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Progress of the NA62 RICH detector

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1 Progress of the NA62 RICH detector
Siena 2013 13° Topical Seminar on Innovative Particle and Radiation Detectors (IPRD13) 7-10 October Siena, Italy Progress of the NA62 RICH detector On behalf of INFN&Univ Perugia INFN&Univ Firenze CERN M.Lenti INFN Sezione di Firenze

2 Outlook NA62: the Rare Kaon Decay Experiment at CERN The NA62 RICH
The Vessel and the Gas system The Mirrors The Photomultipliers FE and DAQ 2007 and 2009 test beams: results Conclusions M.Lenti

3 The NA62 Experiment at CERN
NA62 aim at a 10% measurement of the BR(K+→p+) Theory: BR = (0.85±0.07)×10-10 (very small th.error!!) Present result: ×10-10(BNL E787/E949) Very hard from exp.point of view: one charged track (a pion) and nothing else!! +1.15 -1.05 M.Lenti

4 The NA62 Layout 750 MHz primary Hadron beam at 75GeV/c 6% are Kaons
7-10 MHz of Muon Rate in the Detectors SAV Small Angle g Veto LAV: Large Angle Photon Veto Vacuum Tank CHOD Charged Hodoscope CHANTI Charged Particle Veto Target RICH KTAG Beam Pipe Measure Kaon: Time Angles Momentum GTK LKr MUV RICH Straw Tracker Decay Region 65m Total Length 270m M.Lenti

5 Background n.1: K+→m+n GTK + STRAWS MUV RICH Km2 :largest BR: 63.4%
|PK|=75 GeV/c p qKp K+ n Km2 :largest BR: 63.4% Need ~10-12 rejection factor Kinematics: 10-5 Muon Veto: 10-5 Particle ID: 10-2 n m2miss=(PK-Pp)2 GTK + STRAWS MUV RICH 15<|Pp|<35 GeV/c Match a track (pion) seen by the STRAWS (10 MHz) with a track (kaon) seen by the GTK (750 MHz) Wrong matching: wrong missing mass Measure the track time, both upstream and downstream at 100 ps level M.Lenti

6 The NA62 RICH Detector Mirror mosaic Flanges with 2 x 1000 PMts
Length > 17 m; Ø = up to 4m INFN&Univ Perugia INFN&Univ Firenze CERN Filled with Neon Gas at 1 atm. Beam Pipe M.Lenti

7 The RICH Vessel Conical cap: Support collars Part of one section.
17 m long vessel in construction steel, vacuum proof max overpressure: 150 mbar 4 m wide (beginning), 3.4 m wide (end) 4 cylindrical sections (“drums”) and one conical cap beam pipe (Ø 157 mm) going through thin aluminium entrance and exit windows M.Lenti

8 The Gas System Vessel volume: 200 m3
Neon at slightly above atmospheric pressure Neon density stability < 1% Contaminants < 1% The vessel is first fully evacuated Then fresh Neon is introduced in the vessel At the end the vessel is valve closed M.Lenti

9 The Mirrors Mirror Assembly
18 hexagonal mirrors (700 mm wide, 25 mm thick) 2 half mirrors around the beam pipe. Mirror Parameters + Quality: Spherical mirrors f= 17±0.1 m Reflectivity > 90% (195 – 650nm) Do≤ 4mm (circle which collects 90% of the reflected light.) M.Lenti

10 The Mirrors Alignment The orientation of the mirrors is remotely
adjustable using piezo-motors Aluminum ribbons 200 mm thick and 10 mm wide are used MIRROR SUPPORT DOWEL Mirror Support Prototype Each mirror is supported by means of a dowel inserted in a hole drilled in the back of the mirror A third purely vertical ribbon is used to avoid mirror rotation Piezo Motors 20 Newtons 35 mm range 70 nm resolution LIGHTER TRANSMISSION SUPPORT M.Lenti

11 THE MIRRORS– FRONT VIEW
M.Lenti

12 STABILIZING RIBBONS & MIRROR SUPPORTS – FRONT VIEW
M.Lenti

13 THE HOLES ON THE SUPPORTING HONEYCOMB PANELS – FRONT VIEW
M.Lenti

14 THE TENSIONING RIBBONS – REAR VIEW
M.Lenti

15 The Photomultipliers Hamamatsu R7400U-03 UV-glass, bialkali, 8 dyn
16 mm wide (8 mm active) Gain 1.5 V 280 ps time jitter (FWHM) nm response (420 nm peak) Q.E. around 20% on peak PM output (1 p.e.): 240 fC, peak at 200 mA or -10 mV (50 ) Rise time: 0.78 ns, fall time1.6 ns M.Lenti

16 The PMs, cont’d 976 PMs packed per spot (18 mm min dist.)
Light collection: Winston cones with aluminized mylar foil Quartz window to separate Neon from air O-rings for light tightness and thermal contact M.Lenti

17 The PM, III Neon-air separation disk PM lodging disk PM “face” side
Quartz window side PM “rear” side: detail Few PMs inserted Detail of Winston Cones with and w/o Mylar foils Detail of a quartz window M.Lenti

18 Front-End and DAQ FE+DAQ contribution < 50 ps NINO ASIC (from ALICE) as fast discriminator operated in Time over Threshold HPTDC (developed at CERN) embedded on TEL62 boards (evolution from LHCb TELL1) RICH used in the Level-0 trigger of NA62 M.Lenti

19 Test Beams Strong RD to validate the chosen approach with prototypes
NIM A 593 (2008) NIM A 621 (2010) Test Beams Strong RD to validate the chosen approach with prototypes 2007 Test Beam: RICH proto 96 PMs (time resolution, n.of p.e.) 2009 Test Beam: RICH proto 414 PMs (3s p-m separation, DAQ,…) M.Lenti

20 RICH400: performances NIM A 593 (2008) 314-318
pions pions pions M.Lenti

21 Conclusions The NA62 RICH is a far demanding object
Strong RD validated the project Installation schedule: Nov 2013: RICH vessel delivery Jun 2014: Mirrors Installation completed Aug 2014: PM installation completed Sep 2012: Gas filling completed Oct 2014: RICH commissioning and first physics run of NA62 M.Lenti

22 SPARES M.Lenti

23 Kinematics 92% K+ decays 8% K+ decays PK : beam spectrometer
qKp K+ n n m2miss=(PK-Pp)2 92% K+ decays 8% K+ decays PK : beam spectrometer Pp : straw chambers spectrometer M.Lenti

24 THE HALF CENTRAL MIRROR
TWO DOWELS M.Lenti

25 THE HALF CENTRAL MIRROR
TENSIONING RIBBON (HORIZONTAL AXIS ROTATION) SLIDING DOWEL SYSTEM (VERTICAL AXIS ROTATION) MIRROR SUPPORT M.Lenti

26 THE SLIDING DOWEL SYSTEM - DETAIL
KNOB SUPPORT FIXED DOWEL KNOB ACTUATING BAR SLIDING DOWEL MIRROR SUPPORT M.Lenti

27 THE HALF MIRROR IN PLACE
M.Lenti

28 RICH prototype 17 m long, 0.6 m wide cylindrical vessel
17 m focal, 0.5 m wide mirror 96(2007) or 414(2009) PM Vessel evacuated, then Neon filled Prototype placed along the old NA48 beam line at CERN M.Lenti

29 RICH-100 Prototype 2007 Test Beam
96 PMT Mirror f=17 m p- p=200 GeV/c (SPS) CERN Cavern ECN3 M.Lenti

30 RICH-100: 2007 Test Beam results
NHits ≈ 17 DtEvent ≈ 70 ps M.Lenti

31 RICH-100: results Dqc≈ 50 mrad DtEvent ≈ 70 ps M.Lenti

32 RICH-400: 2009 test beam 414 PMT + FE and DAQ , cooling
Pions at tunable energy M.Lenti

33 RICH-400: fitted rings 20 GeV/c Hard to reconstruct ring… positrons
pion M.Lenti

34 RICH-400: p-m separation Easy to have a good pion beam, not a muon one
For each energy point, take two runs: One at the same nominal energy One at energy×mp/mm (pion velocity equal to muon velocity at nominal energy) Compare the two distributions of the fitted Cherenkov Rings GeV/c M.Lenti

35 RICH-400: results 15 GeV/c e m p p×mp/mm Ring Radius (mm) 35 GeV/c p e
Muon suppression (15-35 GeV/c): 0.7% p×mp/mm Ring Radius (mm) M.Lenti

36 RICH 400: results Paper submitted to NIM on April 23, 2010 9.10.2013
M.Lenti


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