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Crystal Channeling Study (experiment to study and apply channeling to HEP)

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Title: Crystal Channeling Study (experiment to study and apply channeling to HEP)


1
Crystal Channeling Study(experiment to study and
apply channeling to HEP)
  • Vincenzo Guidi
  • University of Ferrara and INFN

2
Channeling in crystals
Trapping of charged particles in the inter-planar
potential well (20 eV in Si)
Critical angle
A bent crystal can be used to steer particles
through channeling
3
Applications to HEP
  • Halo cleaning in the LHC
  • Diffractive physics (TOTEM experiment)
  • In-situ calibration of the calorimeters in LHC
    experiments

4
Two-stage collimation
The number of secondary collimators grows quickly
when background or machine protection
requirements are strict and a high collimation
efficiency is required.
5
Crystal collimation
Use a bent crystal to channel halo away from the
beam core, intercept with a scraper downstream.
Number of secondary collimators can be greatly
reduced.
6
Optimal design for the LHC
Optimal size of the silicon crystal for
collimation is about 10 mm for 0.1 mrad (7 TeV).
NIM B 234 (2005) 23
7
The RD-22 experiment
  • Large channelling efficiency measured for the
    first time in extraction mode
  • Consistent with simulation expectation for high
    energy beams
  • Experimental proof of multi-turn effect
    (channelling after multi-traversals)
  • Definition of a reliable procedure to measure the
    channelling efficiency

The RD22 Collaboration, CERN DRDC 94-11
8
Intas projects
  • Energy at 1.3-70 GeV
  • Intensity 1012 protons in spills of 2 s duration
  • Efficiency greater than 85
  • Equivalent to 1000 T dipole magnetic field

Extraction efficiency vs. crystal length at 70
GeV
PRL 87 (2001) 094802
PRL 90 (2003) 034801
9
Novel crystal configuration
0.5?2?50 mm3
Bending exploits anticlastic effects due to
anysotropy of crystalline Si
10
Novel crystal preparation
  • Dicing of the samples by a diamond-blade saw
    avoiding alignment with major crystalline axes.
  • Defects are induced by the dicing saw (a
    surface layer estimated to be as thick as 30?m is
    rich in stratches, dislocations, line defects and
    anomalies).
  • Planar etching removes crystalline planes one by
    one

RSI 73 (2002) 3170
Removal of such layer by wet planar etching
(HF,HNO3,CH3COOH).
11
Mechanical vs. chemical treatments
Images of the beam deflected through
mechanically treated (left) and chemically
polished crystals (right)
12
NTA-HCCC project
Chemical etching
As diced
As diced
Chemical etching
Chemical polishing enhances standard roughness
(Ra)
13
Surface analysis
30??m
APL 87 (2005) 094102
14
Recent achievements (FNAL)
FNAL results (2005)
Crystal Collimator in E0 to replace a Tungsten
Target
15
Recent achievements (IHEP)
16
Anomalous effects
Exposure of emulsions 1 and 2 made at IHEP in 2002
17
Interpretation
Particle reflection has been indicated as an
interpretation for experimental evidences.
18
Interpretation
First evidence for reflection in a crystal,
theoretically predicted in Sov. J. Tech. 55
(1985) 1598
19
Reconsidering FNAL experiments
1 TeV Channeling at the Tevatron, October 5, 2005
Not volume capture, but volume reflection !
The observed tail beside the channeling peak is
most likely induced by beam reflection into the
crystal itself
20
CCS an experiment to study and apply channeling
to HEP
  • Continuous upgrading of performance of crystals
    boosted new achievements and new prospects.
  • Need for a newly conceived experiment to
    investigate novel phenomena.
  • Three-weeks machine time (external line H8, SPS)
    has been requested in 2006 and decision will be
    taken soon.

21
Basic idea of the experiment
Bent beam
10 ?rad
Line H8 - SPS
Crystal
Primary proton beam
100 ?rad
Unbent beam
20 ?rad
  • 400 GeV/c
  • 105 p/spill
  • 5 mm in diameter
  • 3 ?rad divergence

10 ?rad
Reflected beam
The idea is to track the trajectoriesof the
particles and to determine the cross sections
for each branch
22
Layout of the experiment
Goniometers with crystal holders
Line H8
S2
S3
S1
vacuum
vacuum
p
Si microstrips with 10 ?m resolution (AMS type)
1 m
34 m
23
Collaboration
  • CERN infrastructure of the experiment
  • IHEP lattice design, simulations (INTAS)
  • PNPI crystals (INTAS)
  • JINR simulation, DAQ (INTAS)
  • FNAL mutual participation in experimental runs
  • FE crystals, construction of the apparatus
    (CCS-NTA)
  • LNL goniometers (CCS-NTA)
  • PG Si microstrips (CCS)
  • Participation of persons from PI and TO

24
Details of the experiment CCS
Duration 3 years INFN personnel FE (4 FTE),
PG (2.5 FTE), LNL (4 FTE), TO, PI Cost in
2006 150 kEuro for construction of detectors
(AMS type) and implementation at CERN
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