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Dec7,2007 ie-FP7 Test Beams for detector R&D at CERN The PS East Area The SPS North Area Irradiation facilities.

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Presentation on theme: "Dec7,2007 ie-FP7 Test Beams for detector R&D at CERN The PS East Area The SPS North Area Irradiation facilities."— Presentation transcript:

1 Dec7,2007 ie-FP7 Test Beams for detector R&D at CERN The PS East Area The SPS North Area Irradiation facilities

2 Dec7,2007ie-FP7 The PS East Area

3 Dec7,2007ie-FP7 Schematic view IRRAD TO T7 SEC T8 AREA: Target ZT8.MTV02 T7 AREA: F61S.BHZ02 (irrad.) T7 AREA: ZT7.MTV01 (sec.) NORTH AREA: target F61N.MTV02 Target ZT7.MTV03 The PS East Area

4 Dec7,2007ie-FP7 Experimental Areas The PS East Area

5 Dec7,2007ie-FP7 Beam Characteristics T7The T7 beam is a secondary beam that delivers secondary particles up to 10 GeV/c at a production angle of 0 degrees. T8The T8 beam is a primary beam that delivers primary protons to the DIRAC experiment. Normally the beam momentum is 24 GeV/c. DIRAC T9The T9 beam is a secondary beam that delivers secondary particles up to 15 GeV/c at a production angle of 0 degrees. T10The T10 beam is a secondary beam that delivers secondary particles up to 7 GeV/c at a production angle of 61.6 milliradians. T11The T11 beam is a secondary beam that delivers secondary particles up to 3.5 GeV/c at a production angle of 149.2 milliradians. The PS East Area

6 Dec7,2007ie-FP7 Infrastructure What is (could be) provided Counting houses (barracks) with racks and network connections Beam instrumentation: Scintillator for beam intensity measurement XDWC for beam profile measurement Threshold Cherenkov counter for particle ID Scanning table (XSCA) – shared with SPS North Area users Magnets - see slides later What is not there! Infrastructure for large detectors – size of areas Cryogenics The PS East Area

7 Dec7,2007ie-FP7 The SPS North Area CCC EHN1 BA81 (ps building) BA80 (ps building) TCC2 access TCC2 targets (underground) EHN2 (COMPASS) ECN3 (NA48)

8 Dec7,2007ie-FP7 Introduction The proton beam (400 GeV/c) from SPS is slowly extracted to the North Area at LSS2 The extracted beam is transported in the TT20 tunnel 11% slope to arrive into TCC2 – then horizontal ; ~10m underground The primary proton beam is split in three parts directed towards to the North Area primary targets: T2, T4 and T6 11% slope The SPS North Area

9 Dec7,2007ie-FP7 Introduction The SPS North Area Beams The three proton beams are directed onto the primary targets: T2  H2 and H4 beam lines T4  H6, H8, and P0 beam lines T6  M2 beam line and Experimental Areas: ECN3: underground experimental hall, can receive the primary proton beam with high intensity in ECN3 EHN1: surface experimental hall, can receive secondary beams and/or attenuated primary proton beams EHN2: surface experimental hall, receives the secondary beams or intense muon beam The SPS North Area

10 Dec7,2007ie-FP7 Experimental Areas CMS CERF/SC- RP LHCb ATLAS TOTEM CALICE/ILC GLAST, DREAM, AMS,… ALICE CRYSTALS/LHC Coll. NA49 6.5 Km of beam lines About 1000 equipment installed The SPS North Area

11 Dec7,2007ie-FP7 User statistics The SPS North Area

12 Dec7,2007ie-FP7 The EHN1 beams The SPS North Area was originally designed to house long-lasting experiments demands for high quality of beams: high intensity, high energy, high resolution In the recent years most of the users are “tests” in particular of LHC detectors with permanent or “semi-permanent” BIG installations several users from astroparticle experiments The test users have very different requirements from the big experiments: scan the full energy range ; typically [10, 300] GeV/c with sometimes increased precision (linearity) requirements use beams of all particle types {electrons, pions, protons, muons} with as good as possible separation and identification and, sometimes request high (or very high) rates and all that during the few (or even one!) week(s) of their allocated time! Rapidly changing environment, quite demanding on beam conditions and tunes The SPS North Area

13 Dec7,2007ie-FP7 The EHN1 beams Target Beam Characteristics T2H2High-energy, high-resolution secondary beam. Alternatively can be used to transport: attenuated primary beam of protons, electrons from  -conversion, polarized protons for   decay, enriched low-intensity beam of anti-protons, or K + Main parameters: P max = 400 (450) GeV/c, Acc.=1.5  Sr,  p/p max = ±2.0 % H4High-energy, high-resolution secondary beam. Alternatively can be used to transport: primary protons, electrons from  - conversion, polarized protons for   decay, enriched low-intensity beam of anti-protons, or K + Main parameters: P max = 330 (450) GeV/c, Acc.=1.5  Sr,  p/p max = ±1.4 % T4H6High-energy secondary beam. Main parameters: P max = 203 GeV/c, Acc.= 2.0  Sr,  p/p max = ±1.5 % H8High-energy, high-resolution secondary beam. Alternatively can be used to transport an attenuated primary proton beam Main parameters: P max = 400(450) GeV/c, Acc.= 2.5  Sr,  p/p max = ±1.5 % The SPS North Area

14 Dec7,2007ie-FP7 Production rates Hadron beams Electron beams Particle production by 400 GeV/c protons on Be targets, H.W.Atherton et. al. The SPS North Area

15 Dec7,2007ie-FP7 Design Principle The momentum selection is done in the vertical plane “upstream” V-BENDs (B1, B2) between the primary target and the momentum acceptance collimator “downstream” V-BENDs (B3, B4) the main spectrometer of the beam momentum definition The SPS North Area

16 Dec7,2007ie-FP7 Design Principle View of the H8 and H6 beam lines in TT81 tunnel. The SPS North Area

17 Dec7,2007ie-FP7 Infrastructure What is (could be) provided Counting houses (barracks) with racks and network connections Beam instrumentation: Scintillator for beam intensity measurement XDWC for beam profile measurement Threshold Cherenkov counter for particle ID CEDAR counter for particle ID Electromagnetic calorimeter for particle ID Spectrometer for beam momentum measurement Scanning table (XSCA) Magnets - see slides later Cryogenics installation The SPS North Area

18 Dec7,2007ie-FP7 Experimental Areas https://edms.cern.ch/cdd/plsql/c4w.no_login?jump=FOLDER&p1=83193 The SPS North Area

19 Dec7,2007ie-FP7 Experimental Areas H6/H6A Area The SPS North Area

20 Dec7,2007ie-FP7 Experimental Areas H8/H8B Area The SPS North Area

21 Dec7,2007ie-FP7 Irradiation Facilities PS East Area : T7 line Primary proton beam from PS Up to 2-4 E11 protons / spill @ 24 GeV/c SPS North Area: CERF in H6 beam line : <1E8 ppp @120 GeV/c CERF++ in H4 beam line: <1E11 ppp @ {  400 GeV/c} Under construction GIF Presently “orphan” in West Area Plans to move it to EHN1: H4 or H6 beam lines

22 Dec7,2007ie-FP7 GIF++ In EHN1 H4/H4C The SPS North Area

23 Test beam magnets CERN-PH magnet stock (partly up-to-date): http://ph-dep-dt1.web.cern.ch/ph-dep-dt1/Organization/MM/Magnet-List- 2007.pdf See also: http://doc.cern.ch/archive/electronic/cern/preprints/open/open-2004-003.pdf Presently installed test beam magnets: PS east hall: –TPC-90 magnet (last used by HARP), solenoid diam. 90 cm, 224 cm long, 0.7 T (~1.3 T in pulsed mode). EHN1, H2 beam line: –M1 magnet, superconducting, large dipole, 82 cm gap, 1.4 m diameter, Field 3T,used by CMS –MNP22A, C-shaped classical dipole, 50 cm gap, 1 m width, 1 m depth, 1.37 T (presently 0.7 T)

24 CMS H2 test beam magnet 3T Helmholtz magnet beamB field http://ieeexplore.ieee.org/iel5/20/22845/01060951.pdf?tp=&isnumber=&arnumber=1060951

25 Test beam magnets Presently installed test beam magnets: EHN1, H4 beam line: –Goliath (last user NA57), large classical dipole, ~160*240*360 cm, 0.85 T field EHN1, H8 beam line: –Superconducting dipole, diam. 1.6 m, ~4 m overall length, 1.56 T field at 5000A, used by ATLAS, contains a rail system for inserting detectors


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