Changes for page The FLASH HDF5 structure

Last modified by sndueste on 2026-01-19 14:35

From 95.1 to 94.1 From 106.2 to 106.1

From version 106.1

edited by sndueste
on 2026-01-09 15:29

Change comment: Uploaded new attachment "image.png", version {1}

To version 95.1

edited by sndueste
on 2025-05-19 16:53

Change comment: There is no comment for this version

Raw
Rendered

Summary

Page properties (1 modified, 0 added, 0 removed)
Attachments (0 modified, 0 added, 1 removed)
- image.png

Details

Page properties

Content

@@ -1,3 +1,6 @@
++{{layout}}
++{{layout-section ac:type="single"}}
++{{layout-cell}}
  == Contents ==
@@ -5,25 +5,10 @@
  {{toc/}}
--== General information about HDF5 and how to look on it ==
++== General information about HDF5 ==
  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"]]
--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/]]
--
-- The file content can be browsed by double clicking on the file.
--
--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) and create the link via  :
--
--{{code language="none"}}> ln -sn beamtime path linkname
--e.g.
--> ln -sn /asap3/flash/gpfs/fl23/2025/data/11024321/ ~/beamtime_11024321 {{/code}}
--Then a “beamtime_11024321” folder should appear in your home directory.
--
--
--
--Alternativaly you can also use a conventional HDF viewer:
--
  To download the HDF5 Viewer click [[here>>url:https://portal.hdfgroup.org/display/support/Download+HDFView||shape="rect"]]
  For use on the DESY Maxwell or PAL (max-fsc or pal) **hdfview** is available in the xray module :
@@ -73,17 +73,25 @@
  {{/expand}}
  === HDF examples: ===
++{{/layout-cell}}
++{{/layout-section}}
++{{layout-section ac:type="three_equal"}}
++{{layout-cell}}
  *  ADC data as example for **fast** **data** (10 Hz):
  [[image:attach:image2020-11-16_15-26-28.png||height="250"]]
++{{/layout-cell}}
++{{layout-cell}}
  * 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}})
             ( as example only every 10th train ID is listed in the HDF group "index")
  [[image:attach:image2020-11-16_15-31-45.png||height="250"]]
++{{/layout-cell}}
++{{layout-cell}}
  * (((
  //zraw// group contains the **original DAQ (DOOCS) names**
  )))
@@ -92,7 +92,11 @@
  [[image:attach:image2020-11-16_16-26-3.png||height="400"]]
++{{/layout-cell}}
++{{/layout-section}}
++{{layout-section ac:type="single"}}
++{{layout-cell}}
  {{info}}
  === There are different options that help you to work with the FLASH HDF5 data in Python ===
@@ -99,16 +99,20 @@
  * The currently developed option for large data sets: [[the FAB package>>url:https://hasfcpkg.desy.de/fab/fab.html||shape="rect"]] ... see below
  * 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"]]
--(% class="Object" %)See also the collection of Demo data and sample scripts : [[Collection of HDF5 sample data from different beamlines>>doc:FLASHUSER.Offline data analysis (DAQ).Collection of HDF5 sample data from different beamlines.WebHome]] and [[DEMO - Working with FLASH data>>doc:FLASHUSER.Offline data analysis (DAQ).DEMO - Working with FLASH data.WebHome]]
++(% 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]]
  {{/info}}
++{{/layout-cell}}
++{{/layout-section}}
++{{layout-section ac:type="single"}}
++{{layout-cell}}
++
--
  == Complete list of recordable parameters ==
  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"]].
--== Most popular FLASH parameters and their names in HDF5, DOOCS and (.raw) DAQ ==
++== Most popular FLASH parameters and their names in HDF5, DOOCS and (raw) DAQ ==
  {{id name="DOOCSparameters"/}}
@@ -120,7 +120,7 @@
  The previously used naming scheme (2024 and before) can be found here:
--{{expand expanded="false" title="FLASH1 naming scheme used until 2024"}}
++{{expand expanded="false" title="FLASH1 Naming scheme used until 2024"}}
  ==== (% id="cke_bm_8853497S" style="display:none" %) (%%)Beamline info (FLASH1) ====
  {{code language="none"}}/FL1/Beamlines/Attenuator/pressure{{/code}}
@@ -243,8 +243,8 @@
  {{code language="none"}}/FL1/Photon Diagnostic/GMD/Average energy/energy tunnel{{/code}}
  //always saved (PBD)//
--(% style="color:#000000" %)DOOCS prop : {{code language="none"}}FLASH.FEL/XGM.PHOTONFLUX/FL1.TUNNEL/PHOTONFLUX.UJ{{/code}} (%%)
--(% style="color:#000000" %)DAQ channel: {{code language="none"}}FLASH.FEL/XGM.PHOTONFLUX/FL1.TUNNEL/PHOTONFLUX.UJ{{/code}}
++(% style="color:#000000" %)DOOCS prop : (% style="color: rgb(0, 0, 0); color: rgb(0, 0, 0)" %){{code language="none"}}FLASH.FEL/XGM.PHOTONFLUX/FL1.TUNNEL/PHOTONFLUX.UJ{{/code}}(% style="color:#000000" %) (%%)
++(% style="color:#000000" %)DAQ channel: (% style="color: rgb(0, 0, 0); color: rgb(0, 0, 0)" %){{code language="none"}}FLASH.FEL/XGM.PHOTONFLUX/FL1.TUNNEL/PHOTONFLUX.UJ{{/code}}
  desc : calibrated average SASE Energy/pulse measured in the TUNNEL upstream the gas attenuator
  units : microJ
@@ -253,8 +253,8 @@
  {{code language="none"}}/FL1/Photon Diagnostic/GMD/Pulse resolved energy/energy tunnel{{/code}}
  //always saved (PBD)//
--(% style="color:#000000" %)DOOCS prop : (%%)
--(% style="color:#000000" %){{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}}
++(% style="color:#000000" %)DOOCS prop :
++(% style="color: rgb(0, 0, 0); color: rgb(0, 0, 0)" %){{code language="none"}}FLASH.FEL/XGM.INTENSITY/FL1.TUNNEL/INTENSITY.TD{{/code}}(% style="color:#000000" %)DAQ channel: (% style="color: rgb(0, 0, 0); color: rgb(0, 0, 0)" %){{code language="none"}}FLASH.FEL/XGM.INTENSITY/FL1.TUNNEL/INTENSITY.TD{{/code}}
  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)
  units : a.u. (more or less µJ but need to be calibrated with the "Average energy" for good precision)** [[see here for help>>doc:FS-FLASH USER tmp.jddd-linked help pages.Calibrating the pulse resolved (electron) data from GMD.WebHome]]**
@@ -438,6 +438,431 @@
  units: fs (bigger numbers (typically) indicate later arrival times of the electrons).
++(% style="color:#ff6600" %)DBC2/electron bunch arrival time (raw)  (HDF5 name not yet implemented - see zraw)(% style="color: rgb(255, 102, 0); color: rgb(255, 102, 0)" %){{code language="none"}}/FL1/Electron Diagnostic/BAM/{{/code}}(%%)
++//always saved (PBD)//
++DOOCS prop : FLASH.SDIAG/BAM/FL0.DBC2/ARRIVAL_TIME.ABSOLUTE
++DAQ channel: (% style="color:#000000" %)FLASH.SDIAG/BAM/FL0.DBC2/ARRIVAL_TIME.ABSOLUTE (%%)
++desc: Electron bunch arrival time measured with the BAM inside the accelerator (after bunch compressor 2). Here the complete bunch train from the FEL is recorded (FLASH1 and FLASH2 pulses). Thus there are values from FLASH 1 in the first part. they may be separated by several "0" values if the reprate is different from 1 MHz ...   - It shows a very good correlation to the arrival time  of the XUV pulses in the experiment (see help).
++units: fs (bigger numbers (typically) indicate later arrival times of the electrons).
++
++
++(% style="color:#ff6600" %)DBC2/error  (HDF5 name not yet implemented - see zraw)(% style="color: rgb(255, 102, 0); color: rgb(255, 102, 0)" %){{code language="none"}}/FL1/Electron Diagnostic/BAM/{{/code}}(%%)
++//always saved (PBD)//
++DOOCS prop : FLASH.SDIAG/BAM/FL0.DBC2/ARRIVAL_TIM(% style="color:#000000" %)E.bamError.1(%%)
++DAQ channel: (% style="color:#000000" %)FLASH.SDIAG/BAM/FL0.DBC2/ARRIVAL_TIME.BAMERROR.1(%%)
++desc:(% style="letter-spacing:0.0px" %) status bit: 0 - data is valid; 1 - beam present; 2 - calibration ongoing; 3 - feedback enabled; 4 - feedback acting;  mostly check for bit 0 == 1 is sufficient
++
++
++(% style="color:#ff6600" %)DBC2/status  (HDF5 name not yet implemented - see zraw)(% style="color: rgb(255, 102, 0); color: rgb(255, 102, 0)" %){{code language="none"}}/FL1/Electron Diagnostic/BAM/{{/code}}(%%)
++//always saved (PBD)//
++DOOCS prop : FLASH.SDIAG/BAM/FL0.DBC2/ARRIVAL_TIM(% style="color:#000000" %)E..bamStatus.//1//(%%)
++DAQ channel(% style="color:#000000" %): FLASH.SDIAG/BAM/FL0.DBC2/ARRIVAL_TIME.BAMSTATUS.1(%%)
++desc: (% style="letter-spacing:0.0px" %) status bit: 0 - data is valid; 1 - beam present; 2 - calibration ongoing; 3 - feedback enabled; 4 - feedback acting;  mostly check for bit 0 == 1 is sufficient
++
++
++====== **BAM FL1.SFELC**{{code language="none"}}{{/code}} ======
++
++(% style="font-family:SFMono-Medium,~"SF Mono~",~"Segoe UI Mono~",~"Roboto Mono~",~"Ubuntu Mono~",Menlo,Courier,monospace; letter-spacing:0.0px" %)/FL1/Electron Diagnostic/BAM/**SFELC**(% style="color:#ff6600" %)/electron bunch arrival time   (HDF5 name not yet implemented - see zraw)
++
++//always saved (PBD)//
++(% style="color:#172b4d" %)**FL1.SFELC**(%%)
++(% style="color:#000000" %)channel: FLASH.SDIAG/BAM/(% style="color:#172b4d" %)FL1.SFELC(% style="color:#000000" %)/ARRIVAL_TIME.ABSOLUTE.SA1.COMP
++(% style="color: rgb(0, 0, 0); color: rgb(0, 0, 0)" %){{code language="none"}} DOOCS prop : FLASH.SDIAG/BAM//ARRIVAL_TIME.ABSOLUTE.SA1.COMPDAQ {{/code}}(% style="letter-spacing:0.0px" %)desc: Electron bunch arrival time measured  with the BAM  before the undulator (pulse resolved data). This one was newly installed in 2020.. The property contains only the arrival time of the bunches sent to FL1 (e.g. if there are 30 bunches in FL1 the first 30 values are the arrival time the remaining numbers still may have arbitrary numbers looking like a signal which they are not). These are the same values as the "raw" data below - just "cleaned". The values show a very good correlation to the arrival time  of the XUV pulses in the experiment (see help).
++units: fs (bigger numbers (typically) indicate later arrival times of the electrons).
++
++
++
++(% style="color:#172b4d" %)SFELC(% style="color:#ff6600" %)/electron bunch arrival time (raw)  (HDF5 name not yet implemented - see zraw)(% style="color: rgb(255, 102, 0); color: rgb(255, 102, 0)" %){{code language="none"}}/FL1/Electron Diagnostic/BAM/{{/code}}(%%)
++//always saved (PBD)//
++DOOCS prop : FLASH.SDIAG/BAM/(% style="color:#172b4d" %)FL1.SFELC(%%)/ARRIVAL_TIME.ABSOLUTE
++DAQ channel:** **(% style="color:#000000" %)FLASH.SDIAG/BAM/FL1.SFELC/ARRIVAL_TIME.ABSOLUTE (%%)
++desc: Electron bunch arrival time measured  with the BAM  before the undulator (pulse resolved data). This one was newly installed in 2020.  Here the complete bunch train from the FEL is recorded (FLASH1 and FLASH2 pulses). Thus there are values from FLASH 1 in the first part. they may be separated by several "0" values if the reprate is different from 1 MHz ...   - It shows a very good correlation to the arrival time  of the XUV pulses in the experiment (see help).
++units: fs (bigger numbers (typically) indicate later arrival times of the electrons).
++
++
++(% style="color:#172b4d" %)SFELC(% style="color:#ff6600" %)/error  (HDF5 name not yet implemented - see zraw)(% style="color: rgb(255, 102, 0); color: rgb(255, 102, 0)" %){{code language="none"}}/FL1/Electron Diagnostic/BAM/{{/code}}(%%)
++//always saved (PBD)//
++DOOCS prop : FLASH.SDIAG/BAM/(% style="color:#172b4d" %)FL1.SFELC(%%)/ARRIVAL_TIM(% style="color:#000000" %)E.bamError(%%)
++DAQ channel(% style="color:#000000" %): FLASH.SDIAG/BAM/FL1.SFELC/ARRIVAL_TIME.BAMERROR(%%)
++desc: If the value is 0 , the BAM is working well. If it is non-zero there is a problem !!
++
++
++(% style="color:#172b4d" %)SFELC(% style="color:#ff6600" %)/status  (HDF5 name not yet implemented - see zraw)(% style="color: rgb(255, 102, 0); color: rgb(255, 102, 0)" %){{code language="none"}}/FL1/Electron Diagnostic/BAM/{{/code}}(%%)
++//always saved (PBD)//
++DOOCS prop : FLASH.SDIAG/BAM/(% style="color:#172b4d" %)FL1.SFELC(%%)/ARRIVAL_TIM(% style="color:#000000" %)E..bamStatus.//1//(%%)
++DAQ chann(% style="color:#000000" %)el: FLASH.SDIAG/BAM/FL1.SFELC/ARRIVAL_TIME.BAMSTATUS.1(%%)
++desc:  status bit: 0 - data is valid; 1 - beam present; 2 - calibration ongoing; 3 - feedback enabled; 4 - feedback acting;  mostly check for bit 0 == 1 is sufficient
++
++
++
++===== electron beam profile =====
++
++{{code language="none"}}/FL1/Electron Diagnostic/Electron bunch profile/TDS profile{{/code}}
++//always saved (PBD) - IF LOLA is ON and ACTIVATED in the PBD DAQ (talk to expert)//
++DOOCS prop : {{code language="none"}}TTF2.DAQ/BEAM.PROF.ML/BEAM.PROF/OUT.PROF.CCCED{{/code}}
++DAQ channel: {{code language="none"}}PBD.BEAM.PROF.ML/DAQ.OUT.PROF.CCCED{{/code}}
++desc: temporal profile of electron bunch, y axis in Ampers (FLASH1)
++units: pixel
++
++{{code language="none"}}/FL1/Electron Diagnostic/Electron bunch profile/Expert stuff/TDS calibration constant{{/code}}
++//always saved (PBD) - IF LOLA is ON and ACTIVATED in the PBD DAQ (talk to expert)//
++DOOCS prop : {{code language="none"}}TTF2.DAQ/BEAM.PROF.ML/BEAM.PROF/CALIB.CONST.T{{/code}}
++DAQ channel: = PBD.BEAM.PROF.ML/CCT=
++desc: TDS calibration constant for the x-axis of the profiles: fs per pixel
++units: fs per pixel
++
++{{code language="none"}}/FL1/Electron Diagnostic/Electron bunch profile/TDS profile width rms{{/code}}
++//always saved (PBD) - IF LOLA is ON and ACTIVATED in the PBD DAQ (talk to expert)//
++DOOCS prop : {{code language="none"}}TTF2.DAQ/BEAM.PROF.ML/BEAM.PROF/SOWS.W.CCTED{{/code}}
++DAQ channel: {{code language="none"}}PBD.BEAM.PROF.ML/PROFWIDTHCCTED{{/code}}
++desc: rms pulse width of the measures TDS electron bunch profile
++units: fs
++
++===== electron bunch energy =====
++
++{{code language="none"}}/FL1/Electron Diagnostic/Electron energy/average electron energy{{/code}}
++//always saved (PBD)//
++DOOCS prop : {{code language="none"}}TTF2.DAQ/ENERGY.DOGLEG/E_INTRA_MEAN/VAL{{/code}}
++DAQ channel: {{code language="none"}}PBD.ENERGY.DOGLEG/E_MEAN{{/code}}
++desc: electron bunch energy (average over the bunch train)
++units: (% class="twikiNewLink" %)MeV
++
++{{code language="none"}}/FL1/Electron Diagnostic/Electron energy/pulse resolved energy{{/code}}
++//always saved (PBD)//
++DOOCS prop : {{code language="none"}}TTF2.DAQ/ENERGY.DOGLEG/E_SPECT/VAL.TD{{/code}}
++DAQ channel: {{code language="none"}}PBD.ENERGY.DOGLEG/E_SPECT{{/code}}
++desc: electron bunch energy bunch resolved
++units: (% class="twikiNewLink" %)MeV
++
++
++{{code language="none"}}/FL1/Electron Diagnostic/Electron energy/wavelength bunch train average{{/code}}
++//always saved (PBD)//
++DOOCS prop : {{code language="none"}}TTF2.DAQ/ENERGY.DOGLEG/LAMBDA_MEAN/VAL{{/code}}
++DAQ channel: {{code language="none"}}PBD.ENERGY.DOGLEG/LAMBDA_MEAN{{/code}}
++desc: Wavelength calculated by the electron bunch energy (average over the bunch train) (FLASH1)
++units: nm
++
++[[Contents>>doc:||anchor="Contents"]]
++{{/expand}}
++
++==== Beamline info (FLASH1) ====
++
++{{code language="none"}}/FL1/Beamlines/Attenuator/pressure{{/code}}
++//always saved (PBD)//
++DOOCS prop : {{code language="none"}}FLASH.FEL/GAS_DOSING/FL1.ATTENUATOR/PRESSURE{{/code}}
++DAQ channel: {{code language="none"}}FLASH.FEL/GAS_DOSING/FL1.ATTENUATOR/PRESSURE{{/code}}
++desc: set pressure in the gas attenuator
++units: mbar
++
++{{code language="none"}}/FL1/Beamlines/BL/Fast shutter/open{{/code}}
++//always saved (PBD)//
++DOOCS prop : {{code language="none"}}FLASH.FEL/ADC.SIS.FL1FS/BL.SHUTTER/CH00.TD{{/code}}
++DAQ channel: {{code language="none"}}FLASH.FEL/ADC.SIS.FL1FS/BL.SHUTTER{{/code}}
++desc: BL Beamline Fast shutter state: 1 is open, 0 is closed ( for technical reasons there are 100 vales of this state saved ...)
++units: none
++
++{{code language="none"}}/FL1/Beamlines/PG/Fast shutter/open{{/code}}
++//always saved (PBD)//
++DOOCS prop : {{code language="none"}}FLASH.FEL/ADC.SIS.FL1FS/PG.SHUTTER/CH00.TD{{/code}}
++DAQ channel: {{code language="none"}}FLASH.FEL/ADC.SIS.FL1FS/PG.SHUTTER{{/code}}
++desc: PG Beamline Fast shutter state: 1 is open, 0 is closed ( for technical reasons there are 100 vales of this state saved ...)
++units: none
++
++{{code language="none"}}/FL1/Beamlines/BL/Filters/BL filter wheel/position filter 1{{/code}}
++//always saved (PBD)//
++DOOCS prop : {{code language="none"}}TTF2.FEL/BLFILTERS1/FILTER1/FW.MOTOR.POS{{/code}}
++DAQ channel: {{code language="none"}}TTF2.FEL/BLFILTERS1/FILTER1/FW.MOTOR.POS{{/code}}
++desc: Position of the BL filter wheel 1 - to correlate with the filter material please look [[here>>doc:FS-FLASH USER tmp.jddd-linked help pages.Filter-Units.Filter wheels in FLASH1 and FLASH2.WebHome]]
++units: degree
++
++{{code language="none"}}/FL1/Beamlines/BL/Filters/BL filter wheel/position filter 2{{/code}}
++//always saved (PBD)//
++DOOCS prop : {{code language="none"}}TTF2.FEL/BLFILTERS2/FILTER2/FW.MOTOR.POS{{/code}}
++DAQ channel: {{code language="none"}}TTF2.FEL/BLFILTERS2/FILTER2/FW.MOTOR.POS{{/code}}
++desc: Position of the BL filter wheel 2 - to correlate with the filter material please look [[here>>doc:FS-FLASH USER tmp.jddd-linked help pages.Filter-Units.Filter wheels in FLASH1 and FLASH2.WebHome]]
++units: degree
++
++{{code language="none"}}/FL1/Beamlines/PG/Filters/position filter 1{{/code}}
++//always saved (PBD)//
++DOOCS prop : = TTF2.FEL/BDAF1/BDA.F1/FW.MOTOR.POS=
++DAQ channel: {{code language="none"}}TTF2.FEL/BDAF1/BDA.F1/FW.MOTOR.POS{{/code}}
++desc: Position of the PG filter wheel 1
++units: degree
++
++{{code language="none"}}/FL1/Beamlines/PG/Filters/position filter 2{{/code}}
++//always saved (PBD)//
++DOOCS prop : {{code language="none"}}TTF2.FEL/BDAF2/BDA.F2/FW.MOTOR.POS{{/code}}
++DAQ channel: {{code language="none"}}TTF2.FEL/BDAF2/BDA.F2/FW.MOTOR.POS{{/code}}
++desc: Position of the PG filter wheel 2
++units: degree
++
++{{code language="none"}}/FL1/Beamlines/PG/Filters/position filter 3{{/code}}
++//always saved (PBD)//
++DOOCS prop : {{code language="none"}}TTF2.FEL/PGFILTERS/PGFILTERS/FW.MOTOR.POS{{/code}}
++DAQ channel: {{code language="none"}}TTF2.FEL/PGFILTERS/PGFILTERS/FW.MOTOR.POS{{/code}}
++desc: Position of the PG filter wheel 3
++units: degree
++
++
++
++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
++
++[[Contents>>doc:||anchor="Contents"]]
++
++
++==== Photon Diagnostics SASE ([[GMD>>url:http://photon-science.desy.de/facilities/flash/photon_diagnostics/gmd_intensity_and_position/index_eng.html||shape="rect"]]) ====
++
++{{expand title="Discontinued GMD format (used until 2021)"}}
++(% style="color:#000000" %)**Discontinued GMD data recording / evaluation  (VME + PhotonFlux ML server)**
++
++{{code language="none"}}/FL1/Photon Diagnostic/GMD/Average energy/energy tunnel{{/code}}
++//always saved (PBD)//
++
++(% style="color:#000000" %)DOOCS prop : {{code language="none"}}TTF2.DAQ/PHFLUX/OUT04/VAL{{/code}} (%%)
++(% style="color:#000000" %)DAQ channel: {{code language="none"}}PBD.PHFLUX/TUNNEL.ENPULSEIC{{/code}}(%%)
++desc : calibrated average SASE Energy/pulse measured in the TUNNEL upstream the gas attenuator (ion current)
++units : microJ
++
++{{code language="none"}}/FL1/Photon Diagnostic/GMD/Pulse resolved energy/energy tunnel{{/code}}
++//always saved (PBD)//
++
++DOOCS prop : {{code language="none"}}TTF2.DAQ/PHFLUX/OUT34/VAL{{/code}}
++DAQ channel: {{code language="none"}}PBD.PHFLUX/TUNNEL.ENERGYPULSE.USER{{/code}}
++desc :Energy per pulse Tunnel (from e-) - the values are set to "0" if there was no SASE beam in the FEL
++units : a.u. (more or less µJ but need to be calibrated with the "Average energy" for good precision) **[[see here for help>>doc:FS-FLASH USER tmp.jddd-linked help pages.Calibrating the pulse resolved (electron) data from GMD.WebHome]]**
++
++{{code language="none"}}/FL1/Photon Diagnostic/GMD/Pulse resolved energy/energy tunnel (raw){{/code}}
++//always saved (PBD)//
++DOOCS prop : {{code language="none"}}TTF2.DAQ/PHFLUX/OUT14/VAL{{/code}}
++DAQ channel: {{code language="none"}}PBD.PHFLUX/TUNNEL.ENERGYPULSE.FF{{/code}}
++desc :Energy per pulse Tunnel (from e-) - uncorrected values. There are also values saved if there was no beam ... just background noise
++units : a.u. (more or less µJ but need to be calibrated with the "Average energy" for good precision) **[[see here for help>>doc:FS-FLASH USER tmp.jddd-linked help pages.Calibrating the pulse resolved (electron) data from GMD.WebHome]]**
++
++{{code language="none"}}/FL1/Photon Diagnostic/GMD/Average energy/energy BDA{{/code}}
++//always saved (PBD)//
++
++DOOCS prop : {{code language="none"}}TTF2.DAQ/PHFLUX/OUT05/VAL{{/code}}
++DAQ channel: {{code language="none"}}PBD.PHFLUX/BDA.ENPULSEIC{{/code}}
++desc : calibrated average SASE Energy/pulse measured in the BDA (in the experimental hall) after the attenuator (ion current)
++units : microJ
++
++{{code language="none"}}/FL1/Photon Diagnostic/GMD/Pulse resolved energy/energy BDA{{/code}}
++//always saved (PBD)//
++
++DOOCS prop : {{code language="none"}}TTF2.DAQ/PHFLUX/OUT35/VAL{{/code}}
++DAQ channel: {{code language="none"}}PBD.PHFLUX/BDA.ENERGYPULSE.USER{{/code}}
++desc :Energy per pulse BDA (from e-) - the values are set to "0" if there was no SASE beam in the FEL
++units : a.u. (more or less µJ but need to be calibrated with the "Average energy" for good precision) **[[see here for help>>doc:FS-FLASH USER tmp.jddd-linked help pages.Calibrating the pulse resolved (electron) data from GMD.WebHome]]**
++
++{{code language="none"}}/FL1/Photon Diagnostic/GMD/Pulse resolved energy/energy BDA (raw){{/code}}
++//always saved (PBD)//
++DOOCS prop : {{code language="none"}}TTF2.DAQ/PHFLUX/OUT15/VAL{{/code}}
++DAQ channel: {{code language="none"}}PBD.PHFLUX/BDA.ENERGYPULSE.FF{{/code}}
++desc :Energy per pulse BDA (from e-) - uncorrected values. There are also values saved if there was no beam ... just background noise
++units : a.u. (more or less µJ but need to be calibrated with the "Average energy" for good precision)** [[see here for help>>doc:FS-FLASH USER tmp.jddd-linked help pages.Calibrating the pulse resolved (electron) data from GMD.WebHome]]**
++{{/expand}}
++
++
++(% style="color:#000000; letter-spacing:0px" %)**NEW (since 2021) GMD data recording / evaluation  (same format as FLASH2 and XFEL)**
++
++{{code language="none"}}/FL1/Photon Diagnostic/GMD/Average energy/energy tunnel{{/code}}
++//always saved (PBD)//
++(% style="color:#000000" %)DOOCS prop : {{code language="none"}}FLASH.FEL/XGM.PHOTONFLUX/FL1.TUNNEL/PHOTONFLUX.UJ{{/code}} (%%)
++(% style="color:#000000" %)DAQ channel: {{code language="none"}}FLASH.FEL/XGM.PHOTONFLUX/FL1.TUNNEL/PHOTONFLUX.UJ{{/code}}
++
++desc : calibrated average SASE Energy/pulse measured in the TUNNEL upstream the gas attenuator
++units : microJ
++
++
++{{code language="none"}}/FL1/Photon Diagnostic/GMD/Pulse resolved energy/energy tunnel{{/code}}
++//always saved (PBD)//
++
++(% style="color:#000000" %)DOOCS prop :
++{{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}}
++
++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)
++units : a.u. (more or less µJ but need to be calibrated with the "Average energy" for good precision)** [[see here for help>>doc:FS-FLASH USER tmp.jddd-linked help pages.Calibrating the pulse resolved (electron) data from GMD.WebHome]]**
++
++{{info title="GMD pulse resolved data structure"}}
++For every pulse in the pulse train the information is saved:
++
++1. **Intensity per pulse** (a.u. (more or less µJ ))
++1. Intensity per pulse (auxillary GMD) - not used
++1. Position horizontal (mm, for a single pulse the position information may be very noisy  - talk to your local contact)
++1. Position vertical  (mm, for a single pulse the position information may be very noisy  - talk to your local contact)
++1. **Intensity per pulse sigma**  (a.u. (more or less µJ ), (% style="color:#000000" %)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)(%%))
++1. Position horizontal sigma  (mm, indicates the error (RMS, sigma) of the measurement according to known uncertainties and signal to noise)
++1. Position vertical sigma  (mm, indicates the error (RMS, sigma) of the measurement according to known uncertainties and signal to noise)
++1. Combined warning and error flags
++
++The pulse energy and the error are plotted for the first bunch of the pulse trains saved in this
++file
++
++
++[[image:attach:image2021-2-9_10-51-6.png||height="250"]]
++
++
++{{/info}}
++
++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 !
++
++
++Besides  pulse energy the GMD also provides information about the beam position
++
++{{code language="none"}}/FL1/Photon Diagnostic/GMD/Beam position/position BDA horizontal{{/code}}
++//always saved (PBD)//
++DOOCS prop : {{code language="none"}}FLASH.FEL/XGM.POSMON/FL1.BDA/IX.POS{{/code}}
++DAQ channel: {{code language="none"}}FLASH.FEL/XGM.POSMON/FL1.BDA/IX.POS{{/code}}
++desc :Beam position of the photon Beam determined by the GMD (BDA, x=horizontal)
++units : mm
++
++{{code language="none"}}/FL1/Photon Diagnostic/GMD/Beam position/position BDA vertical{{/code}}
++//always saved (PBD)//
++DOOCS prop : {{code language="none"}}FLASH.FEL/XGM.POSMON/FL1.BDA/IY.POS{{/code}}
++DAQ channel: {{code language="none"}}FLASH.FEL/XGM.POSMON/FL1.BDA/IY.POS{{/code}}
++desc :Beam position of the photon Beam determined by the GMD (BDA, y=vertical)
++units : mm
++
++{{code language="none"}}/FL1/Photon Diagnostic/GMD/Beam position/position tunnel horizontal{{/code}}
++//always saved (PBD)//
++DOOCS prop : {{code language="none"}}FLASH.FEL/XGM.POSMON/FL1.TUNNEL/IX.POS{{/code}}
++DAQ channel: {{code language="none"}}FLASH.FEL/XGM.POSMON/FL1.TUNNEL/IX.POS{{/code}}
++desc :Beam position of the photon Beam determined by the GMD (TUNNEL, x=horizontal)
++units : mm
++
++{{code language="none"}}/FL1/Photon Diagnostic/GMD/Beam position/position tunnel vertical{{/code}}
++//always saved (PBD)//
++DOOCS prop : {{code language="none"}}FLASH.FEL/XGM.POSMON/FL1.TUNNEL/IY.POS{{/code}}
++DAQ channel: {{code language="none"}}FLASH.FEL/XGM.POSMON/FL1.TUNNEL/IY.POS{{/code}}
++desc :Beam position of the photon Beam determined by the GMD (TUNNEL, y=vertical)
++units : mm
++
++
++==== Spectrometer (FLASH1) ====
++
++{{code language="none"}}/FL1/Photon Diagnostic/Wavelength/Tunnelspectrometer/wavelength{{/code}}
++_always saved (when Spectrum is measured !!) (PBD) _
++DOOCS prop : {{code language="none"}}TTF2.EXP/PHOTONWL.ML/WAVE_LENGTH/VAL.TD{{/code}}
++DAQ channel: {{code language="none"}}PBD.PHOTONWL.ML/WAVE_LENGTH{{/code}}
++desc : XUV Spectrum measured with the "tunnel spectrometer"
++units :
++
++{{code language="none"}}/FL1/Photon Diagnostic/Wavelength/Tunnelspectrometer/wavelength start value{{/code}}
++_always saved (when Spectrum is measured !!) (PBD) _
++DOOCS prop : {{code language="none"}}TTF2.EXP/PBD.PHOTONWL.ML/BSTART/VAL{{/code}}
++DAQ channel: {{code language="none"}}TTF2.EXP/PBD.PHOTONWL.ML/BSTART/VAL{{/code}}
++desc : start value (in nm) for the wavelength axis of the XUV Spectrum measured with the "tunnel spectrometer"
++units : nm
++
++{{code language="none"}}/FL1/Photon Diagnostic/Wavelength/Tunnelspectrometer/wavelength increment{{/code}}
++_always saved (when Spectrum is measured !!) (PBD) _
++DOOCS prop : ==
++DAQ channel: ==
++desc : increment value (in nm) for each pixel for the wavelength axis of the XUV Spectrum measured with the "tunnel spectrometer"
++units : nm
++
++{{code language="none"}}/FL1/Photon Diagnostic/Wavelength/PG2 spectrometer/photon energy{{/code}}
++//saved on DEMAND (PBD spectrometer stream)//
++DOOCS prop : ==
++DAQ channel: {{code language="none"}}PBD.PHOTONEN.ML/PHOTON_ENERGY{{/code}}
++desc : XUV Spectrum in eV measured with the "PG2 spectrometer"
++units :
++
++{{code language="none"}}/FL1/Photon Diagnostic/Wavelength/PG2 spectrometer/photon energy start value{{/code}}
++//saved on DEMAND (PBD spectrometer stream)//
++DOOCS prop : ==
++DAQ channel: ==
++desc : start value (in eV) for the wavelength axis of the XUV Spectrum measured with the "PG2 spectrometer"
++units : eV
++
++{{code language="none"}}/FL1/Photon Diagnostic/Wavelength/PG2 spectrometer/photon energy increment{{/code}}
++//saved on DEMAND (PBD spectrometer stream)//
++DOOCS prop : ==
++DAQ channel: ==
++desc : increment value (in eV) for each pixel for the wavelength axis of the XUV Spectrum measured with the "PG spectrometer"
++units : eV
++
++{{code language="none"}}/FL1/Photon Diagnostic/Wavelength/PG2 spectrometer/photon wavelength{{/code}}
++//saved on DEMAND (PBD spectrometer stream)//
++DOOCS prop : ==
++DAQ channel: {{code language="none"}}PHOTONEN.ML/PHOTON_WAVE_LEN{{/code}}
++desc : XUV Spectrum in nm measured with the "PG2 spectrometer"
++units :
++
++{{code language="none"}}/FL1/Photon Diagnostic/Wavelength/PG2 spectrometer/photon wavelength increment{{/code}}
++//saved on DEMAND (PBD spectrometer stream)//
++DOOCS prop : ==
++DAQ channel: ==
++desc : start value (in nm) for the wavelength axis of the XUV Spectrum measured with the "PG2 spectrometer"
++units : nm
++
++{{code language="none"}}/FL1/Photon Diagnostic/Wavelength/PG2 spectrometer/photon wavelength start value{{/code}}
++//saved on DEMAND (PBD spectrometer stream)//
++DOOCS prop : ==
++DAQ channel: ==
++desc : increment value (in nm) for each pixel for the wavelength axis of the XUV Spectrum measured with the "PG spectrometer"
++units : nm
++
++[[Contents>>doc:||anchor="Contents"]]
++
++==== Electron Beam properties (FLASH1) ====
++
++===== bunch charge =====
++
++{{code language="none"}}/FL1/Electron Diagnostic/Bunch charge/after undulator{{/code}}
++//always saved (PBD)//
++DOOCS prop : {{code language="none"}}FLASH.DIAG/TOROID.ML/12EXP/CHARGE.FLASH1{{/code}}
++DAQ channel: {{code language="none"}}FLASH.DIAG/TOROID/12EXP{{/code}}
++desc: electron bunch charge (FLASH1)
++units: nC
++
++=====
++arrival time (BAM) =====
++
++{{info title="BAM information: updates 2022 (status 2025)"}}
++* see: [[Info collection about the BAMs and how to use the BAM data>>doc:FS-FLASH USER tmp.jddd-linked help pages.Info collection for the BAM.WebHome||shape="rect"]]
++* The data format of the BAM has been completely altered in the 2022 shutdown
++* 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 ...
++* THIS is now different. There are new parameters saving only the arrival times for pulses that go to FL1 and to FL2 (in detail: first time slot of the accelerator and second)
++* There has been also a renaming  (and relocation) of the BAMs.
++** acc:  4DBC3 → FL0.DBC2
++** FL1: 1SFELC →  FL1.SFELC
++** FL2: FL2XTDS → (% style="color:#172b4d" %)FL2.SEED5
++* for more Info: [[LINK to detailed infos from MSK>>doc:SDiag.How-to articles.BAM Data Structure.WebHome||shape="rect"]]
++* [[Link a collection of papers related to the BAM and the analysis of pump-probe experiments>>doc:FS-FLASH USER tmp.Additional helpful things1.FLASH beamlines and instruments references.WebHome]]
++* a recent  [[talk about the working principle of the BAM>>attach:BAM-basics and outlook-2018_DESY-template_16-9Format.pdf]]
++{{/info}}
++
++{{expand title="Discontinued BAM format (used until end 2021)"}}
++(% style="color:#000000" %)**Discontinued BAM data recording **
++
++{{code language="none"}}/FL1/Electron Diagnostic/BAM/4DBC3/electron bunch arrival time (low charge){{/code}}
++//always saved (PBD)//
++DOOCS prop : {{code language="none"}}FLASH.SDIAG/BAM/4DBC3/LOW_CHARGE_ARRIVAL_TIME{{/code}}
++DAQ channel: {{code language="none"}}FLASH.SDIAG/BAM.DAQ/4DBC3.LOW_CHARGE_ARRIVAL_TIME{{/code}}
++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).
++units: ps (bigger numbers indicate later arrivaltime of the electrons)
++
++
++{{code language="none"}}/FL1/Electron Diagnostic/BAM/1SFELC/electron bunch arrival time (low charge){{/code}}
++//always saved (PBD)//
++DOOCS prop : {{code language="none"}}FLASH.SDIAG/BAM/1SFELC/LOW_CHARGE_ARRIVAL_TIME{{/code}}
++DAQ channel: {{code language="none"}}FLASH.SDIAG/BAM.DAQ/1SFELC.LOW_CHARGE_ARRIVAL_TIME{{/code}}
++desc: Electron bunch arrival time measured with the BAM  before the undulator (pulse resolved data). This one was newly installed in 2020.
++units: ps (bigger numbers indicate later arrival time of the electrons)
++{{/expand}}
++
++====== **BAM FL0.DBC2**{{code language="none"}}{{/code}} ======
++
++(% style="color:#ff6600" %)**DBC2**/electron bunch arrival time   (HDF5 name not yet implemented - see zraw)(%%)
++//always saved (PBD)//
++{{code language="none"}}/FL1/Electron Diagnostic/BAM/ {{/code}}DOOCS prop : FLASH.SDIAG/BAM/**FL0.DBC2**/ARRIVAL_TIME.ABSOLUTE.SA1.COMP
++DAQ (% style="color:#000000" %)channel: FLASH.SDIAG/BAM/**FL0.DBC2**/ARRIVAL_TIME.ABSOLUTE.SA1.COMP (%%)
++desc: Electron bunch arrival time measured with the BAM inside the accelerator (after bunch compressor 2). The property contains only the arrival time of the bunches sent to FL1 (e.g. if there are 30 bunches in FL1 the first 30 values are the arrival time the remaining numbers  still may have arbitrary numbers looking like a signal which they are not ). These are the same values as the "raw" data below - just "cleaned". The values show a very good correlation to the arrival time  of the XUV pulses in the experiment (see help).
++
++units: fs (bigger numbers (typically) indicate later arrival times of the electrons).
++
++
  (% style="color:#ff6600" %)DBC2/electron bunch arrival time (raw)  (HDF5 name not yet implemented - see zraw){{code language="none"}}/FL1/Electron Diagnostic/BAM/{{/code}}(%%)
  //always saved (PBD)//
  DOOCS prop : FLASH.SDIAG/BAM/FL0.DBC2/ARRIVAL_TIME.ABSOLUTE
@@ -466,8 +466,8 @@
  //always saved (PBD)//
  (% style="color:#172b4d" %)**FL1.SFELC**(%%)
--(% style="color:#000000" %)channel: FLASH.SDIAG/BAM/(% style="color:#172b4d" %)FL1.SFELC(% style="color:#000000" %)/ARRIVAL_TIME.ABSOLUTE.SA1.COMP(%%)
--(% style="color:#000000" %){{code language="none"}} DOOCS prop : FLASH.SDIAG/BAM//ARRIVAL_TIME.ABSOLUTE.SA1.COMPDAQ {{/code}}(% style="letter-spacing:0.0px" %)desc: Electron bunch arrival time measured  with the BAM  before the undulator (pulse resolved data). This one was newly installed in 2020.. The property contains only the arrival time of the bunches sent to FL1 (e.g. if there are 30 bunches in FL1 the first 30 values are the arrival time the remaining numbers still may have arbitrary numbers looking like a signal which they are not). These are the same values as the "raw" data below - just "cleaned". The values show a very good correlation to the arrival time  of the XUV pulses in the experiment (see help).
++(% style="color:#000000" %)channel: FLASH.SDIAG/BAM/(% style="color:#172b4d" %)FL1.SFELC(% style="color:#000000" %)/ARRIVAL_TIME.ABSOLUTE.SA1.COMP
++{{code language="none"}} DOOCS prop : FLASH.SDIAG/BAM//ARRIVAL_TIME.ABSOLUTE.SA1.COMPDAQ {{/code}}(% style="letter-spacing:0.0px" %)desc: Electron bunch arrival time measured  with the BAM  before the undulator (pulse resolved data). This one was newly installed in 2020.. The property contains only the arrival time of the bunches sent to FL1 (e.g. if there are 30 bunches in FL1 the first 30 values are the arrival time the remaining numbers still may have arbitrary numbers looking like a signal which they are not). These are the same values as the "raw" data below - just "cleaned". The values show a very good correlation to the arrival time  of the XUV pulses in the experiment (see help).
  units: fs (bigger numbers (typically) indicate later arrival times of the electrons).
@@ -545,23 +545,20 @@
  [[Contents>>doc:||anchor="Contents"]]
--====   ====
--
--
  ==== Timing information, rep rate etc.  (FLASH1) ====
  ===== bunch repetition rate =====
--{{code language="none"}}/Timing/repetition rate{{/code}}
++{{code language="none"}}/FL1/Timing/repetition rate{{/code}}
  //always saved (PBD)//
  DOOCS prop : {{code language="none"}}FLASH.DIAG/TIMER/FLASHCPUTIME1.0/REP_RATE_KHZ.1{{/code}}
--DAQ channel: {{code language="none"}}FLASH.DIAG/TIMER/FLASHCPUTIME1.0/REP_RATE_KHZ.1{{/code}}
++DAQ channel: {{code language="none"}}TTF2.UTIL/LASER.CONTROL/GUN/PULSE_FREQ{{/code}}
  desc: repetition rate of the bunches / pulses within the burst (FLASH1)
  units: kHz
  ===== set number of pulses =====
--(% style="color:#ff6600" %)(HDF5 name not yet implemented - see zraw)(% style="color:#ff0000" %){{code language="none"}}/Timing/set number of bunches {{/code}}(%%)
++(% style="color:#ff6600" %)(HDF5 name not yet implemented - see zraw)(% style="color:#ff0000" %){{code language="none"}}/FL1/Timing/set number of bunches {{/code}}(%%)
  //always saved (PBD)//
  DOOCS prop : {{code language="none"}}FLASH.DIAG/TIMINGINFO/TIME1.BUNCH_FIRST_INDEX.1 [4th number]{{/code}}
  DAQ channel: {{code language="none"}}FLASH.DIAG/TIMINGINFO/TIME1.BUNCH_FIRST_INDEX.1 [4th number]{{/code}}
@@ -620,8 +620,8 @@
  {{/expand}}
++[[Contents>>doc:||anchor="Contents"]]
--
  ==== Pump Probe Laser (FLASH1) ====
  **PIGLET (PG laser)**
@@ -737,9 +737,10 @@
  * {{code language="none"}}number of samples{{/code}}: total number of samples recorded for each 10 Hz trigger
  [[Contents>>doc:||anchor="Contents"]]
--{{/expand}}
++
++
  === FLASH2 ===
  There is analog to FLASH1 a permanently running "PhotonDagnostic DAQ FLASH2" (PBD2) and 2 User DAQs
@@ -747,6 +747,7 @@
  ==== Beamline info (FLASH2) ====
  {{code language="none"}}/FL2/Beamlines/Attenuator/pressure  {{/code}}
++(% style="color:#000000" %)//always saved (PBD2)// (%%)
  (% style="color:#000000" %)DOOCS prop : {{code language="none"}}FLASH.FEL/ATT.GAS_DOSING/FL2.HALL/PRESSURE{{/code}} (%%)
  (% style="color:#000000" %)DAQ channel:  {{code language="none"}}FLASH.FEL/ATT.GAS_DOSING/FL2.HALL/PRESSURE{{/code}} (%%)
  (% style="color:#000000" %)desc: set pressure in the gas attenuator (%%)
@@ -753,6 +753,7 @@
  (% style="color:#000000" %)units: mbar
  {{code language="none"}}/FL2/Beamlines/FL20/Shutter/open{{/code}}
++//always saved (PBD2)//
  DOOCS prop : {{code language="none"}}FLASH.FEL/ADC.SIS.FL2FS/FL20.SHUTTER/CH00.TD{{/code}}
  DAQ channel: {{code language="none"}}FLASH.FEL/ADC.SIS.FL2FS/FL20.SHUTTER{{/code}}
  desc: BL Beamline Fast shutter state: 1 is open, 0 is closed ( for technical reasons there are 100 vales of this state saved ...)
@@ -760,6 +760,7 @@
  {{code language="none"}}/FL2/Beamlines/Filter wheel/position wheel 1{{/code}}
++//always saved (PBD2)//
  DOOCS prop : {{code language="none"}}FLASH.FEL/FL20H.PH.MOTOR/MOTOR1.MOT3/FPOS{{/code}}
  DAQ channel: FLASH.FEL/FL20H.PH.MOTOR/MOTOR1.MOT3/FPOS
  desc: Position of the BL filter wheel 1 - to correlate with the filter material please look **[[here>>doc:FS-FLASH USER tmp.jddd-linked help pages.Filter-Units.Filter wheels in FLASH1 and FLASH2.WebHome]]**
@@ -766,6 +766,7 @@
  units: degree
  /FL2/Beamlines/Filter wheel/position wheel 2
++always saved (PBD2)
  DOOCS prop : {{code language="none"}}FLASH.FEL/FL20H.PH.MOTOR/MOTOR2.MOT3/FPOS{{/code}}
  DAQ channel: {{code language="none"}}FLASH.FEL/FL20H.PH.MOTOR/MOTOR2.MOT3/FPOS{{/code}}
  desc: Position of the BL filter wheel 2 - to correlate with the filter material please look [[here>>doc:FS-FLASH USER tmp.jddd-linked help pages.Filter-Units.Filter wheels in FLASH1 and FLASH2.WebHome]]
@@ -781,6 +781,7 @@
  ==== Photon Diagnostics SASE ([[XGMD>>url:http://photon-science.desy.de/facilities/flash/photon_diagnostics/gmd_intensity_and_position/index_eng.html||shape="rect"]] - FLASH2) ====
  {{code language="none"}}/FL2/Photon Diagnostic/GMD/Average energy/energy tunnel{{/code}}
++//always saved (PBD2)//
  DOOCS prop : {{code language="none"}}FLASH.FEL/XGM.PHOTONFLUX/FL2.TUNNEL/PHOTONFLUX.UJ{{/code}}
  DAQ channel:{{code language="none"}} FLASH.FEL/XGM.PHOTONFLUX/FL2.TUNNEL/PHOTONFLUX.UJ{{/code}}
  desc : calibrated average ( ~~ 20 sec averaging time ) SASE Energy/pulse measured in the TUNNEL before the attenuator (ion current)
@@ -788,6 +788,7 @@
  {{code language="none"}}/FL2/Photon Diagnostic/GMD/Pulse resolved energy/energy tunnel{{/code}}
++//always saved (PBD2)//
  DOOCS prop : {{code language="none"}}FLASH.FEL/XGM.INTENSITY/FL2.TUNNEL/INTENSITY.TD{{/code}}
  DAQ channel: {{code language="none"}}FLASH.FEL/XGM.INTENSITY/FL2.TUNNEL/INTENSITY.TD{{/code}}
  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)
@@ -822,6 +822,7 @@
  {{code language="none"}}/FL2/Photon Diagnostic/GMD/Average Beam position/position tunnel horizontal{{/code}}
++//always saved (PBD2)//
  DOOCS prop : {{code language="none"}}FLASH.FEL/XGM.POSMON/FL2.TUNNEL/IX.POS{{/code}}
  DAQ channel: {{code language="none"}}FLASH.FEL/XGM.POSMON/FL2.TUNNEL/IX.POS{{/code}}
  desc : the Average ( ~~ 20 sec averaging time ) Beam position of the photon Beam determined by the GMD (tunnel, x=horizontal)
@@ -829,6 +829,7 @@
  {{code language="none"}}/FL2/Photon Diagnostic/GMD/Average Beam position/position tunnel vertical{{/code}}
++//always saved (PBD2)//
  DOOCS prop : {{code language="none"}}FLASH.FEL/XGM.POSMON/FL2.TUNNEL/IY.POS{{/code}}
  DAQ channel: {{code language="none"}}FLASH.FEL/XGM.POSMON/FL2.TUNNEL/IY.POS{{/code}}
  desc : the Average ( ~~ 20 sec averaging time ) Beam position of the photon Beam determined by the GMD (tunnel, x=horizontal)
@@ -836,6 +836,7 @@
  /FL2/Photon Diagnostic/GMD/Pulse resolved beam position/position tunnel x
++always saved (PBD2)
  DOOCS prop : FLASH.FEL/XGM.BPM/FL2.HALL/X.TD
  DAQ channel: FLASH.FEL/XGM.BPM/FL2.HALL:2
  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 ...)
@@ -855,6 +855,7 @@
  {{code language="none"}}/FL2/Photon Diagnostic/Wavelength/OPIS tunnel/Processed/mean photon energy{{/code}}
++// saved opon request (PBD2)//
  DOOCS prop : {{code language="none"}}FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL042{{/code}}
  DAQ channel:{{code language="none"}} FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL042{{/code}}
  desc : mean photon energy ( ~~ 1 sec averaging time ) measured in the TUNNEL for a specific bunch out of the bunch train (via photoelectron spectroscopy)
@@ -862,6 +862,7 @@
  {{code language="none"}}/FL2/Photon Diagnostic/Wavelength/OPIS tunnel/Processed/mean wavelength{{/code}}
++// saved opon request (PBD2)//
  DOOCS prop : {{code language="none"}}FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL040{{/code}}
  DAQ channel:{{code language="none"}} FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL040{{/code}}
  desc : mean wavelength ( ~~ 1 sec averaging time ) measured in the TUNNEL for a specific bunch out of the bunch train (via photoelectron spectroscopy)
@@ -869,28 +869,12 @@
  {{code language="none"}}/FL2/Photon Diagnostic/Wavelength/OPIS tunnel/Processed/number of analyzed bunch        (in older version this can be found in OPIS tunnel/Expert stuff/General operation parameters/){{/code}}
++// saved opon request (PBD2)//
  DOOCS prop : {{code language="none"}}FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL060{{/code}}
  DAQ channel:{{code language="none"}} FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL060{{/code}}
  desc : The bunch number of the bunch used for the wavelength calculation
  units :
--{{expand expanded="false" title="More detailed info on OPIS properties"}}
--FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL370,'%','relative width of photoline in percent of the FEL photon energy ROI1, rising flank'
--FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL375,'%','relative width of photoline in percent of the FEL photon energy ROI1, tailing flank'
--FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL470,'%','relative width of photoline in percent of the FEL photon energy ROI1, mean'
--FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL371,'%','relative width of photoline in percent of the FEL photon energy  ROI2, rising flank'
--FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL376,'%','relative width of photoline in percent of the FEL photon energy  ROI2, tailing flank'
--FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL471,'%','relative width of photoline in percent of the FEL photon energy  ROI2, mean'
--FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL372,'%','relative width of photoline in percent of the FEL photon energy  ROI3, rising flank'
--FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL377,'%','relative width of photoline in percent of the FEL photon energy  ROI3, tailing flank'
--FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL472,'%','relative width of photoline in percent of the FEL photon energy  ROI3, mean'
--FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL373,'%','relative width of photoline in percent of the FEL photon energy  ROI4, rising flank'
--FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL378,'%','relative width of photoline in percent of the FEL photon energy  ROI4, tailing flank'
--FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL473,'%','relative width of photoline in percent of the FEL photon energy  ROI4, mean'
--FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL374,'%','relative width of photoline in percent of the FEL photon energy  ROI5, rising flank'
--FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL379,'%','relative width of photoline in percent of the FEL photon energy  ROI5, tailing flank'
--FLASH.UTIL/STORE/FL2.TUNNEL.OPIS/VAL474,'%','relative width of photoline in percent of the FEL photon energy  ROI5, mean'
--{{/expand}}
  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"]])
@@ -904,6 +904,7 @@
  ===== bunch charge =====
  {{code language="none"}}/FL2/Electron Diagnostic/Bunch charge/after undulator{{/code}}
++//always saved (PBD2)//
  DOOCS prop : {{code language="none"}}FLASH.DIAG/PBD2.TOROID.ML/9FL2BURN/CHARGE.FLASH2{{/code}}
  DAQ channel: {{code language="none"}}FLASH.DIAG/PBD2.TOROID.ML/9FL2BURN/CHARGE.FLASH2{{/code}}
  desc: electron bunch charge FLASH2 (average value for each bunchtrain).
@@ -913,6 +913,7 @@
  ===== electron bunch energy =====
  {{code language="none"}}/FL2/Electron Diagnostic/Electron energy/energy of first bunch/behind undulators{{/code}}
++//always saved (PBD2)//
  DOOCS prop : {{code language="none"}}FLASH.DIAG/BEAM_ENERGY_MEASUREMENT/FL2XTDS/ENERGY.FLASH2{{/code}}
  DAQ channel: (% style="color:#5e6c84" %)TTF2.DAQ/PBD2.BEAM.ENERGY.MEAS.ML.COPY/FL2XTDS.ENERGY.FLASH2{{code language="none"}}{{/code}}(%%)
  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:#5e6c84" %)extraction and septum  in the beginning of FLASH2
@@ -923,19 +923,21 @@
  (% style="color: rgb(94, 108, 132); font-weight: 600; letter-spacing: 0px;" %)
  ===== undulator settings =====
--{{code language="none"}}/FL2/Electron Diagnostic/Undulator setting/set wavelength 1{{/code}}
--DOOCS prop : {{code language="none"}}FLASH.FEL/FL2.WAVELENGTHCONTROL/FLASH2.COLOR1/WAVELENGTH{{/code}}
--DAQ channel:  {{code language="none"}}FLASH.FEL/FL2.WAVELENGTHCONTROL/FLASH2.COLOR1/WAVELENGTH{{/code}}
--desc: Set value for the anticipated wavelength 1 . This parameter is used to set the undulator gap. It may however deviate from the actual wavelength by several % ... For 2 color operation there is also  the same parameter for COLOR 2
++{{code language="none"}}/FL2/Electron Diagnostic/Undulator setting/set wavelength{{/code}}
++//always saved (PBD2)//
++DOOCS prop : {{code language="none"}}TTF2.FEEDBACK/FL2.WAVELENGTHCONTROL/FLASH2/WAVELENGTH{{/code}}
++DAQ channel:  {{code language="none"}}TTF2.FEEDBACK/FL2.WAVELENGTHCONTROL/FLASH2/WAVELENGTH{{/code}}
++desc: Set value for the anticipated wavelength . This parameter is used to set the undulator gap. It may however deviate from the actual wavelength by several % ...
  units: nm
--{{code language="none"}}/FL2/Electron Diagnostic/Undulator setting/SASE13 gap{{/code}}
--DOOCS prop : {{code language="none"}}FLASH.UTIL/FL2.UND.MOTOR/FL2SASE13/GAP{{/code}}
--DAQ channel:  {{code language="none"}}FLASH.UTIL/FL2.UND.MOTOR/FL2SASE13/GAP{{/code}}
--desc: gap value of the undulators. This can be used to follow up how many undulators were closed and if there was a taper.
++{{code language="none"}}/FL2/Electron Diagnostic/Undulator setting/SASE14 gap{{/code}}
++//always saved (PBD2)//
++DOOCS prop : {{code language="none"}}FLASH.UTIL/FL2.UND.MOTOR/FL2SASE14/GAP{{/code}}
++DAQ channel:  {{code language="none"}}FLASH.UTIL/FL2.UND.MOTOR/FL2SASE14/GAP{{/code}}
++desc: gap value of the undulators. This can be used to follow up how many undulators were closed and if there was a taper
  units: mm
--The gap values are saved for all 12 undulators (Nr 2 to 13). Undulator 13 is the one closest to the experimental hall.
++The gap values are saved for all 12 undulators (Nr 3 to 14). Undulator 14 is the one closest to the experimental hall.
  =====
  arrival time (BAM) =====
@@ -1219,7 +1219,7 @@
  {{view-file att--filename="FSLADAQ-DAQParameterlistFL24-2.pdf"}}{{/view-file}}
--internal link to parameter list: [[FS-LA DAQ - XWiki>>url:https://xwiki.desy.de/xwiki/bin/view/FSLADAQ/]]
++
  {{/info}}
  {{expand title="Laser parameters used until 2023"}}
@@ -1694,3 +1694,8 @@
  )))
  [[Contents>>doc:||anchor="Contents"]]
++
++
++{{/layout-cell}}
++{{/layout-section}}
++{{/layout}}

image.png

Author

...	...	@@ -1,1 +1,0 @@
1		-XWiki.sndueste

Size

...	...	@@ -1,1 +1,0 @@
1		-1.1 MB

Content

Changes for page The FLASH HDF5 structure

Summary

Details

Applications

Navigation