A. Calcaterra, R. de Sangro, G. Felici, G. Finocchiaro, P. Patteri, M. Piccolo INFN LNF XIV SuperB General Meeting DCH-I parallel session LNF, 27 September.

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Presentation transcript:

A. Calcaterra, R. de Sangro, G. Felici, G. Finocchiaro, P. Patteri, M. Piccolo INFN LNF XIV SuperB General Meeting DCH-I parallel session LNF, 27 September 2010

Experimental Setup 27/09/20102G. Finocchiaro Prototype 1  6x4 hexagonal cells à la B A B AR – Guard wires to ensure uniformity of electric field among cells – Aluminized mylar windows on entrance-exit faces – small gas volume low rate on cosmics fast gas mixture switching times LST Telescope:  Two identical assemblies of 26 tubes each  3 cm diameter, 100 μm wires  40%-60% Ar-iC 4 H 10 mixture

Tracks reconstructed in the telescope 27/09/20103G. Finocchiaro Al-Mylar windows 10cm lead p cut ~150MeV/c

Space-time relations Measured time vs. extrapolated impact parameter – t vs. R Impact parameter vs. time – R vs. t 27/09/2010G. Finocchiaro4 Example: 60%He-40%C 2 H HV=2010V

Space-time relations fits Fit R vs. t relation using Chebyshev polynomials of order (up to) 5 Time range rescaled to [-1,+1] interval 27/09/2010G. Finocchiaro5 60%He-40%C 2 H 6 HV=2010V

Drift velocity 27/09/2010G. Finocchiaro6 60%He-40%C 2 H 6 HV=2010V

LEFT RIGTH L+R Space-time relations fits (cont.) Internal cells tend to be left-right symmetric 27/09/2010G. Finocchiaro7 Column Row %He-40%C 2 H 6 HV=2010V

LEFT RIGTH L+R Space-time relations fits (cont.) Border cells show some asymmetry 27/09/2010G. Finocchiaro8 Column Row %He-40%C 2 H 6 HV=2010V

Track fit residuals Fit X slices with Gaussian + pol0 27/09/2010G. Finocchiaro9

Spatial resolution – 60%He-40%C 2 H 6 27/09/201010G. Finocchiaro 60%He-40%C 2 H 6 HV=2010V

Tracks reconstructed in Proto1 27/09/201011G. Finocchiaro Al-Mylar windows 10cm lead p cut ~150MeV/c BLUE line is MT track RED line is PROTO1 track

Spatial Resolution form Proto1 tracks 27/09/201012G. Finocchiaro 60%He-40%C 2 H 6 HV=2010V Studied layer excluded from track fit in prototype Preliminary: still need to work out fine details (tails, de- convolution of track resolution… )

STR & Spatial resolution – 73%He- 27%C 2 H 6 27/09/201013G. Finocchiaro 73%He-27%C 2 H 6 HV=1910V

STR & Spatial resolution – 80%He- 20%C 2 H 6 27/09/201014G. Finocchiaro 80%He-20%C 2 H 6 HV=1860V

Gas Mixture Comparison 27/09/2010G. Finocchiaro15  (g/cm 3 ) x1 0 4 X0(m)N P (cm  )N T (cm  )t max (ns)  (  m) 80%He-20%iC 4 H %He-10%iC 4 H %He- 5%iC 4 H %He-65%CH %He-49%CH %He-33%CH %He-21%CH %He-40%C 2 H %He-27%C 2 H %He-21%C 2 H t max and space resolution depend on other parameters. Figures shown are preliminary and indicative Results for iC 4 H 10 and CH 4 –based gas mixtures to be updated with analysis software used for C 2 H 6 gases

Read 3 channels of proto1 through DRS4 (*) “evaluation board” Channel arrangement chosen to see cosmic ray tracks Same channels (after active splitters) as in the standard DAQ chain Waveform Digitization & Cluster Counting 27/09/2010G. Finocchiaro16 (*) A switched capacitor array (SCA) with 1024 cells, capable of digitizing eight analog signals with high speed (6 GSPS) and high accuracy (11.5 bit SNR) on a single chip ( [only 4 channels read-out with current version of firmware] Same acquisition trigger (scintillator counters coincidence) as telescope+proto1 setup shown so far −Proto1 preamp bandwidth <100 MHz −Channel #1 of DRS4 board connected to drift tube with faster preamplifier (see next slides)

Drift Tubes for Cluster Counting Two square-section tubes (24mm side) built to study cluster counting issues in simplified environment. The anode - as in Proto1 - is a 20  m Tungsten wire. One tube (400mm long) already equipped with 300MHz bandwidth preamplifier – Gain ~5mV/fC; noise ~1900 e  RMS 27/09/2010G. Finocchiaro17

Drift Tubes for Cluster Counting 400mm long tube currently on top of our setup Dump the four waveforms when at least one of them exceeds 25mV 27/09/2010G. Finocchiaro18 In spite of x3.5 higher preamp bandwidth, a noise level similar to proto1 (~1.4 mV RMS) is obtained with a careful shielding (…)

Drift Tubes for Cluster Counting (cont.) Adequate preamp bandwidth is (clearly) crucial to count clusters 27/09/2010G. Finocchiaro19 85%He-15%C 2 H 6 n P =10.2/cm

Counting Clusters 27/09/2010G. Finocchiaro20 INPUT SIGNAL 1024 channels, 2Gsample/sec TARGET SIGNAL (cluster) Position of peaks from finding algorithm

More Detectors for Counting Clusters 27/09/2010G. Finocchiaro mm long tube to study signal propagation along the wire – built, strung and tested for gas tightness – in the gas flow circuit and with HV on for some days now – to be equipped with fast preamp soon 2000 mm long square cell prototype (~20 cells) for realistic study (X-talk, undetected clusters, signal propagation…) being designed – hope to have it in hand early 2011

Summary More He-based mixtures, using ethane as quencher, have been analyzed. – preliminary v drift and spatial resolution results show good performance – Methane still seems best candidate for light, fast mixtures (short readout time window to reduce background) Very first attempts at identifying clusters in (almost) realistic conditions – need fast preamps, low noise, low n P mixtures, good control of track length 27/09/2010G. Finocchiaro22