Full-Acceptance Detector Integration at MEIC
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Transcript of Full-Acceptance Detector Integration at MEIC
Full-Acceptance Detector Integration at MEIC
Vasiliy Morozov for MEIC Study Group
Electron Ion Collider Users Meeting, Stony Brook University
June 27, 2014
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Lattice design of geometrically-matched collider rings completedDetector locations minimize synchrotron and hadronic backgrounds
. Close to arc where ions exit. Far from arc where electron exit
Collider Rings
IPs
e-
ions
e-
ions
IP
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50 mrad crossing angle. Improved detection, no parasitic collisions, fast beam separation
Forward hadron detection in three stages. Endcap. Small dipole covering angles
up to a few degrees. Far forward,
up to one degree,for particles passing through accelerator quads
Low-Q2 tagger. Small-angle electron detection
Full-Acceptance Detector
R. Ent, C.E. Hyde, P. Nadel-Turonski
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IR design features. Based on triplet Final Focusing Blocks (FFB). Asymmetric design to satisfy detector requirements and reduce chromaticity. Spectrometer dipoles before and after downstream FFB, second focus downstream of IP. No dispersion at IP, downstream dispersion suppression designed to function as CCB
Ion IR Optics
IP
ions
matching section\coupling comp. FFB FFB
detectorelements CCB\
geom. match\disp. suppression
matching section\coupling comp.
matchingsection
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Detector Modeling & Machine IntegrationFully-integrated detector and interaction region satisfying
– Detector requirements: full acceptance and high resolution
– Beam dynamics requirements: consistent with non-linear dynamics requirements
– Geometric constraints: matched collider ring footprints
far forwardfar forwardhadron detectionhadron detectionlow-Q2
electron detectionelectron detection large-apertureelectron quads
small-diameterelectron quads
central detectorcentral detector with endcaps
ion quads
50 mrad beam(crab) crossing angle
n,
ep
p
small anglesmall anglehadron detectionhadron detection
~60 mrad bend
(from GEANT4)
2 Tm 2 Tm dipoledipole
EndcapEndcap Ion quadrupolesIon quadrupoles
Electron quadrupolesElectron quadrupoles
1 m1 m11 m m
IP FP
Roman potsRoman potsThin exit Thin exit windowswindows
Fixed Fixed trackerstrackers
Trackers and “donut” calorimeterTrackers and “donut” calorimeter
RICH+
TORCH?
dual-solenoid in common cryostat4 m coil
barrel DIRC + TOF
EM
ca
lori
met
er
EM calorimeter
Tracking
EM
ca
lori
met
er
e/π
th
res
ho
ldC
he
ren
ko
v
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Far-Forward AcceptanceTransmission of particles with initial angular and p/p spread vs peak field
– Quad apertures = B max / (fixed field gradient @ 100 GeV/c)– Uniform particle distribution of 0.7 in p/p and 1 in horizontal angle originating at IP– Transmitted particles are indicated in blue (the box outlines acceptance of interest)
6 T max 9 T max 12 T max
elec
tron
bea
m
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Momentum & Angular Resolution– Protons with p/p spread are launched at different angles to nominal trajectory– Resulting deflection is observed at the second focal point– Particles with large deflections can be detected closer to the dipole
elec
tron
bea
m
±10 @ 60 GeV/c
|p/p| > 0.005 @ x,y = 0
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Far-Forward AcceptanceGEMC simulation framework developed by M. UngaroMILOU DVCS event generatorDetection of recoil protons produced in DVCS process by forward detectors
– Acceptance limitation due to beam stay-clear rather than magnet apertures in this case Beam stay-clear depends the emittances achievable by beam cooling:
Z.W. Zhao
/ / / '/ ' / /24 / 5 μm, / 0.24 mradx y x y x y x y x y x y
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Design features similar to that of ion IR. Triplet Final Focusing Blocks (FFB). Asymmetric design to satisfy detector requirements and reduce chromaticity. Spectrometer dipole after downstream FFB, second focus downstream of IP. No dispersion at IP, downstream dispersion suppression by chicane
Electron IR Optics
IP
electrons
matching section
FFB
FFB
detectorelements
disp. suppressionmatching section\coupling comp.CCB matching section\
coupling comp.
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Small-Angle Electron DetectionLow-Q2 tagger
– Dipole chicane for high-resolution detection of low-Q2 electrons
low-Q2 tagger
final focusing elements
e-
ions
e-
ions
Electron beam aligned with solenoid axis
x e-
(top view)
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Compton polarimeter in low-Q2 chicaneSame polarization as at the IP due to zero net bendNon-invasive continuous polarization monitoringPolarization measurement accuracy of ~1% expectedNo interference with quasi real photon tagging detectors
Electron Polarimetry
c
Laser + Fabry Perot cavity
e- beam
Quasi-real high-energy photon tagger
Quasi-real low-energy photon tagger
Electrontracking detector
Photon calorimeter
A. Camsonne, D. Gaskell
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Crab CrossingRestores effective head-on collisions with 50 crossing angle
– Luminosity preserved
Two feasible technologies– Deflective crabbing: transverse electric field of SRF cavities (developed at ODU)– Dispersive crabbing: regular accelerating/bunching cavities in dispersive region
Two possible schemes– Global: one set of cavities upstream of IP next to FFB– Local
• One set of cavities upstream of IP next to FFB• Another set of cavities(n+1/2) downstream of IP
IPe-
ions
global/localcrab cavities
local crab cavities
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Lattice design of geometrically-matched collider rings developed
Interaction regions integrated into collider rings
Detector requirements fully satisfied
Ongoing and future work. Detector modeling. Polarimetry development. Design optimization. Design of interaction region magnets. Systematic investigation of non-linear dynamics. Development of beam diagnostics and orbit correction scheme
Acknowledgements. P. Brindza, A. Camsonne, Ya.S. Derbenev, R. Ent, D. Gaskell, F. Lin,
P. Nadel-Turonski, M. Ungaro, Y. Zhang JLab. C.E. Hyde, K. Park Old Dominion University. M. Sullivan SLAC. Z.W. Zhao JLab & Old Dominion University
Summary & Outlook