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

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

Applications to HEP Halo cleaning in the LHC Diffractive physics (TOTEM experiment) In-situ calibration of the calorimeters in LHC experiments

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.

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.

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

The RD-22 experiment The RD22 Collaboration, CERN DRDC  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

Intas projects Energy at GeV Intensity 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) PRL 90 (2003)

Novel crystal configuration 0.5  2  50 mm 3 Bending exploits anticlastic effects due to anysotropy of crystalline Si

Novel crystal preparation Dicing of the samples by a diamond-blade saw avoiding alignment with major crystalline axes. 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). 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 onePlanar etching removes crystalline planes one by one Removal of such layer by wet planar etching (HF,HNO 3,CH 3 COOH). RSI 73 (2002) 3170

Mechanical vs. chemical treatments 7 meter VACUUM PIPE CRYSTAL S1 S4 S3 S2 EM Images of the beam deflected through mechanically treated (left) and chemically polished crystals (right )

NTA-HCCC project Chemical polishing enhances standard roughness (R a ) As diced Chemicaletching Chemical etching

Surface analysis 30  m APL 87 (2005)

Recent achievements (FNAL) FNAL results (2005) Crystal Collimator in E0 to replace a Tungsten Target

Recent achievements (IHEP) Crystal 1 Magnets Crystal 2 Emulsion 1 S1 S2 S3 Background Channeled_1 30 m 35 m 4.6 m Collimator 1.3 m Emulsion 2 Channeled_2 70 GeV p-beam 5 m R=3 m p-beam

Anomalous effects Exposure of emulsions 1 and 2 made at IHEP in 2002

Interpretation Reflected Channeled d U Particle reflection has been indicated as an interpretation for experimental evidences.

Interpretation First evidence for reflection in a crystal, theoretically predicted in Sov. J. Tech. 55 (1985) 1598

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

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.

Basic idea of the experiment 400 GeV/c 10 5 p/spill 5 mm in diameter 3  rad divergence Unbent beam Reflected beam Bent beam Crystal 10  rad 100  rad 20  rad Primary proton beam Line H8 - SPS The idea is to track the trajectories of the particles and to determine the cross sections for each branch

Layout of the experiment Line H8 vacuum S1 S2S3 Goniometers with crystal holders Si microstrips with 10  m resolution (AMS type) 1 m34 m p

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

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