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The NA61 TPCs (1) Overview: Mechanics readout Position resolution
principle Mechanics readout Position resolution Particle identification Calibration
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Rainer Renfordt, IKF The NA61 TPCs
Rainer Renfordt, IKF The NA61 TPCs
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Rainer Renfordt, IKF The NA61 TPCs
Rainer Renfordt, IKF The NA61 TPCs
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Working principle of a TPC
Voltage divider Field cage R High voltage electrode (negative) Driftgas Magnetic Field (measure particle momentum) Electric field (elctron drift) Multiwire proportional chamber (0V) Rainer Renfordt, IKF The NA61 TPCs
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Signal generation in a multiwire proportional chamber with pad readout
Rainer Renfordt, IKF The NA61 TPCs
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Rainer Renfordt, IKF The NA61 TPCs
Signals of one pad after digitization and zero suppression (NA49 online monitor) Drift time of electron cloud Amplitude (ADC counts) Rainer Renfordt, IKF The NA61 TPCs
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Rainer Renfordt, IKF The NA61 TPCs
The gating grid prevents positive ions from drifting back into drift volume: space charge distortions prevents electrons from entering the amplification region: ageing Garfield calculation of field lines Rainer Renfordt, IKF The NA61 TPCs
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Rainer Renfordt, IKF The NA61 TPCs
The gating grid Different way of presentation: drift lines of electrons/ions Garfield calculation for OROC chambers of ALICE (no field wires → larger signals on pads) Rainer Renfordt, IKF The NA61 TPCs
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Rainer Renfordt, IKF The NA61 TPCs
Gating grid pulser Principle of operation: Badly tuned pulser causes noise in the first couple of time bins ONE THING TO BE CHECKED BY SHIFT CREWS! Rainer Renfordt, IKF The NA61 TPCs
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Rainer Renfordt, IKF The NA61 TPCs
Ageing effects Rainer Renfordt, IKF The NA61 TPCs
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Rainer Renfordt, IKF The NA61 TPCs
Construction of the VTPCs This design allows very light construction: multiple scattering is minimized Rainer Renfordt, IKF The NA61 TPCs
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Rainer Renfordt, IKF The NA61 TPCs
VTPC: looking along the beam direction field cage is split in two halfs, the beam area is outside the field cage Rainer Renfordt, IKF The NA61 TPCs
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Rainer Renfordt, IKF The NA61 TPCs
MTPC field cage Rainer Renfordt, IKF The NA61 TPCs
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Rainer Renfordt, IKF The NA61 TPCs
Inside the MTPC Rainer Renfordt, IKF The NA61 TPCs
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Rainer Renfordt, IKF The NA61 TPCs
MTPC chambers are first inserted through the opening,then pulled back sealing with O-ring Rainer Renfordt, IKF The NA61 TPCs
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Rainer Renfordt, IKF The NA61 TPCs
VTPC chambers are inserted from top and sealed with RTV (silicone) Chamber body Support frame (end plate) Rainer Renfordt, IKF The NA61 TPCs
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Rainer Renfordt, IKF The NA61 TPCs
TPC readout Rainer Renfordt, IKF The NA61 TPCs
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Rainer Renfordt, IKF The NA61 TPCs
Rainer Renfordt, IKF The NA61 TPCs
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Rainer Renfordt, IKF The NA61 TPCs
From Zoltan: Rainer Renfordt, IKF The NA61 TPCs
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Rainer Renfordt, IKF The NA61 TPCs
From Andras: Rainer Renfordt, IKF The NA61 TPCs
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Rainer Renfordt, IKF The NA61 TPCs
motherboard Concentrator board Rainer Renfordt, IKF The NA61 TPCs
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Rainer Renfordt, IKF The NA61 TPCs
Rainer Renfordt, IKF The NA61 TPCs
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Rainer Renfordt, IKF The NA61 TPCs
Rainer Renfordt, IKF The NA61 TPCs
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Rainer Renfordt, IKF The NA61 TPCs
Rainer Renfordt, IKF The NA61 TPCs
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Rainer Renfordt, IKF The NA61 TPCs
Digitized signal of one pad (with zero suppression) Rainer Renfordt, IKF The NA61 TPCs
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Rainer Renfordt, IKF The NA61 TPCs
Resolution issues: position resolution Important for momentum (vector) determination: curvature in magnetic field emission angle Rainer Renfordt, IKF The NA61 TPCs
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Position resolution (pad direction) as fu of drift length (MTPC)
Diff & gas gain fluct & pad size & electr. Noise & threshold measurement Diffusion & gas gain fluct 2 x Diffusion Diffusion only Rainer Renfordt, IKF The NA61 TPCs
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Rainer Renfordt, IKF The NA61 TPCs
Rainer Renfordt, IKF The NA61 TPCs
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Rainer Renfordt, IKF The NA61 TPCs
Optimization of pad angles: track angle relative to beam direction at center of VTPC2 π- from Lambda P from Lambda Angle (rad) All neg tracks All pos tracks Final pad angle RMS X (pad direction [cm] Rainer Renfordt, IKF The NA61 TPCs
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Rainer Renfordt, IKF The NA61 TPCs
Effect of track angle L projection δx ~ L*σ *tanα/√Neff Neff ~ 12/cm (not 40) centroid Rainer Renfordt, IKF The NA61 TPCs
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Rainer Renfordt, IKF The NA61 TPCs
Position resolution as function of track angle Sectors 4 - 6 Sectors 1 - 3 Rainer Renfordt, IKF The NA61 TPCs
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Rainer Renfordt, IKF The NA61 TPCs
Effect of Lorentz angle at wire on cluster width and resolution asymmetric relative to beam direction, i.e. Positive and negatice particles Rainer Renfordt, IKF The NA61 TPCs
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Rainer Renfordt, IKF The NA61 TPCs
to be continued Rainer Renfordt, IKF The NA61 TPCs
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