Read-out set-up and test results

Slides:



Advertisements
Similar presentations
Time over Threshold Electronics for Neutrino Telescopy George Bourlis + multiplicity.
Advertisements

A crude (lower limit) estimation of resolution and event rate Development and Construction of an Extensive Air Shower Array in HOU Antonis Leisos, Hellenic.
The PEPPo e - & e + polarization measurements E. Fanchini On behalf of the PEPPo collaboration POSIPOL 2012 Zeuthen 4-6 September E. Fanchini -Posipol.
Proposal for read-out of Forward Detector straw tubes PANDA DAT requirements General layout Prototypes M. Idzik, M. Kajetanowicz, K.Korcyl, G. Korcyl,
MR (7/7/05) T2K electronics Beam structure ~ 8 (9?) bunches / spill bunch width ~ 60 nsec bunch separation ~ 600 nsec spill duration ~ 5  sec Time between.
LHCC, V0, Sept The V0 detector (Mexico Lyon collaboration)  Segmentation  Simulated performances secondaries / beam-gas  Counters design 1 /
Straw spatial resolution (beam test 2007 and 2008) A.Zinchenko, S.Shkarovskiy.
Feb 10, 2005 S. Kahn -- Pid Detectors in G4MicePage 1 Pid Detector Implementation in G4Mice Steve Kahn Brookhaven National Lab 10 Feb 2005.
Aras Papadelis, OTR meeting NIKHEF, June 17 th LHCb Outer Tracker Cross-talk measurements with Fe-55.
TRD R&D at GSI  Results from test beam 2004  Plans for test beam Feb. 06  Measurements with X-ray stand C. Garabatos, GSI.
Muon Detector Jiawen ZHANG Introduction The Detector Choices Simulation The structure and detector design The Expected performance Schedule.
Status of Beam loss Monitoring on CTF3 Results of Tests on LINAC and PETS as R&D for TBL Anne Dabrowski Northwestern University Thibaut Lefevre CERN CTF3.
Electromagnetic Calorimeter for HADES at SIS100: MAMI and CERN test results Lead-glass modules Tests -  beam at MAMI energy resolution -  - /e - beam.
Self triggered readout of GEM in CBM J. Saini VECC, Kolkata.
TPC R&D status in Japan T. Isobe, H. Hamagaki, K. Ozawa, and M. Inuzuka Center for Nuclear Study, University of Tokyo Contents 1.Development of a prototype.
Mitglied der Helmholtz-Gemeinschaft Calibration of the COSY-TOF STT & pp Elastic Analysis Sedigheh Jowzaee IKP Group Talk 11 July 2013.
The DHCAL Data Analysis José Repond CALICE Meeting, Prague, September 10 – 12, 2007.
Mariana Petris, NIPNE Bucharest CBM Meeting, March 9 -12, 2005 HIGH COUNTING RATE TRANSITION RADIATION DETECTOR Bucharest Prototype In Beam Tests.
PMT Readout and Floor Triggering Charge estimation using the times over the thresholds Event Building and Triggering + multiplicity George Bourlis.
RPC upgrade for the HADES Tracking: MDC e -,e + identification with RICH- TOF/PreShower  0.4 GeV/c TOF is not sufficient- Pre-Shower p,  identification.
PNPI, R&D MUCH related activity ● Segmentation ● Simulation of the neutral background influence ● R&D of the detectors for MUCH ● Preparation to the beam.
Test beam preliminary results D. Di Filippo, P. Massarotti, T. Spadaro.
Test of Electromagnetic Calorimeter modules for HADES, Mainz Sep.2009 A.Krása, F. Křížek, J. Pietraszko, Y. Sobolev, J. Stanislav, A. Reshetin, P. Tlustý.
Beam Test of a Large-Area GEM Detector Prototype for the Upgrade of the CMS Muon Endcap System Vallary Bhopatkar M. Hohlmann, M. Phipps, J. Twigger, A.
The BoNuS Detector: A Radial Time Projection Chamber for tracking Spectator Protons Howard Fenker, Jefferson Lab This work was partially supported by DOE.
Proton Test Beam Experimental Program Overall objective: Study response of modified monochrome DC Plasma Display Panels to low energy proton beam. Energy.
1 First Results of the SLD Cerenkov Polarimeter at the DESY test beam Oleg Eyser Daniela K äfer, Christian Helebrant, Jenny List, Ulrich Velte*
NUMI NUMI/MINOS Status J. Musser for the MINOS Collatoration 2002 FNAL Users Meeting.
MuTr Chamber properties K.Shoji Kyoto Univ.. Measurement of MuTr raw signal Use oscilloscope & LabView Read 1 strip HV 1850V Gas mixture Ar:CO 2 :CF 4.
Mitglied der Helmholtz-Gemeinschaft STT News & Status Peter Wintz (FZ Jülich) for the STT group LII. PANDA CM Giessen, TRK session, Mar-18 th, 2015.
FEE for Muon System (Range System) Status & Plans G.Alexeev on behalf of Dubna group Turin, 16 June, 2009.
STT read-out concepts Detectors requirements and layout Read-out concepts Developments of Analog FE and Digital Boards STS el. group : INFN, FZ Juelich,
HADRON 2009, FloridaAnar Rustamov, GSI Darmstadt, Germany 1 Inclusive meson production at 3.5 GeV pp collisions with the HADES spectrometer Anar Rustamov.
Beam detectors in Au+Au run and future developments - Results of Aug 2012 Au+Au test – radiation damage - scCVD diamond detector with strip metalization.
0 Characterization studies of the detector modules for the CBM Silicon Tracking System J.Heuser 1, V.Kyva 2, H.Malygina 2,3, I.Panasenko 2 V.Pugatch 2,
FWD Meeting, Torino, June 16th, News from Cracow on the forward tracking J. Smyrski Institute of Physics UJ Tests of CARIOCA and LUMICAL preamplifiers.
1 The Scintillation Tile Hodoscope (SciTil) ● Motivation ● Event timing/ event building/ software trigger ● Conversion detection ● Charged particle TOF.
1 straw tube signal simulation A. Rotondi PANDA meeting, Stockolm 15 June 2010.
PreShower Characterisations
Fabio, Francesco, Francesco and Nicola INFN and University Bari
Detector status and commissioning: LUCID
Beam detectors performance during the Au+Au runs in HADES
Activities on straw tube simulation
S.Movchan Straw prototype beam test into the NA48 infrastructure
on behalf of the AGH and UJ PANDA groups
Performance of timing-RPC prototypes with relativistic heavy ions
Entrance Muon Counter (EMC)
DHCAL TECH PROTO READOUT PROPOSAL
IFR Status Summary W. Baldini on behalf of the IFR Group
Alternative FEE electronics for FIT.
Update on Noise Analysis of the DHCal Test Beam at Fermilab
STT Status & News Peter Wintz (FZ Jülich) for the STT group
STT Status Update Peter Wintz (FZ Jülich) for the STT group
HV-CMOS Update The properties device (HVStripV1) we just Birmingham
Preliminary Performance of the L2 Chamber (Side A)
PADI for straw tube readout and diamonds for MIPs and for high precision tracking beam test – Jülich, Feb Jerzy Pietraszko, Michael Träger, Mircea.
First Look at Modeling Photoelectron Energy Distribution for a 2
Analysis of FADC single-crystal data
Results from a preliminary analysis of the MWPC test at the GIF
SuperB LNF meeting March 21st 2012 Marcello Piccolo
Pulse Shape Fitting Beam Test September, October CERN
CMS ECAL Calibration and Test Beam Results
Hellenic Open University
Conceptual design of TOF and beam test results
Use of Beam Loss Monitor type detectors in CNGS muon station
On behalf of CEPC calorimeter working group
Времяпролетный детектор PANDA
High Rate Photon Irradiation Test with an 8-Plane TRT Sector Prototype
Update on SoLID-TOF Wang Yi Outline: Conceptual design of SoLID-TOF
Beam Tests data vs Matlab simulations
Presentation transcript:

Read-out set-up and test results P. Salabura on behalf of Kraków crew

Read-out scheme Prototype I (july 2011) in tests TRB v2 128 channels HPTDC Evaluation board

ASIC interface ASIC setting for in-beam and radioactive source tests in 2012/2013 selected: rising time ~40 ns,pulse duration ~ 150 ns stable operation with tubes (no oscilations) Installed in Kraków, Juelich Installed also at GSI with HADES MDC- comparison to AD8 – on going Fe signal

Examples of signal: Fe-source Preamp- saturation Typical signal Asic setting: reduce Pramp gain (1.) to eliminate preamp-saturation

Event Display (new-since 2 weeks)

Plateau measurements ‘ 2013 Kraków straws January 2013

TOT vs charge characteristics: Fe source Q/Q~11% Q/Q~9% Total charge ~ few percent resolution below 1875 V: for higher HV resolution degradation due to Preamp saturation TOT vs charge dependence : typical shape for quasi-Gaussian pulses

TOT vs Tdrift -0.9 GeV protons September’ 2012 Juelich Simulation: Garfield + FEE transfer 1 GeV/c miuons 130 ns TOT [ns] Tdrift [ns] as expected besides second leg structure in TDrift>130 ns !!! ? pile-up due to micro bunch structure of the beam? – I doubt it – see next slides secondary emission from tube walls? electronic effects : cross talk (we could not find evidence for that)

TOT vs Tdrift vs HV (900 MeV/c protons) 1700 V 1750 V 1800 V T~130 ns time direction reversed separation between 2 structures increases with HV

Sr90 vs in- beam measurement same set-ups : 2 rows of straws aligned w.r.t beam Trigger : and between 2 scint. (in Krakow we use similar straws)

Spectra from one straw Juelich: p 900 MeV HV=1800 V Kraków: Sr90 HV=1800 V Tot [ns] Tdrift [ns] Tdrift [ns] several (>8) straws fired At least 5 straws fired + 2 scintil. similar second leg structure visible in sr90 case Sr90: can not be due to pile-up

Spectra from one straw when 2’d fired Juelich: p 900 MeV second straw in the same row Kraków: sr90 second straw in the same row second straw in the row below second straw in the row below

Correlation plots Juelich: p 900 MeV second straw in the row below Tdrift j+1 Kraków: Sr90 second straw in the row below Tdrift j j j+2 j+1

Further source tests are needed to understand origing of delayed signals in straw (Gas, mixtures, HV dependence, ASIC settings?) will be continued in Kraków Test at GSI with MDC . FEE + TRB installed . ASIC adopted to MDC signals (faster rising and larger gain) TOT / Charge / position resolution from in-beam data– see Jacek talk