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Chris Smith California Institute of Technology EPS Conference 2003

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1 Chris Smith California Institute of Technology EPS Conference 2003
The MINOS Detectors Chris Smith California Institute of Technology EPS Conference 2003 Outline The MINOS Experiment Detector Technology Far, Near and Calibration Detector Detector Performance Summary

2 The MINOS Experiment Two Detector, long baseline, neutrino oscillation experiment: NuMI beam (Neutrinos at the Main Injector) Near Detector - on site at Fermilab Far Detector – 730km away in Soudan mine, Minnesota Calibration Detector – in a series of test-beams at CERN Oscillations lead to differences in Near-Far event rates, energy spectra Confirm Super-K result Measure parameters to 10% Near Far Chris Smith , Caltech

3 Detector Technology Iron/Scintillator tracking calorimeters
4.1 x 1cm scintillator strips, up to 8m long Extruded polystyrene (co-extruded TiO2 coating) PPO (1%), POPOP (0.03%) fluors Readout via wavelength shifting fibres Kuraray 1.2mm fibre (Y-11 fluor, 175 ppm) Hamamatsu Multi-anode PMTs Alternate planes rotated by  90o for 3D hits Near and Far detectors magnetised Chris Smith , Caltech

4 Far, Near and Calibration Detector
u v Detectors are designed to be as similar as possible Far: Large octagon, 5400 tons Near: Squashed octagon, 980 tons Calibration: Small section, 12 tons Chris Smith , Caltech

5 Near Detector - FNAL 241 planes in 4 sections:
Veto Target Hadron Shower Muon Spectrometer Planes already constructed at FNAL Beneficial occupancy in cavern from Dec 2003 Installation ~ 12 months Chris Smith , Caltech

6 Far Detector – Soudan 2 supermodules, 484 planes
Plane installation completed June 2nd Coil installed July Cosmic ray veto shield Unmanned running expected August Already taking CR and atmos n data Chris Smith , Caltech

7 Calibration Strategy MINOS designed for 2% relative (detector-detector) and 5% absolute energy calibration Light Injection System Electronics/PMT non-linearity PMT gain shift Cosmic ray muons Strip-to-strip normalisation Calibration Detector (CalDet) Characterise muon, electron and hadron responses Understand event topologies Test calibration procedures 1 month running at FarDet  1 hour at CalDet Chris Smith , Caltech

8 CalDet – CERN 1x1m cut-out section of larger MINOS detectors
60 planes x 24 strips for (x,y,z) Double-ended read-out Not magnetised T11 T7 3.6 GeV/c 10 GeV/c x 60 (3.7 m) 1m 24 strips Scintillator Steel 5.9 cm CalDet exposed to T7 and T11 beams at CERN PS in summer 2001, 2002 Provides e, m, p, p from 0.2 – 10 GeV Chris Smith , Caltech

9 Event Topologies at CalDet
Particle ID using TOF and Cerenkov detectors. 2 GeV topologies (single view): (Without Single PEs) Electron Pion Muon Proton Strip Plane Chris Smith , Caltech

10 Particle Response and Resolution
Preliminary results from CalDet agree well with predictions Response Resolution Hadrons 47 MIPs/GeV 55%/E Electrons 60 MIPs/GeV 22%/E MC expectation Chris Smith , Caltech

11 Timing Resolution at the Far Detector
Time Residuals for CR Muons Resolution determined by decay time of Y-11 fluor in WLS fibre ~8 ns Resolution measurement using down-going muons at Far Detector ~2.6 ns/plane Expect ~2.5 ns based on photoelectron statistics for muons Direction of muons can be determined with ~10 planes for contained vertex events To distinguish up and down through-going muons need ~20 planes  ~ 2.6 ns Time (ns) Chris Smith , Caltech

12 Light Output Factors affecting light at phototube include
Map of scintillator strip (Far Detector) Light Output Factors affecting light at phototube include Scintillator light output Path-length in strip Attenuation in WLS fibres Connector efficiency Apply corrections to infer response for perpendicular plane crossing (through 1cm scintillator) Observe ~8-10 PEs/strip for cosmic ray muons at surface Fit to a muon energy spectrum Chris Smith , Caltech

13 Candidate Neutrino Events at FarDet
Contained vertex atmospheric neutrino event? NO! CR muons entering between planes mimic atmospheric n events MINOS uses a double layer of scintillator to give  95% efficiency and to prevent gaps Strip vs Plane U view V view Y vs X y x z Chris Smith , Caltech

14 Candidate Neutrino Events at FarDet
Up-going muons produced by n interactions in Earth’s crust y Y vs X Y vs Z Strip vs Plane Time vs Y Time vs Z x z Example event: m+ p = 5.4GeV/c Expect ~450 up-going events in 5 year exposure of MINOS B field allows m charge to be measured up to ~100 GeV Chris Smith , Caltech

15 Summary Far Detector construction completed on schedule
Very successful installation CR and atmospheric neutrino data regularly being taken Data analysis underway Near Detector preparations underway Planes assembled on surface ready for installation Beneficial occupancy in cavern from December ‘03 CalDet data-taking and analysis has produced preliminary results Good agreement with predictions Test-beam run this summer will be used to compare Near and Far detector electronics MINOS is in good shape for NuMI beam in Dec ‘04! Chris Smith , Caltech


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