OPTICS UPDATE Ulisse Bravar University of Oxford 3 August 2004.
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Transcript of OPTICS UPDATE Ulisse Bravar University of Oxford 3 August 2004.
OPTICS UPDATE
Ulisse Bravar
University of Oxford
3 August 2004
How to tune the MICE channel
• Baseline configuration: flip modep = 200 MeV/c = 42 cm in LH Bz = 4 T in solenoids
• Steps: achieve minimum as stated: FC & CCuniform B-field inside spectrometer (to 1%): ECuniform inside spectrometer: MC
Software• Matching code from Bob Palmer:
written in QuickBasic, runs on Windows ICOOL + minimization routine ‘empty’ MICE channelparaxial tracks
• Numerical evolution of by John Cobb: ‘empty’ MICE channel from G. Penn, MuCool note 71: 2 ’’ – (’)2 + 4
2 2 – 4 = 0
• Work in progress: a) matching & minimization for Unix, ICOOL independentb) study of large amplitude tracks, with dE/dx & RF, p-spread
Present status of solutions• For every set of coil configurations: a) Determine paraxial solutions for p = 200 MeV/c, flip and no-flip
modes, = 42, 25, 17, 7 cm in LH: 8 sets of currents b) Semi flip mode obtained by combining flip & no-flip: 4 more
setsc) Stages IV and V of MICE obtained from stage VId) p < 200 MeV/c: scale solutions from p = 200 MeV/c: (8 + 4) x 2 =
24 additional sets of currentse) p = 240 MeV/c: scale FC and CC, repeat matching:
12 more currents
• So far, have several of the solutions from first line. Also, solutions for reduced gaps: 400 mm, 500 mm…
Optical solutions (1)
• MICE proposal to RAL (2003):
• coil configuration from tab. 4.1
• currents from tab. 4.2, case 1a
• p = 220 MeV/c• p = 200 MeV/c• p = 180 MeV/c
• MISMATCH for p = 200 MeV/c !!!
z (m)
(
m)
Bz
(T)
Optical solutions (2)
• Currents from Bob Palmer’s note, Sept. 2003Tab. 4 & 5 SFOFO = 43 cm
• 200 MeV/c looks OK:
= minimum in LH
= uniform in solenoid
• Mismatches at 180 and 220 MeV/c z (m)
Bz
(T)
(
m)
Optical solutions (3)
• Coil configuration from Mike Green and INFN-GE agreed upon at CERN 2004 meeting
• 600 mm GAP
• Currents determined with Bob Palmer’s minimization routine
• Again at p = 200 MeV/c looks OK
• Note: big increase in match coil region z (m)
Bz
(T)
(
m)
What happens at large amplitudes?
in the centre of LH cell
• Flip mode, p = 200 MeV/c
• From Bob Palmer, June 2004
• Optical solutions with paraxial rays work fine for beams with = 6 mm rad
momentum (GeV/c)
(
m)
What is wrong with the present coil configuration?
• 600 mm gap causes growth. Possible consequences: beam scraping, smaller momentum acceptance
• 600 mm gap causes increase. The beam that we are measuring is not the beam that we are cooling
• The smaller the gap, the better
Bob Palmer 9/2003
`M. Green 600 mm’• larger -- presumably due to increased spacing
matching – focus coils and smaller B
• Smaller momentum acceptance:off momentum muons might scrape beam aperture
Different here
Bz
Reminder
functions @ 200 MeV/c, M. Green configurations, 400, 500, 600mm
400 mm 500 mm 600 mmNew New Old
Green = - 5% solid -10% dashed Black = On momentumRed = + 5% solid +10% dashed
Beta always > 1.8 metres in 2nd RF for p = 1.1 x ptune
Decreased spacing helps beta-stability
‘400mm’ not as stable as Palmer solution (not buildable?)
functions @ 240 MeV/c, M. Green configurations, 400, 500, 600mm
400 mm 500 mm 600 mmNew New New
240 MeV/c looks ‘tidier’
Beta still rises in 2nd RF – but less than at 200 MeV/c
Emittance growth in 600 mm gap
• MICE Note 49 (Bob Palmer, September 2003)
• Present coils (Mike Green et al., March 2004)
from ecalc9f increases in drift
• Quick fix: x-px correlation in the Gaussian beam in the upstream solenoid
PROBLEM
z (m)
(
m r
ad)
Quick fix: x – px correlation
Note 49MG coils
MG coilswith
x-px correlation
z (m)
(
m r
ad)
x (m)px (GeV/c)
dE/dx and acceleration
• From Bob Palmer, June 2004
• Conclusion: Acceleration, dE/dx have no observable effect on MICE optics
momentum (GeV/c)
(
m)
MICE stages IV and V
z (m)z (m)
(
m)
Bz
(T)
Stage VStage V Stage IV
MICE stage III
z (m)z (m)
(
m)
Bz
(T)
(
m r
ad)
Flip and no-flip modes
z (m)z (m)
(
m)
Bz
(T)
Conclusions
• Optical matching technique works fine, software upgrades in progress
• 48 optic solutions for every coil configuration, for stage VI only. Currents will be updated as necessary
• 450 mm gap looks better than 600 mm, but how good is good enough?
• Need decision on B-field in spectrometer when p < 200 MeV/c