @@ -38,7 +38,7 @@ 38 38 \\ 39 39 40 40 {{expand title="Discontinued HDF formats"}} 41 -== =Comparison to FLASH's deprecated HDF formats ===37 +== Comparison to FLASH's deprecated HDF formats == 42 42 43 43 Before 2021, FLASH provided two different HDF formats formally known as //near-online// and //offline// HDF files. 44 44 ... ... @@ -47,25 +47,9 @@ 47 47 While the near-online HDF files were converted live during the beamtime, the offline HDF files were manually compiled weeks/months later. Near-online HDF files were used by a provided API [[BeamtimeDaqAccess>>url:https://confluence.desy.de/display/FLASHUSER/Near-Online+data+analysis#Near-Onlinedataanalysis-BriefUserGuidetoBeamtimeDAQAccess||shape="rect"]], which also searches for DAQ channels in files. With assembled files "by run", all DAQ channels were existing in the same HDF file. While shorter runs usually fitted into one file, longer runs still had to be aggregated over several files. The creation of the assembled type of files still involves the use of fairly unstable DAQ Mex-functions As the environment required for using the Mex-functions is already deprecated, its continued existence is uncertain. 48 48 49 49 The HDF hierarchy is almost identical in all formats. While in the the recent format each DAQ channel contains the data sets "value" and "index", the deprecated format had one data set for each DAQ channel. The deprecated formats supplies no time axis parameters for spectra data types. 50 - 51 -\\ 52 - 53 -**HDF5 example files (old format)** 54 - 55 -Here we have a few HDF5 samples (User data combined with Photon diagnostics data) from a few beamtimes showing the different kind options. 56 - 57 -[[image:attach:image2019-10-21_17-2-50.png||thumbnail="true" width="300"]] [[download HDF5 (Images @ FL2)>>url:https://desycloud.desy.de/index.php/s/nyEgeCWJFC4gao2||shape="rect"]] 58 - 59 -\\ 60 - 61 -[[~[~[image:attach:image2019-10-22_10-52-27.png~|~|thumbnail="true" width="300"~]~]download HDF5 (GHz ADC and OPIS @ FL2)>>url:https://desycloud.desy.de/index.php/s/AeA2kPNNnZgX95A||shape="rect"]] 62 - 63 -\\ 64 - 65 -\\ 66 66 {{/expand}} 67 67 68 -=== HDF ex amples: ===48 +=== HDF excerpt: === 69 69 {{/layout-cell}} 70 70 {{/layout-section}} 71 71 ... ... @@ -103,12 +103,12 @@ 103 103 104 104 {{layout-section ac:type="single"}} 105 105 {{layout-cell}} 106 -{{info}} 86 +{{info title="Sample scripts in python"}} 107 107 === Reference implementation (Python) === 108 108 109 - (imperative) (% class="Object" %)[[https:~~/~~/gitlab.desy.de/christopher.passow/flash-daq-hdf>>url:https://gitlab.desy.de/christopher.passow/flash-daq-hdf||shape="rect"]]89 +[[~[~[image:attach:binder_badge.png~|~|thumbnail="true" width="120"~]~]>>url:https://mybinder.org/v2/git/https%3A%2F%2Fgitlab.desy.de%2Fchristopher.passow%2Fflash-daq-hdf/master||shape="rect"]] 110 110 111 -(% class="Object" %) (object oriented)[[https:~~/~~/gitlab.desy.de/christopher.passow/fdh-builder>>url:https://gitlab.desy.de/christopher.passow/fdh-builder.git||shape="rect"]]91 +(% class="Object" %)[[https:~~/~~/gitlab.desy.de/christopher.passow/flash-daq-hdf>>url:https://gitlab.desy.de/christopher.passow/flash-daq-hdf||shape="rect"]] 112 112 {{/info}} 113 113 {{/layout-cell}} 114 114 {{/layout-section}} ... ... @@ -115,15 +115,49 @@ 115 115 116 116 {{layout-section ac:type="single"}} 117 117 {{layout-cell}} 118 -== Completelist of recordableparameters==98 +== The discontinued (till 2021) FLASH HDF5 structure == 119 119 120 -The complete list for the relation between DOOCS names and HDF5 names for the recordable parameters can be found in [[DESY's Repository~[~[image:url:http://hasfweb.desy.de/pub/TWiki/TWikiDocGraphics/external-link.gif~|~|width="13" height="12"~]~]>>url:https://stash.desy.de/projects/CS/repos/pah/browse/src/camp/data/channel2HdfName.dat||shape="rect"]]. 100 +The photon diagnostic, electron diagnostic and beamline information as well as the information about the pump-probe laser and the infrastructure offered for users (GHz/MHz ADCs) can be included in one HDF5 file which is organized according to train IDs. The general structure is: 101 + 102 +* Electron Diagnostic 103 +* Photon Diagnostics 104 +* Beamlines 105 +* Experiment 106 +* Timing 107 +[[image:attach:HDF5_structure.jpg||height="400"]] 108 + 109 +A detailed description of (most) channels can be found in the lower part of the hdf5 viewer: 110 +[[image:attach:HDF5_structure_desc.jpg||thumbnail="true" height="250"]] 111 + 112 +[[Contents>>doc:||anchor="Contents"]] 113 + 121 121 \\ 122 122 116 +=== HDF5 example files (old format) === 117 + 118 +Here we have a few HDF5 samples (User data combined with Photon diagnostics data) from a few beamtimes showing the different kind options. 119 + 120 +[[image:attach:image2019-10-21_17-2-50.png||thumbnail="true" width="300"]] [[download HDF5 (Images @ FL2)>>url:https://desycloud.desy.de/index.php/s/nyEgeCWJFC4gao2||shape="rect"]] 121 + 122 +\\ 123 + 124 +[[~[~[image:attach:image2019-10-22_10-52-27.png~|~|thumbnail="true" width="300"~]~]download HDF5 (GHz ADC and OPIS @ FL2)>>url:https://desycloud.desy.de/index.php/s/AeA2kPNNnZgX95A||shape="rect"]] 125 + 126 +\\ 127 + 128 +\\ 129 + 130 +[[Contents>>doc:||anchor="Contents"]] 131 + 132 +\\ 133 + 123 123 == Most popular FLASH parameters and their names in HDF5, DOOCS and (raw) DAQ == 124 124 125 125 {{id name="DOOCSparameters"/}} 126 126 138 +The complete list for the relation between DOOCS names and HDF5 names for the recordable parameters can be found in [[DESY's Repository~[~[image:url:http://hasfweb.desy.de/pub/TWiki/TWikiDocGraphics/external-link.gif~|~|width="13" height="12"~]~]>>url:https://stash.desy.de/projects/CS/repos/pah/browse/src/camp/data/channel2HdfName.dat||shape="rect"]]. 139 +The most common and often used ones are summarized below: 140 + 127 127 Note, the HDF group and data set names apply to our HDF tree version since vers. 0.3.0. 128 128 129 129 \\ ... ... @@ -130,6 +130,8 @@ 130 130 131 131 === FLASH1 === 132 132 147 +\\ 148 + 133 133 ==== Beamline info (FLASH1) ==== 134 134 135 135 {{code language="none"}}/FL1/Beamlines/Attenuator/pressure{{/code}} ... ... @@ -206,7 +206,8 @@ 206 206 207 207 ==== Photon Diagnostics SASE ([[GMD>>url:http://photon-science.desy.de/facilities/flash/photon_diagnostics/gmd_intensity_and_position/index_eng.html||shape="rect"]]) ==== 208 208 209 -{{expand title="Discontinued GMD format (used until 2021)"}} 225 +\\ 226 + 210 210 (% style="color: rgb(0,0,0);" %)**Discontinued GMD data recording / evaluation (VME + PhotonFlux ML server)** 211 211 212 212 {{code language="none"}}/FL1/Photon Diagnostic/GMD/Average energy/energy tunnel{{/code}} ... ... @@ -254,11 +254,10 @@ 254 254 DAQ channel: {{code language="none"}}PBD.PHFLUX/BDA.ENERGYPULSE.FF{{/code}} 255 255 desc :Energy per pulse BDA (from e-) - uncorrected values. There are also values saved if there was no beam ... just background noise 256 256 units : a.u. (more or less µJ but need to be calibrated with the "Average energy" for good precision)** [[see here for help>>doc:FLASHUSER.jddd-linked help pages.Calibrating the pulse resolved (electron) data from GMD.WebHome]]** 257 -{{/expand}} 258 258 259 259 \\ 260 260 261 -(% style=" letter-spacing: 0px; color: rgb(0,since2021) GMD data recording / evaluation (sameformatasFLASH2 and XFEL)**277 +(% style="color: rgb(0,0,0);" %)**NEW (2021) GMD data recording / evaluation (MTCA, analog to FLASH2 and XFEL)** 262 262 263 263 {{code language="none"}}/FL1/Photon Diagnostic/GMD/Average energy/energy tunnel{{/code}} 264 264 //always saved (PBD)// ... ... @@ -416,26 +416,8 @@ 416 416 units: nC 417 417 418 418 ===== 419 -arrival time (BAM)=====435 +arrival time ===== 420 420 421 -{{info title="BAM information: updates 2022"}} 422 -* The data format of the BAM has been completely altered in the 2022 shutdown 423 -* before 2022 BAMs were always saving the arrival time information for each 1µs bucked regardless if there were electrons in the accelerator or not. IN addition the arrival times for FL1 and FL2 were saved in the same parameter ... 424 -* THIS is now different. there are new parameters for pulses that go to FL1 and to FL2 (in detail: first time slot of the accelerator and second) 425 -* There has been also a renaming (and relocation) of the BAMs. 426 -** acc: 4DBC3 → FL0.DBC2 427 -** FL1: 1SFELC → FL1.SFELC 428 -** FL2: FL2XTDS → (% style="color: rgb(23,43,77);" %)FL2.SEED5 429 -* for more Info: [[LINK to detailed infos from MSK>>url:https://confluence.desy.de/display/SDiagPublic/BAM+Data+Structure||shape="rect"]] 430 -* [[Link a collection of papers related to the BAM and the analysis of pump-probe experiments>>doc:FLASHUSER.Additional helpful things.FLASH beamlines and instruments references.WebHome]] 431 -* a recent [[talk about the working principle of the BAM>>attach:BAM-basics and outlook-2018_DESY-template_16-9Format.pdf]] 432 -{{/info}} 433 - 434 -\\ 435 - 436 -{{expand title="Discontinued BAM format (used until end 2021)"}} 437 -(% style="color: rgb(0,0,0);" %)**Discontinued BAM data recording ** 438 - 439 439 {{code language="none"}}/FL1/Electron Diagnostic/BAM/4DBC3/electron bunch arrival time (low charge){{/code}} 440 440 //always saved (PBD)// 441 441 DOOCS prop : {{code language="none"}}FLASH.SDIAG/BAM/4DBC3/LOW_CHARGE_ARRIVAL_TIME{{/code}} ... ... @@ -449,30 +449,11 @@ 449 449 DAQ channel: {{code language="none"}}FLASH.SDIAG/BAM.DAQ/1SFELC.LOW_CHARGE_ARRIVAL_TIME{{/code}} 450 450 desc: Electron bunch arrival time measured with the BAM before the undulator (pulse resolved data). This one was newly installed in 2020. 451 451 units: ps (bigger numbers indicate later arrivaltime of the electrons) 452 -{{/expand}} 453 453 454 -\\ 455 - 456 -{{code language="none"}}/FL1/Electron Diagnostic/BAM/4DBC3/electron bunch arrival time (low charge){{/code}} 457 -//always saved (PBD)// 458 -DOOCS prop : {{code language="none"}}FLASH.SDIAG/BAM/4DBC3/LOW_CHARGE_ARRIVAL_TIME{{/code}} 459 -DAQ channel: {{code language="none"}}FLASH.SDIAG/BAM.DAQ/4DBC3.LOW_CHARGE_ARRIVAL_TIME{{/code}} 460 -desc: Electron bunch arrival time measured with the BAM inside the accelerator - however shows a very good correlation to the arrivaltime of the XUV pulses in the experiment (pulse resolved data). 461 -units: ps (bigger numbers indicate later arrivaltime of the electrons) 462 - 463 -{{code language="none"}}/FL1/Electron Diagnostic/BAM/1SFELC/electron bunch arrival time (low charge){{/code}} 464 -//always saved (PBD)// 465 -DOOCS prop : {{code language="none"}}FLASH.SDIAG/BAM/1SFELC/LOW_CHARGE_ARRIVAL_TIME{{/code}} 466 -DAQ channel: {{code language="none"}}FLASH.SDIAG/BAM.DAQ/1SFELC.LOW_CHARGE_ARRIVAL_TIME{{/code}} 467 -desc: Electron bunch arrival time measured with the BAM before the undulator (pulse resolved data). This one was newly installed in 2020. 468 -units: ps (bigger numbers indicate later arrivaltime of the electrons) 469 - 470 -\\ 471 - 472 472 {{info title="BAM hints"}} 473 473 * besides the arrivaltime from FLASH1 there is also the FLASH2/3 electron arrival time saved.In case of doubt ask your local contact 474 474 * [[Link a collection of papers related to the BAM and the analysis of pump-probe experiments >>doc:FLASHUSER.Additional helpful things.FLASH beamlines and instruments references.WebHome]] 475 -* [[LINK to detailed infos from MSK >>url:https://confluence.desy.de/display/SDiagPublic/BAM+Data+Structure||shape="rect"]]454 +* [[LINK to detailed infos from MSK (may only work inside DESY network~[~[image:url:http://hasfweb.desy.de/pub/TWiki/TWikiDocGraphics/external-link.gif~|~|width="13" height="12"~]~]>>url:http://www.desy.de/~~mbock/pages/BAM_daq_channel_descriptions.html||shape="rect"]] 476 476 * a recent [[talk about the working principle of the BAM>>attach:BAM-basics and outlook-2018_DESY-template_16-9Format.pdf]] 477 477 {{/info}} 478 478 ... ... @@ -571,7 +571,7 @@ 571 571 //always saved (PBD)// 572 572 DOOCS prop : {{code language="none"}}TTF2.DIAG/PBD.TOROID.ML/12EXP/CHARGE.TD{{/code}} 573 573 DAQ channel: {{code language="none"}}TTF2.DIAG/PBD.TOROID.ML/12EXP{{/code}} 574 -desc: The bunch pattern as function of time in a burst recorded by toroid diagnostic BEHIND the undulator. (FLASH1) 553 +desc: The bunch pattern as function of time in a burst recorded by toroide diagnostic BEHIND the undulator. (FLASH1) 575 575 units: 576 576 \\ 577 577 ... ... @@ -644,7 +644,7 @@ 644 644 //always saved (PBD)// 645 645 DOOCS prop : {{code language="none"}}TTF2.FEL/TDOLFEL/TDOLFEL/STREAK.CAM.TIME{{/code}} 646 646 DOOCS prop : {{code language="none"}}TTF2.FEL/TDOLFEL/TDOLFEL/STREAK.CAM.TIME{{/code}} 647 -desc: delay 626 +desc: delaytime between the optical laser and the FEL units: ps 648 648 649 649 \\ 650 650 ... ... @@ -654,7 +654,7 @@ 654 654 655 655 ==== User Data (FLASH1) ==== 656 656 657 -The data saved specifically for detectors at an experiment will show up in /Experiment/ there is a large number of options for cameras or monitoring ofslow properties (motor positions etc) for user experiments. For details please ask your local contact.636 +The data saved specifically for detectors at an experiment will show up in /Experiment/ there is a large number of options for cameras or monitoring pslow properties (motor positons etc) for user experiments. For details please ask your local contact. 658 658 659 659 NOTE: If parameters for an experiment are included on short notice the correct naming in the HDF5 may not be in time and the data will show up in /uncategorized/ with the DOOCS names 660 660 ... ... @@ -682,13 +682,13 @@ 682 682 {{code language="none"}}/FL1/Experiment/BL3/ADQ412 GHz ADC/CH03/TD{{/code}} 683 683 684 684 DOOCS prop : {{code language="none"}}FLASH.FEL/ADC.ADQ.PG/EXP1.CH00/CH00.TD or CH00.DAQ.TD{{/code}} 685 -here the {{code language="none"}}CH00.TD{{/code}} is the full ADC trace as it is sampled ( typically several 100.000 samples per pulse train) while the {{code language="none"}}CH00.DAQ.TD{{/code}} trace only has the number of samples which are sent to the DAQ OR if //grouping// is activated the {{code language="none"}}CH00.DAQ.TD{{/code}} con tains only the grouped spectra. To read the ADC trace with an online analysis program the {{code language="none"}}CH00.DAQ.TD{{/code}} is used preferably.664 +here the {{code language="none"}}CH00.TD{{/code}} is the full ADC trace as it is sampled ( typically several 100.000 samples per pulse train) while the {{code language="none"}}CH00.DAQ.TD{{/code}} trace only has the number of samples which are sent to the DAQ OR if //grouping// is activated the {{code language="none"}}CH00.DAQ.TD{{/code}} conatins only the grouped spectra. To read the ADC trace with an online analysis program the {{code language="none"}}CH00.DAQ.TD{{/code}} is used preferablly. 686 686 DAQ channel: {{code language="none"}}FLASH.FEL/ADC.ADQ.PG/EXP1.CH00{{/code}} 687 687 688 688 In addition there are also additional parameters saved like: 689 689 690 690 * {{code language="none"}}sample frequency{{/code}}: it shows the sample frequency in MHz (number of samples per µs). NOTE: the clock of the ADC is NOT synchronized to the FLASH timing system. Thus the number of samples between bunches in the bunch train may be not integer numbers which will be show up for long bunch trains. 691 -* {{code language="none"}}number of samples{{/code}}: total number of sam ples recorded for each 10 Hz trigger670 +* {{code language="none"}}number of samples{{/code}}: total number of samoles recorded for each 10 Hz trigger 692 692 * {{code language="none"}}error (ADC):{{/code}} 0 indicates that there was no error 693 693 694 694 ===== MHz ADCs ===== ... ... @@ -701,7 +701,7 @@ 701 701 In addition there are also additional parameters saved like: 702 702 703 703 * {{code language="none"}}sample frequency{{/code}}: it shows the sample frequency in MHz (number of samples per µs). NOTE: the clock of the ADC is NOT synchronized to the FLASH timing system. Thus the number of samples between bunches in the bunch train may be not integer numbers which will be show up for long bunch trains. 704 -* {{code language="none"}}number of samples{{/code}}: total number of sam ples recorded for each 10 Hz trigger683 +* {{code language="none"}}number of samples{{/code}}: total number of samoles recorded for each 10 Hz trigger 705 705 706 706 [[Contents>>doc:||anchor="Contents"]] 707 707 ... ... @@ -862,7 +862,7 @@ 862 862 // saved opon request (PBD2)// 863 863 DOOCS prop : {{code language="none"}}FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL040{{/code}} 864 864 DAQ channel:{{code language="none"}} FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL040{{/code}} 865 -desc : mean 844 +desc : meanwavelength ( ~~ 1 sec averaging time ) measured in the TUNNEL for a specific bunch out of the bunch train (via photoelectron spectroscopy) 866 866 units : nm 867 867 868 868 \\ ... ... @@ -876,11 +876,11 @@ 876 876 877 877 \\ 878 878 879 -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 sav ing 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"]])858 +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 savng the compleate 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"]] ( respobsible for [[OPIS>>url:http://photon-science.desy.de/facilities/flash/photon_diagnostics/opis_spectrometer/index_eng.html||shape="rect"]]) 880 880 881 881 \\ 882 882 883 -In case OPIS was not operating there is still informat ion about the **set wavelength** for the undulators (see below) which may differ by up to 5 % from the actual wavelength due to different settings in the FEL ...862 +In case OPIS was not operating there is still informaton about the **set wavelength** for the undulators (see below) which may differ by up to 5 % from the actual wavelength due to different settings in the FEL ... 884 884 885 885 \\ 886 886 ... ... @@ -899,21 +899,8 @@ 899 899 900 900 \\ 901 901 902 -===== electronbunchenergy=====881 +===== undulator settings ===== 903 903 904 -{{code language="none"}}/FL2/Electron Diagnostic/Electron energy/energy of first bunch/behind undulators{{/code}} 905 -//always saved (PBD2)// 906 -DOOCS prop : {{code language="none"}}FLASH.DIAG/BEAM_ENERGY_MEASUREMENT/FL2XTDS/ENERGY.FLASH2{{/code}} 907 -DAQ channel: (% style="color: rgb(94,108,132);" %)TTF2.DAQ/PBD2.BEAM.ENERGY.MEAS.ML.COPY/FL2XTDS.ENERGY.FLASH2{{code language="none"}}{{/code}}(%%) 908 -desc: electron bunch energy measured behind the undulator. Data is saved with 10 Hz - BUT (for computation reasons) only the energy of the FIRST bunch is recorded. The data is also available for (% style="color: rgb(94,108,132);" %)extraction and septum in the beginning of FLASH2 909 - 910 -(% style="letter-spacing: 0.0px;" %)units: (% class="twikiNewLink" %)MeV 911 - 912 -\\ 913 - 914 -(% style="color: rgb(94,108,132);font-weight: 600;letter-spacing: 0.0px;" %) 915 -undulator settings 916 - 917 917 {{code language="none"}}/FL2/Electron Diagnostic/Undulator setting/set wavelength{{/code}} 918 918 //always saved (PBD2)// 919 919 DOOCS prop : {{code language="none"}}TTF2.FEEDBACK/FL2.WAVELENGTHCONTROL/FLASH2/WAVELENGTH{{/code}} ... ... @@ -1141,7 +1141,6 @@ 1141 1141 1142 1142 \\ 1143 1143 1144 -(% class="wrapped" %) 1145 1145 |=((( 1146 1146 earlier HDF path (vers. 0.2) 1147 1147 )))|=((( ... ... @@ -1243,6 +1243,14 @@ 1243 1243 [[Contents>>doc:||anchor="Contents"]] 1244 1244 1245 1245 \\ 1211 + 1212 +== HDF5 and DOOCS == 1213 + 1214 +Here is an outdated [[list with the available properties that are always saved (PBD) for FLASH1 as>>attach:FLASH1__DaqChannel2HdfNamePbd.xlsx]] HDF5 names and the corresponding DOOCS names 1215 + 1216 +[[Contents>>doc:||anchor="Contents"]] 1217 + 1218 +\\ 1246 1246 {{/layout-cell}} 1247 1247 {{/layout-section}} 1248 1248 {{/layout}}