Difference between revisions of "KLF beamline meeting - July 26, 2024"

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(Created page with "= Agenda = *; Announcements *; FSD system for electron beam excursions (Pavel, Hovanes) *; Impact of the beam bleedthrough *; CPS & KPT design progress (Tim) *; Do we...")
 
 
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*; Announcements  
 
*; Announcements  
  
*; FSD system for electron beam excursions (Pavel, Hovanes)
+
*; [[media:cps_simulations_july24_2024.pptx | Updates on CPS simulations]] (Pavel)
  
*; Impact of the beam bleedthrough  
+
*; [[media:bleedthrough_07_26_2024.pdf | Potential impact of the beam bleedthrough]]  (Hovanes)
  
*; CPS & KPT design progress (Tim)
+
*; CPS & KPT design progress (Josh)
 +
**; Is the latest collimator cave/KPT layout approved so we can begin procurements?
 +
 
 +
*; KFM update (Mikhail)
  
 
*; Do we need photon beam in the hall during KLF? (Sean, Mikhail, Ig)
 
*; Do we need photon beam in the hall during KLF? (Sean, Mikhail, Ig)
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= Minutes =
 
= Minutes =
  
Present:   
+
Present: Igor, Hovanes, Josh, Eugene, Pavel, Edy, Beni, Marshall, Vitaly, Sean, Moskov
 +
 
 +
----
 +
 
 +
 
 +
* Pavel showed is recent simulations to optimize the beam displacement monitor.
 +
* Current conceptual design consists of two main components sitting just upstream of CPS entrance:
 +
*# a copper ring with 0.5mm thickness in Z, and IR=4.5mm and OR=5.5mm
 +
*# a set of four PMT-based counters around the beam pipe with a glass puck mounted on them for Cerenkov light production, plus some shielding around them.
 +
* Pavel simulated beam offsets of 0mm, 0.5mm, 1.0mm and 2.0mm. The setup show pretty good sensitivity to 1mm beam shifts: the counter in the direction of the shift see x5 increase in the counting rates.
 +
* A narrow beam (FWHM=2.0mm insted of FWHM=2.8mm) reduces the counting rate, and also would reduce the sensitivity of these device to the beam excursions. Therefore, beam width needs to be monitored independently using regular wire scans.
 +
* Vitaly asked if this was just position shift or the angular shift as well. Pavel's answer was that he simulated parallel shifts only. Hovanes commented that angular changes are supposed to be monitored by the active collimator in front of KPT which would also trip the FSD if some position limit is exceeded.
 +
* Radiation dose rates created by this setup with nominal beam conditions are similar to what is present at the sides of CPS (10 rad/hr).
 +
* Eugene asked if the magnetic fields present in this area would affect sensitivity of the detector if the main source of the signal are low energy electrons. This has not been investigated.
 +
* Hovanes pointed out that the closest magnet is the CPS magnet, and next closest magnet is the GlueX quad just upstream of the tagger magnet.
 +
 
 +
 
 +
----
 +
 
 +
 
 +
* Hovanes showed his calculations in an attempt to estimate the impact of the bleedthrough present in the out-of-time bunches coming every 4ns. He assumed that at 5μA beam current there will be 5nA out-of-time beam current. Note, that during GlueX we see about 2-3nA bleedthrough when running at 350nA. He did not do Monte-Carlo simulations, instead he just calculated these analytically assuming momentum spectrum from Ilya's simulations.
 +
* The calculations showed that these bunches separated by 4ns would show up low reconstructed (<2 GeV) momentum and low reconstructed W (<2.5GeV). Therefore, the event selection should be used to get rid of the background that could produce false bumps in this range of the W-spectrum.
 +
* Hovanes suggested that it would be good if the physics channels that are being analyzed come up with an estimated of the bleedthrough that they can tolerate without impacting physics conclusions. This would entail simulating and reconstructing events from the physics channel interest as well as from the channels that can populate the W-range if produce by the bleed-through kaons.
 +
* There was suggestion from Eugene how the K+ momentum cuts in the event selections could reduce the background from out-of-time bunches.
 +
* Moskov added that they (ODU) are working on the event selection for the K+n channel, and that other channels will need to identify events before plotting W-spectra.
 +
* We had to cut this discussion short to cover the remaining items on the agenda.
 +
 
 +
 
 +
----
 +
 
 +
 
 +
* Josh reported that the CPS magnet design is nearly complete and the PR will be issued in a week or so.
 +
* KPT engineering design is complete (assuming there is no need for photon beam in the hall). Hovanes asked collaboration leadership to take a look at the final design before large procurements start. Igor agreed to take a look at the design and approve it or provide comments and suggestions within a week. Igor will contact Josh for details.
 +
* Eugene pointed out that changes to the KPT assembly needed for providing photon beam will not affect the procurement of some major items like beryllium, tungsten block, or the lead.
 +
* Josh said that the deadline for PR submission for this fiscal year is close, and we should not delay until next meeting because the timeline will be too tight. (added by Hovanes later: August 19, 2024 for purchases below $250K).
 +
 
  
 
----
 
----
 +
 +
 +
* Since the meeting went longer than 1 hour, Sean had to leave. Therefore, we did not have a fruitful discussion on the topic of photon beam in the hall. We just had some exchange of opinions. This will be revisited at the software meetings and at the next beamline meeting.
 +
 +
 +
----
 +
 +
 +
* Next meeting will be held in two weeks.

Latest revision as of 15:54, 26 July 2024

Agenda

  • Announcements
  • CPS & KPT design progress (Josh)
    • Is the latest collimator cave/KPT layout approved so we can begin procurements?
  • KFM update (Mikhail)
  • Do we need photon beam in the hall during KLF? (Sean, Mikhail, Ig)
  • Any other business

Minutes

Present: Igor, Hovanes, Josh, Eugene, Pavel, Edy, Beni, Marshall, Vitaly, Sean, Moskov



  • Pavel showed is recent simulations to optimize the beam displacement monitor.
  • Current conceptual design consists of two main components sitting just upstream of CPS entrance:
    1. a copper ring with 0.5mm thickness in Z, and IR=4.5mm and OR=5.5mm
    2. a set of four PMT-based counters around the beam pipe with a glass puck mounted on them for Cerenkov light production, plus some shielding around them.
  • Pavel simulated beam offsets of 0mm, 0.5mm, 1.0mm and 2.0mm. The setup show pretty good sensitivity to 1mm beam shifts: the counter in the direction of the shift see x5 increase in the counting rates.
  • A narrow beam (FWHM=2.0mm insted of FWHM=2.8mm) reduces the counting rate, and also would reduce the sensitivity of these device to the beam excursions. Therefore, beam width needs to be monitored independently using regular wire scans.
  • Vitaly asked if this was just position shift or the angular shift as well. Pavel's answer was that he simulated parallel shifts only. Hovanes commented that angular changes are supposed to be monitored by the active collimator in front of KPT which would also trip the FSD if some position limit is exceeded.
  • Radiation dose rates created by this setup with nominal beam conditions are similar to what is present at the sides of CPS (10 rad/hr).
  • Eugene asked if the magnetic fields present in this area would affect sensitivity of the detector if the main source of the signal are low energy electrons. This has not been investigated.
  • Hovanes pointed out that the closest magnet is the CPS magnet, and next closest magnet is the GlueX quad just upstream of the tagger magnet.




  • Hovanes showed his calculations in an attempt to estimate the impact of the bleedthrough present in the out-of-time bunches coming every 4ns. He assumed that at 5μA beam current there will be 5nA out-of-time beam current. Note, that during GlueX we see about 2-3nA bleedthrough when running at 350nA. He did not do Monte-Carlo simulations, instead he just calculated these analytically assuming momentum spectrum from Ilya's simulations.
  • The calculations showed that these bunches separated by 4ns would show up low reconstructed (<2 GeV) momentum and low reconstructed W (<2.5GeV). Therefore, the event selection should be used to get rid of the background that could produce false bumps in this range of the W-spectrum.
  • Hovanes suggested that it would be good if the physics channels that are being analyzed come up with an estimated of the bleedthrough that they can tolerate without impacting physics conclusions. This would entail simulating and reconstructing events from the physics channel interest as well as from the channels that can populate the W-range if produce by the bleed-through kaons.
  • There was suggestion from Eugene how the K+ momentum cuts in the event selections could reduce the background from out-of-time bunches.
  • Moskov added that they (ODU) are working on the event selection for the K+n channel, and that other channels will need to identify events before plotting W-spectra.
  • We had to cut this discussion short to cover the remaining items on the agenda.




  • Josh reported that the CPS magnet design is nearly complete and the PR will be issued in a week or so.
  • KPT engineering design is complete (assuming there is no need for photon beam in the hall). Hovanes asked collaboration leadership to take a look at the final design before large procurements start. Igor agreed to take a look at the design and approve it or provide comments and suggestions within a week. Igor will contact Josh for details.
  • Eugene pointed out that changes to the KPT assembly needed for providing photon beam will not affect the procurement of some major items like beryllium, tungsten block, or the lead.
  • Josh said that the deadline for PR submission for this fiscal year is close, and we should not delay until next meeting because the timeline will be too tight. (added by Hovanes later: August 19, 2024 for purchases below $250K).




  • Since the meeting went longer than 1 hour, Sean had to leave. Therefore, we did not have a fruitful discussion on the topic of photon beam in the hall. We just had some exchange of opinions. This will be revisited at the software meetings and at the next beamline meeting.




  • Next meeting will be held in two weeks.