tevatron crystal channeling t-980 collaboration: fnal, slac, bnl,cern,pnpi,ihep,infn
DESCRIPTION
Tevatron Crystal Channeling T-980 Collaboration: FNAL, SLAC, BNL,CERN,PNPI,IHEP,INFN. Dean Still April 13, 2009 All Experimenters Meeting. Overview. Explanation of crystal channeling Tevatron Crystal Setup End of Store (EOS) Measurements for 2008/2009 - PowerPoint PPT PresentationTRANSCRIPT
Tevatron Crystal Channeling
T-980 Collaboration:FNAL, SLAC, BNL,CERN,PNPI,IHEP,INFNDean Still
April 13, 2009
All Experimenters Meeting
AEM Crystal Channeling - D. Still 2
Overview Explanation of crystal channeling Tevatron Crystal Setup End of Store (EOS) Measurements for
2008/2009 Moving to a Beginning of Store (BOS) Study Preliminary Results from BOS Conclusion
Tevatron E0 Crystal Layout
crystalE03H Collimator
3.5 mmchanneled beam
23.731 m
Pin Diode
LE033 BLM
FlyingWire
23.731 m
33.115m
LE0PIN
Channeled beamAt E03H
AEM Crystal Channeling - D. Still 5
EOS Measurement for 2008/2009
Thus far, T980 has requested 7 EOS studies since Sept 14, 2008 provide data and understanding on how to utilize crystal collimation.
These 7 EOS can be broken down into 2 categories:1) 1- 5 EOS establish channeling with reinstalled O shape
crystal (installed AUG 2008) AND attempt to understand 2 fundamental questions about what has been demonstrated.
2) 6-7 EOS test for incorporating the crystal into the Tevatron automated halo removal system
AEM Crystal Channeling - D. Still 6
Summary of EOS Work
Analysis & Slide: Vladimir Shiltsev
From very EOS on Sept 14 EOS demonstrated channeling & improved loss localization with new goniometer, characterized crystals, and enhanced beam diagnostics, BUT … there are 2 basic questions to understand:
1) Why channel width and VR efficiency are different and worse than 2005.
2) Why the channeled beam does not appear to have the correct displacement at E03H collimator.
All these are important questions to answer which tell us about crystal performance, efficiencies, …
AEM Crystal Channeling - D. Still 7
Learned Info from EOS
Newly learned information from studies with new instrumentation included:
1) Mainly abort gap beam was being channeled.
With this knowledge coupled with the fact that there is a large miscut angle maybe could answer some of the initial questions. - Is it related to beam dynamic or crystal property.
Channeled abort gap beam
Bunched beam
AEM Crystal Channeling - D. Still 8
Effects Due to Crystal Mis-Cut AngleAccording to most recent simulations
Having wrong sign(+) of large miscutangle can explain broading of channel width& difference in displaced beam at collimator.
February 3, 2009 A.Drozhdin, A,Apyan
AEM Crystal Channeling - D. Still 9
Overview
Plan and Motivation for 2009 End of Store (EOS) Measurements for
2008/2009 Moving to a Beginning of Store (BOS) Study Preliminary Results from BOS Conclusion
AEM Crystal Channeling - D. Still 10
Plan and Motivation for 2009The ultimate goal of T980 for 2009 is to have enough understanding and practice
to use single plane crystal collimation as part of the normal halo removal operation for every store.
By having the capability of incorporating crystal channeling into every store or many stores gain benefits for: More possible hours of utilizing crystal channeling over ONLY EOS. Gain practical and operational experience using crystal channeling. Hopefully demonstrate reduction of halo loss for either or both CDF and D0
detectors.
Of Course the caveat to incorporating crystal channeling for every store:it can have NO negative impact on the Tevatron Collider Run
AEM Crystal Channeling - D. Still 11
Moving to Beginning of Store Studies (BOS)
Things for certain to this point:•Crystal channeled beam could be collimated & intercepted locally (by E03H) thus improving collimation system efficiency•Results are reproducible contrary to earlier studies.
There are many questions about performance and efficiencies to still be answered but we felt we are very confident in the one fact that channeledbeam can be collimated.
We wanted to move to our main goal which is to use the crystal during a store to start seeing if it can truly reduce proton halo back grounds.
AEM Crystal Channeling - D. Still 12
T-980 Review Process Aug 7, 2008 : T-980 had a formal Installation review by Accelerator
Division, CDF and D0 to confirm readiness and impact to collider program for crystal collimation. Additional mandatory review for determining readiness for conducting a BOS.
Feb 4, 2009: T-980 held BOS review which recommended BOS
with EOS confirmation of automated placement of crystal.
AEM Crystal Channeling - D. Still 13
EOS for Store 6901 – Test for BOS
Auto insertion of crystal Horizontal worked well
After angle set toChanneling, completedE03H scan to verify channeling
Used EOS of 6901 to test full auto insertion of crystal and check that channelingCan be established.
Setting the crystal angle To channeling
AEM Crystal Channeling - D. Still 14
Overview
Plan and Motivation for 2009 End of Store (EOS) Measurements for
2008/2009 Moving to a Beginning of Store (BOS) Study Preliminary Results from BOS Conclusion
AEM Crystal Channeling - D. Still 15
Finding channeling point for BOS
Store 6903 BOS No clear channel point Store 6901 EOS clear channeling
Channeling should be ~-250urad
AEM Crystal Channeling - D. Still 16
Preliminary Look at 1st BOS - Store 6903
Crystal AngleDrift ~ 90urad
Loss in bunchAt E03H
Losses in Abort gap at E03H
This is crystal channel point.
Crystal angle drifted ~ 90urad over 16 hours during store.
This is most likely do to Thermal heating of Goniometer.
Need better angular Control.
AEM Crystal Channeling - D. Still 17
-400 -200 0 200
Crystal Angle (urad)
2000
7000
12000
17000
22000
27000
T:E
1L
AB
T L
oss
(h
z)
20
40
60
80
100
120
T:L
E0
PIN
Lo
ss (
hz)
Store 6903 EOS angle scanT.E1LABTT.LE0PIN
Angle Scans at the End of Store 6903
AEM Crystal Channeling - D. Still 18
-350 -300 -250 -200 -150
crystal angle (urad)
0
5000
10000
15000
20000
Loss
(hz)
6903_EOS_ANG_SCAN_E1LABT.PAGE1
T.E1LABT
Spread of Angles Around Channel
-285 -252
AEM Crystal Channeling - D. Still 19
-310 -300 -290 -280 -270 -260
Crystal Angle (urad)
0
40000
80000
120000
T:E
1lA
BT
Lo
ss (
hz)
0
50000
100000
150000
T:E
1L
BN
C lo
ss (
hz)
Store 6903 Losses around channelT:E1LABTT:E1LBNC
ChanneledDistributionAngles
Store 6903 BOS – Losses at the collimator
AEM Crystal Channeling - D. Still 20
Halo Losses During BOS Store 6903
Store 6906 – Normal store No crystal Store 6903 – Crystal Collimation used
CDF proton halo lossD0 proton halo lossLE033 – local crystal lossCDF Luminosity
AEM Crystal Channeling - D. Still 21
Crystal Angle Stabilization Software Added software to correct for temp. effects that change crystal angle.
Corrects to ~ 4urad around a given set point.
Max deviation ~ 14 urad during motor reversal periods.
Crystal Laser Angle(urad)
4 urad
Crystal AngularMotor counts
AEM Crystal Channeling - D. Still 22
Conclusion First big transition step in being able to use crystal collimation at
the beginning of store (BOS).
There was no negative effect to the collider store from the BOS and hopeful that crystal collimation can be used for many stores.
The angle of the crystal changed by ~90urad of the store which has been addressed as a software angle feedback system.
Crystal collimation during the BOS showed signs of channeling at E0 but it is too early to demonstrate effect around the ring or benefits to CDF and D0 IP’s.
There is still much work to be done to understand and demonstrate effects to miscut angle and effect of losses around the ring.