can micro channeling improve the totem experiment
DESCRIPTION
Suggestions by V. Avati and K. Eggert Idea : Crystal placed at 6 s from the LHC beam, deflecting the protons, can improve considerably the proton acceptance of the TOTEM Roman pots Principle lay-out Physics example : Higgs search in central diffraction. - PowerPoint PPT PresentationTRANSCRIPT
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Can micro channeling improve the TOTEM experimentCan micro channeling improve the TOTEM experiment
Suggestions by V. Avati and K. Eggert
Idea: Crystal placed at 6 from the LHC beam, deflecting the protons, can improve considerably the proton acceptance of the TOTEM Roman pots
Principle lay-out
Physics example: Higgs search in central diffraction
Crystal Collimation in Hadron Storage Rings, CERN 7-8 March 2005
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TOTEM ROMAN POT IN CERN SPS BEAM
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TOTEM APV hybridFlexible
connections(In production)
detector
beam
ROMAN POT DETECTORS and ELECTRONICSROMAN POT DETECTORS and ELECTRONICS
Readout chip VFAT
Pitch adapter on detector
Test card for VFAT
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Detector Distance vs. Beam
nσ-reach?
(RA LHC MAC 13/3/03)
Detector distance vs. beam is determined by the beam halo.
n = dmin/x,y(z) 10-15
Expected halo rate: 6kHz(for 43 bunches, Np = 1010, N = 1m, n = 10)
Active detector starts at the distance from the physical edge
Closest approach :n = 10
= 200m
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Elastic Scattering* = 1540 m
acceptance
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Example ProcessesExample Processes
2
22 'ppp
P
p1
p2p2’
X d/dproton:p2’ diffractive system Xrapidity gap
=–ln
min 0ln(2pL/pT) max
Measure leading proton ( and rapidity gap ( test gap survival).
Single Diffraction:
2=– ln 1=– ln
p1
p2 p2’
p1’
PMX
2 = s
PX
diffractive system Xproton:p2’proton:p1’
rapidity gaprapidity gap
min max
Double Pomeron Exchange:
Measure leading protons ( 1, 2) and compare with MX, 1, 2
MX2 = s
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Diffractive Higgs ProductionDiffractive Higgs Production
MH2 = s
%86.0%86.0
1202
12
cGeVM Higgs
beam
p’
p’roman pots roman pots
dipoledipole
b -jet
Hgap gap
b -jet
p p
(1-p
(1-p
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Roman Pots in the forward regions
Leading diffractive protons seen at different detector locations (* = 0.5m)
y(m
m)
x(mm)
220m
y(m
m)
x(mm)
420m
Dispersion D = 0.08 m D=1.5m
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Crystal extraction
RP stations
6 6 x x beam profilebeam profile with crystal extraction with crystal extraction
RP stations
Crystal extraction
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Hit distribution in the RP detectorHit distribution in the RP detector
protons deflected by the crystal
the other protons in RP
X [m]
Y [m]
10 beam profile
Detector edge
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Angular distribution in the detectorAngular distribution in the detector
= 15rad
Bent by the crystal (by 0.5 mrad)
rad
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-acceptance for a Higgs with -acceptance for a Higgs with MMHH=120 GeV/c=120 GeV/c22
In Totem acceptance (68% of 1)
With cristal extraction
2<1
Totem acceptance with cristal extraction (87% of 1)2<1
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Conclusions
Crystal extraction is promising to approach the LHC beams Crystal extraction is promising to approach the LHC beams closer than with standard RP detectorscloser than with standard RP detectors
Larger acceptance for diffractively produced HiggsLarger acceptance for diffractively produced Higgs
Same method could be used for elastic scattered protons to Same method could be used for elastic scattered protons to reach the Coulomb regionreach the Coulomb region
Needs extensive tests with crystals and Roman Pots in the Needs extensive tests with crystals and Roman Pots in the SPS (see talk of Marco Oriunno)SPS (see talk of Marco Oriunno)