The Main Injector Particle Production experiment

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Presentation transcript:

The Main Injector Particle Production experiment Andrew Godley for the MIPP Collaboration: BNL, Colorado, EFI Fermilab, Harvard, IIT, Iowa, Indiana, Livermore, Michigan, South Carolina, Virginia Muon 07 UCLA January 2007

MIPP overview Measure particle production off various nuclei Incoming secondary beams of π±, K± and p± from 5 to 80 GeV/c or primary p beam from the Main Injector (120 GeV/c) Large acceptance spectrometer featuring a Time Projection Chamber Measure momentum of all charged particles produced Identify particles with dE/dx, ToF, differential and ring imaging Cerenkovs. A Godley, MIPP, Muon 07

The MIPP Spectrometer TPC PID: < 1 GeV/c DCKOV PID: 3-17 GeV/c TOF PID: 1-3 GeV/c JGG Analysing Magnet 0.7T RICH PID: 17-80 GeV/c Wire Chambers Rosie Analysing Magnet 0.6T Wire Chambers EMCAL Physicists HCAL A Godley, MIPP, Muon 07

MIPP Physics Particle Physics Nuclear physics Service measurements Non-perturbative QCD hadron dynamics, Particle fragmentation scaling laws (MIPP can test general scaling law in 36 reactions) Spectroscopy – Search for missing baryon resonances, glueballs Nuclear physics Y-scaling (Measure cross sections of hadrons on nucleons in the nuclear medium.) Propagation of strangeness through nuclei Service measurements Hadron shower models in Geant4, MARS,... Proton radiography, stockpile stewardship, national security applications Neutrino production (NuMI, T2K, MiniBooNE, atmospheric) n-factory A Godley, MIPP, Muon 07

Application to neutrino experiments Hadron production is largest uncertainty in neutrino flux prediction Existing hadron production data sparse Measure production from NuMI target Use event by event measurement as input to NuMI beam simulator (replace Fluka target) Also use to tune beam simulations and fits Thin C, Al and Be targets also measured – help simulate interactions downstream of the target Combine thin and thick target data to benchmark cascade calculations in thick targets Distribution of hadrons decaying to produce neutrinos at the MINOS far (top) and near detectors A Godley, MIPP, Muon 07

Data collected Ran throughout 2005 and first two months of 2006 5 thin targets Be, C, Al, Bi, U 7 million Liquid Hydrogen triggers 1.78 million triggers on the NuMI target 14 million triggers with no TPC (faster data rate) for Kaon mass measurement from RICH ring diameter First reconstruction pass completed – DST produced for analyses GeV/c A Godley, MIPP, Muon 07

Beam particle ID and trigger Tag incoming particle, use two upstream Cerenkov detectors >85% purity (tested with RICH) Can use beam TOF for 5 GeV/c (and lower) Added small scintillator trigger upstream of thin targets Combined with multiplicity in first drift chamber Purpose built scintillator trigger for NuMI target PRELIMINARY A Godley, MIPP, Muon 07

TPC Reconstruction From raw TPC data form clusters of hits in Z slices, then form tracks and the vertex TPC distortion effects: Inhomogeneous magnetic field causes drift electrons to deviate from path to readout Corrections applied using a measured magnetic field map Distortion effects now < 3mm A Godley, MIPP, Muon 07

Chamber Alignment First determine Drift Chamber time offsets Compute residual of track fits for each wire when it is NOT used in the fit, move plane (of wires) within 30% of this residual and iterate Then align chambers together using beam tracks that hit all 3 beam and 6 post target chambers, or secondary tracks that hit all 6 post target chambers Original alignment found problems in the survey and its implementation in our geometry and in the field maps – Corrected Average RMS of wire plane alignment is now ~60mm A Godley, MIPP, Muon 07

Tracking Basic procedure is to fit TPC tracks then match track candidates from chambers to these TPC tracks Improvements: Track merging (eliminate duplicates), included high angle tracks (needed for vertexing) Kalman filter based tracking also being developed for TPC and then global tracking TPC XZ TPC XY TPC YZ A Godley, MIPP, Muon 07

IN PROGRESS Particle ID - TPC TPC dE/dx already shows reasonable Pi/K/P separation Calibrate anode voltage and drift times Normalise dE/dx to minimum ionization level Continue improving dE/dx resolution Then extract Particle ID probabilities TPC dE/dx IN PROGRESS A Godley, MIPP, Muon 07

Particle ID – TOF and CKOV Calibrating delays of individual bars in TOF wall With rough timing and previous tracking can see proton band Calibration of CKOV light levels in progress v cm/ns IN PROGRESS P GeV Expected A Godley, MIPP, Muon 07

Particle ID - RICH ID by radius of cerenkov ring Beam Tracks ID by radius of cerenkov ring Ring finding and fitting algorithms complete Secondary Tracks A Godley, MIPP, Muon 07

Reconstruction Summary New deterministic annealing vertexing method improves vertex resolution Developing tracking with Kalman-filter based technique (RecPack) in parallel to current tracking efforts New DST production in a month to include these major improvements TPC, TOF and Differential Cerenkov PID continuing Full detector Monte Carlo almost complete Recreates different target and running conditions A Godley, MIPP, Muon 07

NuMI target data PRELIMINARY Beam aligned Δx=0.002 cm Δy=0.051 cm Total positive tracks, Pions and Kaons identified by the RICH PRELIMINARY A Godley, MIPP, Muon 07

Physics analyses in progess Target fragmentation multiplicities Hanbury Brown and Twist quantum interfence effect Charged kaon mass Soft pion production cross sections Proton and anti-proton production cross sections A Godley, MIPP, Muon 07

MIPP Upgrade - Hardware Hundred fold increase in data taking rate – record 5 million events per day from limited beam (spill every 2 minutes) TPC readout electronics limit data taking (30Hz)– use ALICE ALTRO chips JGG coil replacement New silicon pixel trigger (B-TeV design) with veto New chamber electronics New TOF/CKOV readout eletronics (TripT chip) New Recoil detector DAQ upgrade Beamline optics and shielding – run with 1 to 85 GeV/c beam A Godley, MIPP, Muon 07

MIPP Upgrade - Physics More MINOS target statistics, NOvA target and others (MiniBooNE, T2K) Pi and K production cross sections on liquid nitrogen for atmospheric neutrino or cosmic ray experiments Larger list of targets: H2, D2, Li, Be, B, C, N2, O2, Mg, Al, Si, P, S, Ar, K, Ca, Fe, Ni, Cu, Zn, Nb, Ag, Sn, W, Pt, Au, Hg, Pb, Bi, U Target area to be reengineered – can accommodate any unusual target system – but need details soon ILC - Tagged neutral beams and higher statistics for hadron shower simulations ILC calorimeters need to achieve 30%/√E – current shower simulators are in a poor state (see HSSW06) Limiting factor is manpower, new collaborators welcome! A Godley, MIPP, Muon 07

Summary MIPP collected 17 million events that will address a broad range of physics Reconstruction is being finalised, preliminary analysis results expected throughout the summer Upgrade work is ongoing. Most of the new electronics is designed. Encouragement from Fermilab management for the upgrade but our proposal needs more support to be approved The upgrade will allow MIPP to drastically improve its statistics of complete particle coverage events Current plan is to start commissioning run in Q1 2008 New collaborators most welcome – opportunities to have specific NFMC targetry data taken Excellent training for students and postdocs A Godley, MIPP, Muon 07