Wiki source code of Info collection for the BAM
Version 8.1 by sndueste on 2020-06-10 15:23
Show last authors
| author | version | line-number | content |
|---|---|---|---|
| 1 | === Some basic stuff: === | ||
| 2 | |||
| 3 | * The relevant data is the arrival time FLASH.SDIAG/BAM/4DBC3/LOW_CHARGE_ARRIVAL_TIME | ||
| 4 | * Besides the arrival time from FLASH1 there is also the FLASH2/3 electron arrival time saved. The BAM data is saved for the complete RF pulse. First bunches are from FLASH1 then there is a gap for switching and then there is a second part for FLASH2 (starting at the FLASH2 start time (recorded in DAQ as {{code language="none"}}/FL2/Timing/start time flash2{{/code}})) | ||
| 5 | * There are LOW and HIGH charge channels. For now the LOW_CHARGE Channel is the relevant one. | ||
| 6 | * Bigger numbers indicate later arrival time of the electrons | ||
| 7 | * The arrival time should be within -20 ps and +20 ps - otherwise there might be a problem ... | ||
| 8 | |||
| 9 | === Data structure === | ||
| 10 | |||
| 11 | (% style="color: rgb(0,0,0);" %)The details about the functionality and the data structure can be found on the page: (%%)**[[ BAM Data Structure>>doc:SDiagPublic.BAM Data Structure]]** | ||
| 12 | |||
| 13 | \\ | ||
| 14 | |||
| 15 | = General information for the data analysis of pump-probe experiments = | ||
| 16 | |||
| 17 | \\ | ||
| 18 | |||
| 19 | please have a close look to the publication: | ||
| 20 | |||
| 21 | Evgeny Savelyev, et al, //Jitter-Correction for IR/UV-XUV Pump-Probe Experiments at the FLASH Free-Electron Laser//, | ||
| 22 | New J. Phys. **19**, 043009 (2017), [[https:~~/~~/doi.org/10.1088/1367-2630/aa652d>>url:https://doi.org/10.1088/1367-2630/aa652d||shape="rect"]] | ||
| 23 | |||
| 24 | describing in detail the usage of BAM, streak camera and delay line data in order to get the actual time axis as reliable as possible. | ||
| 25 | |||
| 26 | \\ | ||
| 27 | |||
| 28 | Here is a summary of the ideas: | ||
| 29 | |||
| 30 | == Streak camera info == | ||
| 31 | |||
| 32 | * the streak camera measures the delay between optical (amplified) laser and FEL (dipole radiation). - not in respect to the master clock ! | ||
| 33 | * streak camera ONLY delivers data which is averaged over several 10 seconds. There is NO shot to shot info. | ||
| 34 | * a larger value of the streak camera delay (typically) indicates that the optical laser comes later than the FEL (or FEL earlier than the laser ...) | ||
| 35 | |||
| 36 | \\ | ||
| 37 | |||
| 38 | \\ | ||
| 39 | |||
| 40 | {{info title="Correction of pump-probe delay"}} | ||
| 41 | * BAM measurement: difference between electrons and timing system | ||
| 42 | ** usually the BAM signal has to be added to the delay ... | ||
| 43 | ** it is the best to test addition/subtraction and check the results on a step function (more/less sharp) - if there is no change of the data with + and - there is anyway something wrong. please contact your local contact for more information / help | ||
| 44 | * Streak camera: difference between electrons and optical laser | ||
| 45 | ** it is a slow signal and should only be used as a rolling average over multiple minutes | ||
| 46 | ** if you see a drift in the streak camera which you do not see in the BAM it is resulting from the optical laser | ||
| 47 | ** if this (BAM - streak camera signal) is significant e.g. 200 fs over 1 h, it means the drift compensation was probably off and it should be compensated | ||
| 48 | ** addition/subtraction is dependent on the setup and have to be checked | ||
| 49 | {{/info}} |