KEK Analysis Report Makoto Yoshida Osaka Univ. 2006/06/10 MICE CM15 Contents • Integration work towards G4MICE • Introduction to KEK beam test • We have two independent.
Download ReportTranscript KEK Analysis Report Makoto Yoshida Osaka Univ. 2006/06/10 MICE CM15 Contents • Integration work towards G4MICE • Introduction to KEK beam test • We have two independent.
KEK Analysis Report Makoto Yoshida Osaka Univ. 2006/06/10 MICE CM15 Contents • Integration work towards G4MICE • Introduction to KEK beam test • We have two independent analyses – Hideyuki’s – Aron’s in the framework of G4MICE KEK Beam Test • • • Schematic view of detectors KEK beam test was performed on located in the beam line September 30th to October 7th in 2006 at KEK-PS p2 beam line with the collaboration of UK, US, Europe and Japan. Main purpose is to confirm the performance of SciFi tracker in 1-Tesla solenoid field. Prototype SciFi tracker – SciFi tracker is consists of 4 stations, and there are 3 views for station B,D and 2 views for station A,C. VLPCs – Photon signals from Scintillating fiber were readout by VLPCs. – We used two VLPC cassettes. One of them has high gain and the other has low gain. – VLPCs were cooled down to 9K by a cryocooler. Prototype SciFi Tracker with 4 Stations Setup Readout System Before installing waveguides AFE Board P2 Beam Line JACEE MAGNET (B=1T) TOF hodoscope Cryocooler BEAM Low Gain High Gain Cassette Cassette Sci-Fi Prototype Prototype Tracker consisted of 4 stations. Stations B & D - 3 Views Stations A & C - 2 Views Readout - VLPCs, AFEII, Cryostat. X View V View W View Station D 2,500 ppm 2,500 ppm 5,000 ppm Station A mixture Station C 5,000 ppm 5,000 ppm Station B 5,000 ppm 2,500 ppm 3,500 ppm 5,000 ppm Event Selection • To ensure that a pion surely passes through SciFi tracker, PID by TOF of D1 and D2 counter are required. • Integration window in Trip chip is measured. Time difference from the beam trigger is restricted to reject events in which beam particles are not synchronized to Trip gate. TOF D1 SciFi STATION B STATION A D2 STATION C STATION D View alignment among stations D C BEAM 3 GeV/c p Station B View V Fiber # View X View W Residual A B View Alignment Station D View V Fiber # View X View W Residual Search for center fiber • In order to find combination of crossing of fibers of 3 views, adjustment is done by shifting X-view by same amount. – Down figure shows the results after shifting by -20 fibers. W view #101 V view #101 X view #81 Pitches for Station D • DATA shows fiber pitch is 420 mm on all stations • Inspection of 4th Station “D” confirmed 420 mm pitches. Difference of fiber# V View Red = 427 mm X View Black = 420 mm W View Fiber# MICEModel work in G4MICE • Representations of the model are produced for specific purposes (Simulation, Reconstruction, Visualisation…). • The Model allows us to have the same geometry for the Reconstruction of Data and Geant4 Simulation, so that they can be compared. • Configuration files have also been implemented, which list the material, location and orientation etc. of each module in the MICEModel (TOF, SciFi…) with respect to the other modules. G4MICE Status • The TOF Decoding, Cabling & calibration files & code have now been written and used in G4MICE. • Atsushi’s time walk corrections have been used and implemented into G4MICE. • The TOF Reconstruction code has now been produced including “TofSlabHits” & ”TofSpacePoints”. • VLPC decoding used is that from Osaka (jp map 12). • VLPC calibration used is that made by Malcolm in November 2005. • Common Mode Noise algorithm updated (use similar technique to that described by Hideyuki). • Clustering algorithm unchanged (2.0 PE total light in a cluster, neighbouring hits are summed). • Space point code now takes into account arbitrary rotations and misalignments (no longer requires trackers to be perpendicular to the Z axis!). • Track reconstruction used for this analysis not final one. MICEModel Set Up of KEK Test Beam TOF Hodoscope (Blue & Green Slabs) Pb Diffuser T1 & R1 Counters Solenoid (White) ACC MICEModel Set Up of KEK Test Beam T1 Counter R1 Counter Pb Diffuser ACC MICEModel Set Up of KEK Test Beam TOF Analysis 1 Black: 3 GeV/c Red: 325 MeV/c Blue: 250 MeV/c TOF Selection “High P” “Low P Electrons” “Low P Muons” Sci-Fi Summary 1/2 Low mom. m Low mom. e High mom. Station A Plane V 9.51 8.14 8.00 Station A Plane X 9.98 8.12 7.98 Station B Plane V 9.13 8.21 7.22 Station B Plane X 8.37 7.31 7.21 Station B Plane W 9.74 8.73 8.58 Station C Plane X 9.74 9.41 9.18 Station C Plane W 11.0 8.76 8.86 Station D Plane V 5.96 4.48 3.57 Station D Plane X 5.98 5.15 4.49 Station D Plane W 5.02 5.28 4.28 Light Yield –X view 8.0 0.2 10.2 0.2 8.9 0.3 4.7 0.2 15.0 0.4 18.6 0.4 8.5 0.6 Light Yield Summary Light Yield Light yield 3GeV/c 1GeV/c protons p- Ratio p/p- Station View Gain of cassette 3HF concent. B X LOW 5000 7.9 15.0 1.9 B V LOW 2500 8.6 15.6 1.8 B W LOW 3500 9.8 16.9 1.7 A X LOW 5000 10.3 18.6 1.8 A V LOW 5000 9.1 15.3 1.7 C X HIGH mixture 8.8 --- --- C W HIGH 5000 8.9 --- --- D X HIGH 2500 4.7 8.5 1.8 D V HIGH 2500 4.8 9.1 1.9 D W HIGH 5000 5.1 9.4 1.8 Beam Profile –MC and DATA Horizontal RMS (cm) Vertical RMS (cm) DATA 10.0 10.0 MC 10.0 10.0 Pt,Pz Distribution --MC Station @X view D C A B Pt (MeV/c) 28.5 (8.6) 29.0 (9.7) 29.4 (10.3) 29.4 (10.0) Pz (Mev/c) 227.2 (2.3) 226.8 (2.4) 226.4 (2.4) 225.9 (2.4) Momentum shift can be seen due to non-uniform magnetic field upstream Reconstructed Distri. --MC muon PT distribution MeV/c PZ distribution MeV/c Reconstructed mom. DATA MC Pt (MeV/c) 28.3 (10.3) 30.1 (10.3) Pz (Mev/c) 230.7 (26.7) 233.7 (19.7) Chi2 Distribution In this analysis, position resolution is assumed to be 1mm (should be 0.4mm) DATA MC Mean 2.8 Mean 1.8 RMS 2.3 RMS 1.6 DATA has little more broad distribution than MC. It could be caused by noise in DATA, mismatch of injected beam, … Summary • We have confirmed basic performance and capability to measure transverse / longitudinal momentum of low momentum muons. – Analysis on details are on the way to check two independent analyses • Analysis tools integrating TOF and other beam counters are implemented in G4MICE framework. • Test each stage of the Reconstruction (hits, clusters, points, tracks, matching) using the Geant4 simulation of test beam. • Test Reconstruction of real data (TOF & SciFi).