RICH detectors for LHCb Tito Bellunato INFN Milano-Bicocca On behalf of the LHCb RICH collaboration 10th International Conference on Instrumentation for.

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Presentation transcript:

RICH detectors for LHCb Tito Bellunato INFN Milano-Bicocca On behalf of the LHCb RICH collaboration 10th International Conference on Instrumentation for Colliding Beam Physics Novosibirsk, –

Outline of the talk The LHCb experiment RICH1 & RICH2 The Hybrid Photon Detector (HPD) The aerogel radiator Commissioning and performance Summary Novosibirsk, T. Bellunato- INSTR082

b-Physics at the LHC Novosibirsk, T. Bellunato- INSTR08 3 particle identification secondary vertices forward event leptons ν _ μ ~10 mm

The LHCb experiment Novosibirsk, T. Bellunato- INSTR08 Two Ring Imaging Cherenkov detectors provide p/K/π identification RICH2 RICH1 250 mrad 300 mrad VErtex LOcator Dipole Track Calo Muon

The experimental site Novosibirsk, T. Bellunato- INSTR08 5 RICH2 RICH1

Novosibirsk, T. Bellunato- INSTR08 6 C 4 F 10 gas n= Up to ~70 GeV/c CF 4 gas n= Beyond ~100 GeV/c Silica Aerogel n= GeV/c RICH1 : 25  250 mrad vertical 25  300 mrad horizontal RICH2 : 15  100 mrad vertical, 15  120 mrad horizontal Cherenkov radiators All charged tracks in b-events

RICH layout Novosibirsk, T. Bellunato- INSTR glass spherical mirrors 40 glass flat mirrors Central Tube support structure 8m 288 HPDs and magnetic shielding Aerogel

Novosibirsk, T. Bellunato- INSTR08 8 Photon detectors requirements C 4 F 10 (small) Aerogel (large) CF 4 RICH1 RICH2 total area: 3.3 m 2 single photon sensitivity: nm quantum efficiency: >20% good granularity: 2.5 x 2.5 mm 2 active area fraction: 63% # of channels: 500k LHCb DAQ rate: 40MHz rad. tolerant: 3kRad/year Hits in the photon detectors for one event (full LHCb simulation)

Pixel Hybrid Photon Detectors Novosibirsk, T. Bellunato- INSTR08 9  Pixel HPDs developed in collaboration with industry (Photonis-DEP lead partner)  Vacuum tube with silicon pixel readout ( Quartz window with S20 photocathode)  75 mm active diameter  484 HPDs to meet the requirements  Factor 5 20kV  Encapsulated electronics: – 8192 pixels logically OR-ed in groups of 8 to form a matrix of 32 x 32 – binary output of 1024 channels

Magnetic distorsions Novosibirsk, T. Bellunato- INSTR G Shielded 10 G Unshielded Residual distorsions monitored and corrected for by projecting patterns on the HPDs in situ

HPD qualification Novosibirsk, T. Bellunato- INSTR08 11 Two Photon Detector Test Facilities (PDTFs) have qualified all 550 HPDs produced by Photonis/DEP. 98% of tubes have passed the selection criteria. Excellent response, QE, dark counts, ion feedback. The development and serial production of very high quantum efficiency photocathodes for the HPD has been an ouststanding technological success

Novosibirsk, T. Bellunato- INSTR m Upper Magnetic Shielding Spherical Mirrors Lightweight carbon fibre mirrors 1.5% radiation length Glass Planar Mirrors Beryllium beampipe (defines RICH1 inner acceptance) Photon detector plane 14 by 7 Hybrid Photon Detectors (HPDs) Gas Enclosure supports mirrors and aerogel, contains C 4 F 10 RICH1 Exit Window Carbon fibre & PMMI foam Sealed direct to the beampipe. RICH1 schematics Aerogel goes here

Carbon Fibre Mirrors RICH1 installation Novosibirsk, T. Bellunato- INSTR08 13 Beryllium beampipe, seal to VELO and flat mirrors Upper HPD box 98 HPDs

RICH2 Novosibirsk, T. Bellunato- INSTR08 14 HPD modules inserted here HPD column module

RICH2 Commissioning Novosibirsk, T. Bellunato- INSTR08 15 Routine operation with high voltage and full integration into LHCb Control system and Data acquisition system. RICH2 HPD planes, pulsed laser Ready for collisions! HPD array from inside RICH2

Silica aerogel Novosibirsk, T. Bellunato- INSTR litres produced for LHCb 200x200x50 mm tiles – the largest ever Exceptional clarity C ~  m 4 cm -1 I/I 0 = A exp –(Ct/ λ 4 ) for thickness t in cm Hygroscopic, produced by Boreskov Institute of Catalysis Novisibirsk

Aerogel for LHCb Novosibirsk, T. Bellunato- INSTR08 17 Successfully tested against: humidity : loss of transparency recovered by baking at 500 °C radiation: neutron, proton and γ up to several LHCb lifetimes exposure to C 4 F 10 : tolerable slight modification of optical parameters Performance of the aerogel as radiator for the RICH of LHCb has been confirmed by several tests on charged particle beams over the years 10 LHC years

Refractive index characterisation Novosibirsk, T. Bellunato- INSTR08 18 Homogeneity measured with laser and charged particle beam: σ (n-1)/(n-1) ~ 0.76% (contribution to   ~ 0.8 mrad) Refractive index measured over wide wavelength range = 1.028

Aerogel mechanics Novosibirsk, T. Bellunato- INSTR08 19 Carbon fiber box with wings to stop photons radiated upstream of aerogel D263 glass filter to kill scattered photons and improve resolution Trial installation successful, aerogel goes in as last component in spring

RICH performance Novosibirsk, T. Bellunato- INSTR08 20 Pixel map of a C 4 F 10 ring focussed on 4 HPDs integrated over ~50k events  Performance of the RICH system has been verified in a 80 GeV/c charged particle beam at CERN SPS. C 4 F 10 ~1m radiator length  Realistic 25 ns beam structure  Final RICH hardware and DAQ  Full simulation results for photon yield and θ c resolution have been validated

Particle ID performance Novosibirsk, T. Bellunato- INSTR08 21  Ring finding - The algorithm uses tracks, and performs a global likelihood fit to particle hypotheses across both RICH detectors.  π – K separation - Excellent efficiency and low mis-ID rate AerogelC 4 F 10 CF 4 photon yield isolated tracks single p.e. resolution (mrad) Kaon identification performance

Summary and prospects LHCb RICH project in good shape RICH2 fully equipped, commissioning is already at an advanced stage RICH1 is almost completed, commissioning will benefit from RICH2 experience Excellent quality and highly performing HPDs The RICH system will contribute to physics results starting from LHC day one. Novosibirsk, T. Bellunato- INSTR08

Novosibirsk, T. Bellunato- INSTR08 23