Changes for page The FLASH HDF5 structure

Last modified by sndueste on 2025/02/06 10:55

From version 32.1
edited by erkben
on 2020/06/16 11:05
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To version 41.1
edited by sndueste
on 2021/02/09 14:40
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1 -XWiki.erkben
1 +XWiki.sndueste
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8 8  
9 9  == General information about HDF5 ==
10 10  
11 -HDF5 is a data format maintained by the HDF group. For detailed general information see [[here~[~[image:url:http://hasfweb.desy.de/pub/TWiki/TWikiDocGraphics/external-link.gif~|~|width="13" height="12"~]~]>>url:https://www.hdfgroup.org/HDF5/||shape="rect"]]
11 +HDF5 is a data format maintained by the HDF group. For detailed general information see [[here~[~[image:url:http://hasfweb.desy.de/pub/TWiki/TWikiDocGraphics/external-link.gif~|~|width="13" height="12"~]~]>>url:https://portal.hdfgroup.org/display/support||shape="rect"]]
12 12  
13 -To download the HDF5 Viewer click [[here~[~[image:url:http://hasfweb.desy.de/pub/TWiki/TWikiDocGraphics/external-link.gif~|~|width="13" height="12"~]~]>>url:https://support.hdfgroup.org/products/java/hdfview/index.html||shape="rect"]]
13 +To download the HDF5 Viewer click [[here~[~[image:url:http://hasfweb.desy.de/pub/TWiki/TWikiDocGraphics/external-link.gif~|~|width="13" height="12"~]~]>>url:https://portal.hdfgroup.org/display/support/Download+HDFView||shape="rect"]]
14 14  
15 15  For use on the DESY Maxwell or PAL (max-fsc or pal) **hdfview** is available in the xray module :
16 16  {{code language="none"}}> module load xray{{/code}}
... ... @@ -18,25 +18,78 @@
18 18  
19 19  [[Contents>>doc:||anchor="Contents"]]
20 20  
21 -== FLASH HDF5 structure ==
21 +== The new (starting 2021) HDF5 format ==
22 22  
23 -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 organised according to train IDs. The general structure is:
23 +\\
24 24  
25 +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.
26 +
27 +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.
28 +
29 +Reference implementation, which follows the concept of Python libraries like Pandas, Xarray, or Dask, is given below.
30 +
31 +\\
32 +
33 +{{expand title="Discontinued HDF formats"}}
34 +== Comparison to FLASH's deprecated HDF formats ==
35 +
36 +Before 2021, FLASH provided two different HDF formats formally known as //near-online// and //offline// HDF files.
37 +
38 +All data sets were aligned by the same global index by filling in missing data. Fast DAQ channels  (pulse synchronous data - update 10 Hz) are filled in by NaN or 0, slow channels (not pulse synchronous data - update e.g. 1 Hz ) are interpolated by the DAQs libraries, by keeping the value constant up to the next change.
39 +
40 +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.
41 +
42 +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.
43 +{{/expand}}
44 +
45 +== HDF excerpt: ==
46 +
47 +* ADC data as example for **fast** **data** (10 Hz):            [[image:attach:image2020-11-16_15-26-28.png||height="250"]]
48 +* The //average// FEL pulse energy as example for the **slow** **data** (different e.g. 1 Hz):[[image:attach:image2020-11-16_15-31-45.png||height="250"]]
49 +
50 + ( every 10th train ID is listed in the HDF group "index")
51 +
52 +* (((
53 +//zraw// group contains the **original DAQ (DOOCS) names[[image:attach:image2020-11-16_16-26-3.png||thumbnail="true" height="250"]]**
54 +)))
55 +
56 + of the properties saved in the DESY internal raw format. (For experts)
57 +
58 +\\
59 +
60 +\\
61 +
62 +{{info title="Sample scripts in python"}}
63 +== Reference implementation (Python) ==
64 +
65 +[[~[~[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"]]
66 +
67 +(% class="Object" %)[[https:~~/~~/gitlab.desy.de/christopher.passow/flash-daq-hdf>>url:https://gitlab.desy.de/christopher.passow/flash-daq-hdf||shape="rect"]]
68 +{{/info}}
69 +
70 +\\
71 +
72 +\\
73 +
74 +== The discontinued (till 2021) FLASH HDF5 structure ==
75 +
76 +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:
77 +
25 25  * Electron Diagnostic
26 26  * Photon Diagnostics
27 27  * Beamlines
28 28  * Experiment
29 29  * Timing
30 -[[~[~[image:url:http://hasfweb.desy.de/pub/Setup/HDF5main/HDF5_structure.jpg~|~|alt="HDF5_structure.jpg" width="700" height="500"~]~]>>attach:HDF5_structure.jpg]]
83 +[[image:attach:HDF5_structure.jpg||height="400"]]
31 31  
32 -A detailled description of (most) channels can be found in the lower part of the hdf5 viewer:
33 -[[~[~[image:url:http://hasfweb.desy.de/pub/Setup/HDF5main/HDF5_structure_desc.jpg~|~|alt="HDF5_structure_desc.jpg" width="341" height="413"~]~]>>attach:HDF5_structure_desc.jpg]]
85 +A detailed description of (most) channels can be found in the lower part of the hdf5 viewer:
86 +[[image:attach:HDF5_structure_desc.jpg||thumbnail="true" height="250"]]
34 34  
35 35  [[Contents>>doc:||anchor="Contents"]]
36 36  
37 37  \\
38 38  
39 -== HDF5 example files ==
92 +=== HDF5 example files (old format) ===
40 40  
41 41  Here we have a few HDF5 samples (User data combined with Photon diagnostics data) from a few beamtimes showing the different kind options.
42 42  
... ... @@ -54,8 +54,6 @@
54 54  
55 55  \\
56 56  
57 -\\
58 -
59 59  == Most popular FLASH parameters and their names in HDF5, DOOCS and (raw) DAQ ==
60 60  
61 61  {{id name="DOOCSparameters"/}}
... ... @@ -139,23 +139,29 @@
139 139  \\
140 140  
141 141  
142 -NOTE: Aperture positions in the beamline as well as the positions of the beam steering mirrors are also saved. for more Info contact your local contact
193 +NOTE: Aperture positions in the beamline as well as the positions of the beam steering mirrors are also saved. For more Info contact your local contact
143 143  
144 144  [[Contents>>doc:||anchor="Contents"]]
145 145  
146 146  \\
147 147  
148 -==== Photon Diagnostics SASE ([[GMD>>url:http://photon-science.desy.de/facilities/flash/photon_diagnostics/gmd_intensity_and_position/index_eng.html||shape="rect"]]) / Spectrometer (FLASH1) ====
199 +==== Photon Diagnostics SASE ([[GMD>>url:http://photon-science.desy.de/facilities/flash/photon_diagnostics/gmd_intensity_and_position/index_eng.html||shape="rect"]]) ====
149 149  
201 +\\
202 +
203 +(% style="color: rgb(0,0,0);" %)**Discontinued GMD data recording / evaluation  (VME + PhotonFlux ML server)**
204 +
150 150  {{code language="none"}}/FL1/Photon Diagnostic/GMD/Average energy/energy tunnel{{/code}}
151 -//always saved (PBD)//
152 -DOOCS prop : {{code language="none"}}TTF2.DAQ/PHFLUX/OUT04/VAL{{/code}}
153 -DAQ channel: {{code language="none"}}PBD.PHFLUX/TUNNEL.ENPULSEIC{{/code}}
154 -desc : calibrated average SASE Energy/pulse measured in the TUNNEL before the attenuator (ion current)
206 +//always saved (PBD)//
207 +
208 +(% style="color: rgb(0,0,0);" %)DOOCS prop : {{code language="none"}}TTF2.DAQ/PHFLUX/OUT04/VAL{{/code}} (%%)
209 +(% style="color: rgb(0,0,0);" %)DAQ channel: {{code language="none"}}PBD.PHFLUX/TUNNEL.ENPULSEIC{{/code}}(%%)
210 +desc : calibrated average SASE Energy/pulse measured in the TUNNEL upstream the gas attenuator (ion current)
155 155  units : microJ
156 156  
157 157  {{code language="none"}}/FL1/Photon Diagnostic/GMD/Pulse resolved energy/energy tunnel{{/code}}
158 -//always saved (PBD)//
214 +//always saved (PBD)//
215 +
159 159  DOOCS prop : {{code language="none"}}TTF2.DAQ/PHFLUX/OUT34/VAL{{/code}}
160 160  DAQ channel: {{code language="none"}}PBD.PHFLUX/TUNNEL.ENERGYPULSE.USER{{/code}}
161 161  desc :Energy per pulse Tunnel (from e-) - the values are set to "0" if there was no SASE beam in the FEL
... ... @@ -169,7 +169,8 @@
169 169  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]]**
170 170  
171 171  {{code language="none"}}/FL1/Photon Diagnostic/GMD/Average energy/energy BDA{{/code}}
172 -//always saved (PBD)//
229 +//always saved (PBD)//
230 +
173 173  DOOCS prop : {{code language="none"}}TTF2.DAQ/PHFLUX/OUT05/VAL{{/code}}
174 174  DAQ channel: {{code language="none"}}PBD.PHFLUX/BDA.ENPULSEIC{{/code}}
175 175  desc : calibrated average SASE Energy/pulse measured in the BDA (in the experimental hall) after the attenuator (ion current)
... ... @@ -176,7 +176,8 @@
176 176  units : microJ
177 177  
178 178  {{code language="none"}}/FL1/Photon Diagnostic/GMD/Pulse resolved energy/energy BDA{{/code}}
179 -//always saved (PBD)//
237 +//always saved (PBD)//
238 +
180 180  DOOCS prop : {{code language="none"}}TTF2.DAQ/PHFLUX/OUT35/VAL{{/code}}
181 181  DAQ channel: {{code language="none"}}PBD.PHFLUX/BDA.ENERGYPULSE.USER{{/code}}
182 182  desc :Energy per pulse BDA (from e-) - the values are set to "0" if there was no SASE beam in the FEL
... ... @@ -189,6 +189,57 @@
189 189  desc :Energy per pulse BDA (from e-) - uncorrected values. There are also values saved if there was no beam ... just background noise
190 190  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]]**
191 191  
251 +\\
252 +
253 +(% style="color: rgb(0,0,0);" %)**NEW (2021) GMD data recording / evaluation  (MTCA, analog to FLASH2 and XFEL)**
254 +
255 +{{code language="none"}}/FL1/Photon Diagnostic/GMD/Average energy/energy tunnel{{/code}}
256 +//always saved (PBD)//
257 +(% style="color: rgb(0,0,0);" %)DOOCS prop : {{code language="none"}}FLASH.FEL/XGM.PHOTONFLUX/FL1.TUNNEL/PHOTONFLUX.UJ{{/code}} (%%)
258 +(% style="color: rgb(0,0,0);" %)DAQ channel: {{code language="none"}}FLASH.FEL/XGM.PHOTONFLUX/FL1.TUNNEL/PHOTONFLUX.UJ{{/code}}
259 +
260 +desc : calibrated average SASE Energy/pulse measured in the TUNNEL upstream the gas attenuator
261 +units : microJ
262 +
263 +\\
264 +
265 +{{code language="none"}}/FL1/Photon Diagnostic/GMD/Pulse resolved energy/energy tunnel{{/code}}
266 +//always saved (PBD)//
267 +
268 +(% style="color: rgb(0,0,0);" %)DOOCS prop : 
269 +{{code language="none"}}FLASH.FEL/XGM.INTENSITY/FL1.TUNNEL/INTENSITY.TD{{/code}}DAQ channel: {{code language="none"}}FLASH.FEL/XGM.INTENSITY/FL1.TUNNEL/INTENSITY.TD{{/code}}
270 +
271 +desc : Energy per pulse measured in the Tunnel.  In addition measurement errors and beam position are included for EACH pulse in the pulse train  !! (see below)
272 +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]]**
273 +
274 +{{info title="GMD pulse resolved data structure"}}
275 +For every pulse in the pulse train the information is saved:
276 +
277 +
278 +1. **Intensity per pulse** (a.u. (more or less µJ ))
279 +1. Intensity per pulse (auxillary GMD) - not used
280 +1. Position horizontal (mm, for a single pulse the position information may be very noisy  - talk to your local contact)
281 +1. Position vertical (mm, for a single pulse the position information may be very noisy  - talk to your local contact)
282 +1. **Intensity per pulse sigma** (a.u. (more or less µJ ), (% style="color: rgb(0,0,0);" %)This parameter gives an indication of the error of the measurement of the pulse energy. This takes signal to noise,  detector resolution, uncertainties in crossection etc into account. (it is NOT the measurement of the statistical fluctuation of the SASE pulses)(%%))
283 +1. Position horizontal sigma  (mm, indicates the error (RMS, sigma) of the measurement according to known uncertainties and signal to noise)
284 +1. Position vertical sigma  (mm, indicates the error (RMS, sigma) of the measurement according to known uncertainties and signal to noise)
285 +1. Combined warning and error flags
286 +
287 +The pulse energy and the error are plotted for the first bunch of the pulse trains saved in this 
288 +file
289 +
290 +
291 +[[image:attach:image2021-2-9_10-51-6.png||height="250"]]
292 +
293 +\\
294 +{{/info}}
295 +
296 +All values for the GMD are also available for the** BDA GMD **which is located in the experimental hall down stream the gas attenuator. If the attenuator is on the ratio between BDA and Tunnel signal shows the attenuation. **BUT NOTE** that the filter units  are downstream the GMD. So if filters  are used this influence is NOT measured by the GMD BDA !
297 +
298 +\\
299 +
300 +Besides  pulse energy the GMD also provides information about the beam position
301 +
192 192  {{code language="none"}}/FL1/Photon Diagnostic/GMD/Beam position/position BDA horizontal{{/code}}
193 193  //always saved (PBD)//
194 194  DOOCS prop : {{code language="none"}}FLASH.FEL/XGM.POSMON/FL1.BDA/IX.POS{{/code}}
... ... @@ -217,6 +217,10 @@
217 217  desc :Beam position of the photon Beam determined by the GMD (TUNNEL, y=vertical)
218 218  units : mm
219 219  
330 +\\
331 +
332 +==== Spectrometer (FLASH1) ====
333 +
220 220  {{code language="none"}}/FL1/Photon Diagnostic/Wavelength/Tunnelspectrometer/wavelength{{/code}}
221 221  _always saved (when Spectrum is measured !!) (PBD) _
222 222  DOOCS prop : {{code language="none"}}TTF2.EXP/PHOTONWL.ML/WAVE_LENGTH/VAL.TD{{/code}}
... ... @@ -300,10 +300,25 @@
300 300  //always saved (PBD)//
301 301  DOOCS prop : {{code language="none"}}FLASH.SDIAG/BAM/4DBC3/LOW_CHARGE_ARRIVAL_TIME{{/code}}
302 302  DAQ channel: {{code language="none"}}FLASH.SDIAG/BAM.DAQ/4DBC3.LOW_CHARGE_ARRIVAL_TIME{{/code}}
303 -desc: Electron bunch arrival time measured with the BAM (more or less) before the undulator (pulse resolved data)
304 -units: ps (bigger numbers indicate later arrivaltime of the electrons)
305 -note: besides the arivaltime from FLASH1 there is also the FLASH2/3 electron arrival time saved. [[LINK to detailled 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"]] and to a recent  [[talk about the working principle of the BAM>>attach:BAM-basics and outlook-2018_DESY-template_16-9Format.pdf]]
417 +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).
418 +units: ps (bigger numbers indicate later arrivaltime of the electrons)
306 306  
420 +{{code language="none"}}/FL1/Electron Diagnostic/BAM/1SFELC/electron bunch arrival time (low charge){{/code}}
421 +//always saved (PBD)//
422 +DOOCS prop : {{code language="none"}}FLASH.SDIAG/BAM/1SFELC/LOW_CHARGE_ARRIVAL_TIME{{/code}}
423 +DAQ channel: {{code language="none"}}FLASH.SDIAG/BAM.DAQ/1SFELC.LOW_CHARGE_ARRIVAL_TIME{{/code}}
424 +desc: Electron bunch arrival time measured with the BAM  before the undulator (pulse resolved data). This one was newly installed in 2020.
425 +units: ps (bigger numbers indicate later arrivaltime of the electrons)
426 +
427 +{{info title="BAM hints"}}
428 +* besides the arrivaltime from FLASH1 there is also the FLASH2/3 electron arrival time saved.In case of doubt ask your local contact
429 +* [[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]]
430 +* [[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"]]
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 +
307 307  ===== electron beam profile =====
308 308  
309 309  {{code language="none"}}/FL1/Electron Diagnostic/Electron bunch profile/TDS profile{{/code}}
... ... @@ -332,7 +332,7 @@
332 332  ===== electron bunch energy =====
333 333  
334 334  {{code language="none"}}/FL1/Electron Diagnostic/Electron energy/average electron energy{{/code}}
335 -_always saved (PBD)
464 +//always saved (PBD)//
336 336  DOOCS prop : {{code language="none"}}TTF2.DAQ/ENERGY.DOGLEG/E_INTRA_MEAN/VAL{{/code}}
337 337  DAQ channel: {{code language="none"}}PBD.ENERGY.DOGLEG/E_MEAN{{/code}}
338 338  desc: electron bunch energy (average over the bunch train)
... ... @@ -340,7 +340,7 @@
340 340  \\
341 341  
342 342  {{code language="none"}}/FL1/Electron Diagnostic/Electron energy/pulse resolved energy{{/code}}
343 -_always saved (PBD)
472 +//always saved (PBD)//
344 344  DOOCS prop : {{code language="none"}}TTF2.DAQ/ENERGY.DOGLEG/E_SPECT/VAL.TD{{/code}}
345 345  DAQ channel: {{code language="none"}}PBD.ENERGY.DOGLEG/E_SPECT{{/code}}
346 346  desc: electron bunch energy bunch resolved
... ... @@ -349,7 +349,7 @@
349 349  \\
350 350  
351 351  {{code language="none"}}/FL1/Electron Diagnostic/Electron energy/wavelength bunch train average{{/code}}
352 -_always saved (PBD)
481 +//always saved (PBD)//
353 353  DOOCS prop : {{code language="none"}}TTF2.DAQ/ENERGY.DOGLEG/LAMBDA_MEAN/VAL{{/code}}
354 354  DAQ channel: {{code language="none"}}PBD.ENERGY.DOGLEG/LAMBDA_MEAN{{/code}}
355 355  desc: Wavelength calculated by the electron bunch energy (average over the bunch train) (FLASH1)
... ... @@ -543,12 +543,12 @@
543 543  
544 544  ==== Beamline info (FLASH2) ====
545 545  
546 -(% style="color: rgb(255,153,0);" %)(not yet available){{code language="none"}}/FL2/Beamlines/Attenuator/pressure  {{/code}}(%%)
547 -(% style="color: rgb(193,199,208);" %)//always saved (PBD2)// (%%)
548 -(% style="color: rgb(193,199,208);" %)DOOCS prop : {{code language="none"}}FLASH.FEL/ATT.GAS_DOSING/FL2.HALL/PRESSURE{{/code}} (%%)
549 -(% style="color: rgb(193,199,208);" %)DAQ channel:  {{code language="none"}}FLASH.FEL/ATT.GAS_DOSING/FL2.HALL/PRESSURE{{/code}} (%%)
550 -(% style="color: rgb(193,199,208);" %)desc: set pressure in the gas attenuator (%%)
551 -(% style="color: rgb(193,199,208);" %)units: mbar(%%)
675 +{{code language="none"}}/FL2/Beamlines/Attenuator/pressure  {{/code}}
676 +(% style="color: rgb(0,0,0);" %)//always saved (PBD2)// (%%)
677 +(% style="color: rgb(0,0,0);" %)DOOCS prop : {{code language="none"}}FLASH.FEL/ATT.GAS_DOSING/FL2.HALL/PRESSURE{{/code}} (%%)
678 +(% style="color: rgb(0,0,0);" %)DAQ channel:  {{code language="none"}}FLASH.FEL/ATT.GAS_DOSING/FL2.HALL/PRESSURE{{/code}} (%%)
679 +(% style="color: rgb(0,0,0);" %)desc: set pressure in the gas attenuator (%%)
680 +(% style="color: rgb(0,0,0);" %)units: mbar(%%)
552 552  \\
553 553  
554 554  {{code language="none"}}/FL2/Beamlines/FL20/Shutter/open{{/code}}
... ... @@ -567,11 +567,13 @@
567 567  units: degree
568 568  \\
569 569  
699 +/FL2/Beamlines/Filter wheel/position wheel 2
700 +always saved (PBD2)
701 +DOOCS prop : {{code language="none"}}FLASH.FEL/FL20H.PH.MOTOR/MOTOR2.MOT3/FPOS{{/code}}
702 +DAQ channel: {{code language="none"}}FLASH.FEL/FL20H.PH.MOTOR/MOTOR2.MOT3/FPOS{{/code}}
703 +desc: Position of the BL filter wheel 2 - to correlate with the filter material please look [[here>>doc:FLASHUSER.jddd-linked help pages.Filter-Units.Filter wheels in FLASH1 and FLASH2.WebHome]]
704 +units: degree
570 570  
571 -//always saved (PBD2)//
572 -\\\\**[[here>>doc:FLASHUSER.jddd-linked help pages.Filter-Units.Filter wheels in FLASH1 and FLASH2.WebHome]]**
573 -{{code language="none"}}/FL2/Beamlines/Filter wheel/position wheel 2 DOOCS prop : FLASH.FEL/FL20H.PH.MOTOR/MOTOR2.MOT3/FPOS DAQ channel: FLASH.FEL/FL20H.PH.MOTOR/MOTOR2.MOT3/FPOS desc: Position of the BL filter wheel 2 - to correlate with the filter material please look units: degree{{/code}}
574 -
575 575  \\
576 576  
577 577  NOTE: Aperture positions in the beamline as well as the positions of the beam steering mirrors are also saved. for more Info contact your local contact
... ... @@ -593,40 +593,37 @@
593 593  
594 594  \\
595 595  
596 -(% style="color: rgb(255,204,0);" %)average Sigma    to be included in
597 -
598 -(% style="color: rgb(193,199,208);" %){{code language="none"}}/FL2/Photon Diagnostic/GMD/Average energy/energy tunnel uncertainty{{/code}} (%%)
599 -(% style="color: rgb(193,199,208);" %)//always saved (PBD2)// (%%)
600 -(% style="color: rgb(193,199,208);" %)DOOCS prop : FLASH.FEL/XGM.PHOTONFLUX/FL2.TUNNEL/PHOTONFLUX.UJ.SIGMA (%%)
601 -(% style="color: rgb(193,199,208);" %)DAQ channel: FLASH.FEL/XGM.PHOTONFLUX/FL2.TUNNEL/PHOTONFLUX.UJ.SIGMA (%%)
602 -(% style="color: rgb(193,199,208);" %)desc :  This parameter gives an indication of the error of the measurement of the average pulse energy. This takes signal to noise,  detector resolution, uncertainties in crossection etc into account. (it is NOT the measurement of the statistical fluctuation of the SASE pulses)(%%)
603 -(% style="color: rgb(193,199,208);" %)units : microJ
604 -
605 -\\
606 -
607 -\\
608 -
609 609  {{code language="none"}}/FL2/Photon Diagnostic/GMD/Pulse resolved energy/energy tunnel{{/code}}
610 610  //always saved (PBD2)//
611 611  DOOCS prop : {{code language="none"}}FLASH.FEL/XGM.INTENSITY/FL2.TUNNEL/INTENSITY.TD{{/code}}
612 612  DAQ channel: {{code language="none"}}FLASH.FEL/XGM.INTENSITY/FL2.TUNNEL/INTENSITY.TD{{/code}}
613 -desc : Energy per pulse measured in the Tunnel  (in fromt of the gas attenuator and the apertures in the Hall)
731 +desc : Energy per pulse measured in the Tunnel  (in front of the gas attenuator and the apertures in the Hall) In addition measurement errors and beam position are included for EACH pulse in the pulse train  !! (see below)
614 614  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]]**
615 615  
616 -\\
734 +{{info title="GMD pulse resolved data structure"}}
735 +For every pulse in the pulse train the information is saved:
736 +
617 617  
618 -\\
738 +1. **Intensity per pulse** (a.u. (more or less µJ ))
739 +1. Intensity per pulse (auxillary GMD) - not used
740 +1. Position horizontal (mm, for a single pulse the position information may be very noisy  - talk to your local contact)
741 +1. Position vertical (mm, for a single pulse the position information may be very noisy  - talk to your local contact)
742 +1. **Intensity per pulse sigma** (a.u. (more or less µJ ), (% style="color: rgb(0,0,0);" %)This parameter gives an indication of the error of the measurement of the pulse energy. This takes signal to noise,  detector resolution, uncertainties in crossection etc into account. (it is NOT the measurement of the statistical fluctuation of the SASE pulses)(%%))
743 +1. Position horizontal sigma  (mm, indicates the error (RMS, sigma) of the measurement according to known uncertainties and signal to noise)
744 +1. Position vertical sigma  (mm, indicates the error (RMS, sigma) of the measurement according to known uncertainties and signal to noise)
745 +1. Combined warning and error flags
619 619  
620 -{{code language="none"}}/FL2/Photon Diagnostic/GMD/Pulse resolved energy/energy tunnel uncertainty (sigma){{/code}}
621 -//always saved (PBD2)//
622 -DOOCS prop : {{code language="none"}}FLASH.FEL/XGM.INTENSITY/FL2.TUNNEL/INTENSITY.SIGMA.TD{{/code}}
623 -DAQ channel: {{code language="none"}}FLASH.FEL/XGM.INTENSITY/FL2.TUNNEL:4{{/code}}
624 -desc :(% style="color: rgb(0,0,0);" %)This parameter gives an indication of the error of the measurement of the pulse energy. This takes signal to noise,  detector resolution, uncertainties in crossection etc into account. (it is NOT the measurement of the statistical fluctuation of the SASE pulses)(%%)
625 -units : a.u. (more or less µJ - related to the value of the pulse energy )
747 +The pulse energy and the error are plotted for the first bunch of the pulse trains saved in this 
748 +file
626 626  
750 +
751 +[[image:attach:image2021-2-9_10-51-6.png||height="250"]]
627 627  
628 -{{code language="none"}}{{/code}}
753 +\\
754 +{{/info}}
629 629  
756 +\\
757 +
630 630  All values for the GMD are also available for the** HALL GMD **which is located in the experimental hall down stream the gas attenuator. If the attenuator is on the ratio between Hall and Tunnel signal shows the attenuation. **BUT NOTE** that the filter unit and the Aperture 4 are downstream the GMD. So if filters and aperture are used this influence is NOT measured by the GMD hall !
631 631  
632 632  \\
... ... @@ -653,13 +653,15 @@
653 653  
654 654  \\
655 655  
784 +/FL2/Photon Diagnostic/GMD/Pulse resolved beam position/position tunnel x
785 +always saved (PBD2)
786 +DOOCS prop : FLASH.FEL/XGM.BPM/FL2.HALL/X.TD
787 +DAQ channel: FLASH.FEL/XGM.BPM/FL2.HALL:2
788 +desc: Besides the well calibrated averaged beam position information there is also the option to measure the beam position on a single bunch level. HOWEVER this methide needs a perfectly adjusted signal level (talk to your local contact !!) and also then the signal to noise is rather small and one needs some averaging ... BUT with this option one can determine if there was a spatial slope on a burst (say forst bunches were lower than the last ones or so ...)
789 +units : mm   
656 656  
657 -//always saved (PBD2)//
658 -\\\\{{code language="none"}}/FL2/Photon Diagnostic/GMD/Pulse resolved beam position/position tunnel x DOOCS prop : FLASH.FEL/XGM.BPM/FL2.HALL/X.TDDAQ channel: FLASH.FEL/XGM.BPM/FL2.HALL:2 desc: {{/code}}Besides the well calibrated averaged beam position information there is also the option
659 -{{code language="none"}}to measure the beam position on a single bunch level. HOWEVER this methide needs a perfectly adjusted signal level (talk to your local contact !!) and also then the signal to noise is rather small and one needs some averaging ... BUT with this option one can determine if there was a spatial slope on a burst (say forst bunches were lower than the last ones or so ...)units : mm    {{/code}}
791 +(x=horizontal, y = vertial)
660 660  
661 -{{code language="none"}}(x=horizontal, y = vertial){{/code}}
662 -
663 663  again the same parameter set is available for the **HALL GMD**
664 664  
665 665  \\
... ... @@ -745,17 +745,30 @@
745 745  =====
746 746  arrival time =====
747 747  
878 +{{code language="none"}}/FL2/Electron Diagnostic/BAM/8FL2XTDS/electron bunch arrival time (low charge){{/code}}
879 +//always saved (PBD2)//
880 +DOOCS prop : {{code language="none"}}FLASH.SDIAG/BAM/8FL2XTDS/LOW_CHARGE_ARRIVAL_TIME{{/code}}
881 +DAQ channel: {{code language="none"}}FLASH.SDIAG/BAM.DAQ/8FL2XTDS.LOW_CHARGE_ARRIVAL_TIME{{/code}}
882 +desc: Electron bunch arrival time measured with the BAM after the FLASH2 undulator (pulse resolved data)
883 +units: ps (bigger numbers indicate later arrivaltime of the electrons)
884 +
748 748  **FL1**{{code language="none"}}//Electron Diagnostic/BAM/4DBC3/electron bunch arrival time (low charge){{/code}}
749 749  //always saved (PBD2)//
750 750  DOOCS prop : {{code language="none"}}FLASH.SDIAG/BAM/4DBC3/LOW_CHARGE_ARRIVAL_TIME{{/code}}
751 751  DAQ channel: {{code language="none"}}FLASH.SDIAG/BAM.DAQ/4DBC3.LOW_CHARGE_ARRIVAL_TIME{{/code}}
752 -desc: Electron bunch arrival time measured with the BAM (more or less) before the undulator (pulse resolved data)
889 +desc: Electron bunch arrival time measured with the BAM  in the accelerator  (pulse resolved data)
753 753  units: ps (bigger numbers indicate later arrivaltime of the electrons)
754 754  
755 -The BAM measures the arrivaltime of** FLASH 1 and FLASH2** in the same data set (thus also sorted in at /FL1/ !). The first values are for FLASH1 bunches.
756 -After a gap of about 70 micros ( 70 colums)  with  as entry for the switching between FLASH 1 and 2 the values for the electrons used in FLASH2 start.  The start time of FLASH2 is also recorded in the DAQ. FLASH1 start time is for historic reasons 700. thus if e.g. the start time of FLASH2 ( property name see below) is 1200 it means that FLASH starts at column 500 (1200-700) ...
892 +\\
757 757  
758 -Docu for BAM:  [[LINK to detailled 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"]] and to a recent [[talk about the working principle of the BAM>>attach:BAM-basics and outlook-2018_DESY-template_16-9Format.pdf]]
894 +{{info title="BAM hints"}}
895 +* The BAM 4DBC3 measures the arrivaltime of** FLASH 1 and FLASH2** in the same data set (thus also sorted in at /FL1/ !).
896 +* The BAM 8FL2XTDS measures only for FLASH2 BUT has the same data structure as the other BAMS ... thus there are also (random) values in in the  FLASH1 time slot 
897 +** Structure: The first values are for FLASH1 bunches. After a gap of about 70 micros ( 70 colums)  with  as entry for the switching between FLASH 1 and 2 the values for the electrons used in FLASH2 start.  The start time of FLASH2 is also recorded in the DAQ. FLASH1 start time is for historic reasons 700. thus if e.g. the start time of FLASH2 ( property name see below) is 1200 it means that FLASH starts at column 500 (1200-700) ... .In case of doubt ask your local contact
898 +* [[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]]
899 +* [[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"]]
900 +* a recent  [[talk about the working principle of the BAM>>attach:BAM-basics and outlook-2018_DESY-template_16-9Format.pdf]]
901 +{{/info}}
759 759  
760 760  
761 761  [[Contents>>doc:||anchor="Contents"]]
... ... @@ -1047,67 +1047,14 @@
1047 1047  
1048 1048  \\
1049 1049  
1050 -=== Samples how to read HDF5 with Matlab ===
1193 +== HDF5 and DOOCS ==
1051 1051  
1052 -The examples apply to HDF files with HDF tree version before vers. 0.3.0.
1195 +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
1053 1053  
1054 -(% style="color: rgb(0,128,0);" %)%% read in the needed data p=path; path(p,'D:\mess-daten\DAQ-data\hdf5\Gotthard') % add the actual folder to the path hdf5file='FLASH1_EXP-2016-03-16T1420.h5'; % data with Gotthard and VLS
1197 +[[Contents>>doc:||anchor="Contents"]]
1055 1055  
1056 -(% style="color: rgb(0,128,0);" %)% h5disp(hdf5file,'/','min') % to get an idea what is in the file % h5info(hdf5file,'/Experiment/Gotthard1/BL.0') % get info about the individual channel
1057 -
1058 -(% style="color: rgb(0,128,0);" %)% read a Number per 10 Hz pulse train:
1059 -
1060 -(% class="code" %)
1061 -(((
1062 -FEL_Wavelength_energy_server=h5read(hdf5file,'/Photon Diagnostic/Wavelength/Calculated by energy/wavelength' );
1063 -)))
1064 -
1065 -(% style="color: rgb(0,128,0);" %)% read in a 1D array (spectrum) %GMD data GMD_Spectrum=h5read(hdf5file,'/Photon Diagnostic/GMD/Pulse resolved energy/energy BDA');
1066 -
1067 -(% style="color: rgb(0,128,0);" %)% This reads in all the data . One can also limit the amount of data read to a subset of the data stored in the file. e.g. for image Data (Gotthard)
1068 -
1069 1069  \\
1070 1070  
1071 -(% class="code" %)
1072 -(((
1073 -Start_event= 500 ; % define the first 10 Hz event
1074 - Number_of_events = 20; % how many 10 Hz events to load
1075 -)))
1076 -
1077 -(% style="color: rgb(0,128,0);" %)% read only part of the data:
1078 -
1079 -(% class="code" %)
1080 -(((
1081 -Gotthard_data=h5read(hdf5file,'/Experiment/Gotthard1/BL.0',[2 650 Start_event],[50 85 Number_of_events]);
1082 -)))
1083 -
1084 -(% style="color: rgb(0,128,0);" %)% start stop increment "manual" for 2 D data : [start bunch number in Gotthard data start pixelin spectrum start sample in 10 Hz trains], % [number of bunches in the Gotthard data number of points in the spectrum number of spectra ]
1085 -
1086 -(% class="code" %)
1087 -(((
1088 -VLS_Spectrum=h5read(hdf5file,'/Photon Diagnostic/Wavelength/VLS online spectrometer/PCO.ROI.X',[400 Start_event],[200 Number_of_events] );
1089 -
1090 -)))
1091 -
1092 -(% style="color: rgb(0,128,0);" %)% start stop increment "manual" for 1D data : [start sample in the spectrum start sample in 10 Hz trains],[number of points in the spectrum number of spectra ]
1093 -
1094 -(% style="color: rgb(0,128,0);" %)%GMD data
1095 -
1096 -(% class="code" %)
1097 -(((
1098 -GMD_Spectrum=h5read(hdf5file,'/Photon Diagnostic/GMD/Pulse resolved energy/energy BDA',[1 Start_event],[40 Number_of_events] );
1099 -)))
1100 -
1101 -[[Contents>>doc:||anchor="Contents"]]
1102 -
1103 -=== How to read HDF5 with Python via FLASHH5 ===
1104 -
1105 -With [[FlashH5>>doc:FLASHUSER.FLASHH5 for easier access of FLASH's HDF5 files]] we provide h5py based examples to access and evaluate FLASH's HDF5 files.
1106 -
1107 1107  \\
1108 1108  
1109 -== HDF5 and DOOCS ==
1110 -
1111 -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
1112 -
1113 -[[Contents>>doc:||anchor="Contents"]]
1203 +\\