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2015-09-15 m1 optics discussion » History » Version 3

Rogers, Chris, 15 September 2015 18:10

1 1 Rogers, Chris
h1. 2015-09-15 m1 optics discussion
2 2 Rogers, Chris
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h2. Notes
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We went through Rogers slides. Came up with following job list:
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0. Finish outstanding optics studies + optimisation routines (Rogers)
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1. Investigate optics settings for "Hold SSU at 4T, degrade only SSD" etc (Rogers)
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2. Send Ryan some currents and beams settings to look at MC of "asymmetric" setting (Rogers)
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3. Run MC (Bayes/Liu)
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4. Look at tracker resolution vs Bz (Bayes/Liu)
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5. Look at Demo options (Pasternak/Lagrange)
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6. Validate optics study (Blackmore)
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Nb: It might make sense to pull in Chris Hunt to help out with the tracker resolution study.
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While everything is "wild", it probably makes sense to talk reasonably frequently. Can we regroup on Thursday at noon?
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|p  |   mode   |  FC    |M1_DS|M2_DS |M1_US  |M2_US  |E1_US |CC_US |E2_US|E1_DS |CC_DS |E2_DS| comment |
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|200| solenoid |  60    | 0   |210.93|76.03  |79.06  |234   |274   |253  |234   |274   |253  | This is a not derated solenoid mode; it should have reasonably good beam quality, but will heat - the beta function is large in FC|
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|200| flip     |  67.5  | 0   |275.91|110.95 |147.97 |23.4  |27.4  |25.3 |23.4  |27.4  |25.3 | This is a flip mode; it should have reasonably good beam quality and will cool - but note that the field in the tracker is down to 0.4 T which is pretty low, so tracker reconstruction will be poor|
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Use 
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* 200 MeV/c beam
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* no momentum spread
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* transverse emittances of 3, 6, 10 mm (try all three)
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* start the beam in the upstream tracker region (e.g. 2300 mm from absorber centre) using constant_solenoid mode on the beam and the expected bz
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* Don't bother tracking through the beamline/quadrupoles. 
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Use two configurations; 
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* no materials at all, only fields (equivalent set physics_model none)
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* full materials
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Return, following cut on PID == -13
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* Transmission(z)
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and then plotting only particles which are transmitted into the downstream tracker region
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* Emittance(z)
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* Beta(z)
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* angular momentum(z)