THE USER “POINT OF VIEW” ABOUT THE VFAT2 The first day.... The first week.... The first month.... The first year... But at the end you will be a friend.

Slides:



Advertisements
Similar presentations
Kondo GNANVO Florida Institute of Technology, Melbourne FL.
Advertisements

Specific requirements for analog electronics of a high counting rate TRD Vasile Catanescu NIHAM - Bucharest CBM 10th Collaboration Meeting Sept 25 – 28,
CMS ECAL Laser Monitoring System Toyoko J. Orimoto, California Institute of Technology, on behalf of the CMS ECAL Group High-resolution, high-granularity.
28 August 2002Paul Dauncey1 Readout electronics for the CALICE ECAL and tile HCAL Paul Dauncey Imperial College, University of London, UK For the CALICE-UK.
6 June 2002UK/HCAL common issues1 Paul Dauncey Imperial College Outline: UK commitments Trigger issues DAQ issues Readout electronics issues Many more.
Slide 1 sCVD Diamond for the CMS Pixel Detector May 2004 R.Stone, Rutgers J.Doroshenko, L.Perera, S.Schnetzer RD42 Collaboration Meeting Overview.
Luminosity Monitors MICE Video Conference 7 May 2009 Paul Soler.
Saverio Minutoli INFN Genova 1 T1 Electronic status Electronic items involved: Anode Front End Card Cathode Front End Card Read-Out Control card Slow Control.
2012 IEEE Nuclear Science Symposium Anaheim, California S. Colafranceschi (CERN) and M. Hohlmann (Florida Institute of Technology) (for the CMS GEM Collaboration)
The PEPPo e - & e + polarization measurements E. Fanchini On behalf of the PEPPo collaboration POSIPOL 2012 Zeuthen 4-6 September E. Fanchini -Posipol.
Chamber parameters that we can modify and that affect the rising time Number of ionisation clusters produced in the drift gap: Poisson Distribution Probability.
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.
TURBO: VFAT CTRL/READOUT BOARD INVOLVED PEOPLE TOTEM(Pisa/Siena group and students), GDD-RD51(Matteo, Gabriele), CMS GEM upgrade group (Andrey, Stefano,
CONTROL SOFTWARE On December 11th 2006 By Juha Petäjäjärvi On December 11th 2006 By Juha Petäjäjärvi.
My working experience Marco Villa Tue, 2 nd Dec 2008.
TTP Related SW December 4th 2007 Juha Petäjäjärvi December 4th 2007 Juha Petäjäjärvi Totem Test Platform.
GEM R&D Update Kondo Gnanvo. Outline  GEM R&D and assembly facilities at UVa  Cosmic test results  Update on the 40 × 50 cm 2 GEM prototype  Plans.
Performance of a Large-Area GEM Detector Prototype for the Upgrade of the CMS Muon Endcap System Vallary Bhopatkar M. Hohlmann, M. Phipps, J. Twigger,
January 31, MICE DAQ MICE and ISIS Introduction MICE Detector Front End Electronics Software and MICE DAQ Architecture MICE Triggers Status and Schedule.
News on GEM Readout with the SRS, DATE & AMORE
Update on the Triple GEM Detectors for Muon Tomography K. Gnanvo, M. Hohlmann, L. Grasso, A. Quintero Florida Institute of Technology, Melbourne, FL.
We really need to check all the results showed. We change the GEM from the fully-well-shielded to the less shielded one (top- bottom-fan out with aluminum)
LC Power Distribution & Pulsing Workshop, May 2011 Super-ALTRO Demonstrator Test Results LC Power Distribution & Pulsing Workshop, May nd November.
B.Satyanarayana Department of High Energy Physics Tata Institute of Fundamental Research Homi Bhabha Road, Colaba, Mumbai,
11 October 2002Paul Dauncey - CDR Introduction1 CDR Introduction and Overview Paul Dauncey Imperial College London.
TEMPLATE DESIGN © CONFIG. 1: 12mm(Drift) / 12mm(T1) / 12mm(T2) / 12mm(Induction) CMS Endcap Resistive Plate Chamber Muon.
BPM stripline acquisition in CLEX Sébastien Vilalte.
Status and organization of the H8c area Mirko Berretti 08/07/2015 (with M.Bozzo, N.Minafra, E.Oliveri, X. Pons…)
RD51 GEM Telescope: results from June 2010 test beam and work in progress Matteo Alfonsi on behalf of CERN GDD group and Siena/PISA INFN group.
CMS Binary Chip (CBC): status and development D.Braga, L.Jones, P.Murray, M.Prydderch (RAL) G.Hall, M.Pesaresi, M.Raymond (IC) CMS Upgrade Week, FNAL,
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.
SDHCAL. outline  SDHCAL concept, validation and construction  Test Beam and technological prototype performance  Perspectives and Conclusion  SDHCAL.
Large GEM test beam November 2012 C. Armaingaud, J. Merlin, S. Colafranceschi, A. Marinov Y. Maghrbi, P. Barria, S. Salva.
Update on works with SiPMs at Pisa Matteo Morrocchi.
SKIROC status CERN – CALICE/EUDET electronic & DAQ meeting – 22/03/2007 Presented by Julien Fleury.
TRIPLEGEM and VFATs at The Test Beam Area TRIPLEGEM and VFATs at The Test Beam Area N. Turini……reporter Eraldo Oliveri! Eraldo Oliveri main worker! N.
Trigger & Tracking detector for CMS
Understanding of SKIROC performance T. Frisson (LAL) On behalf of the SiW ECAL team Special thanks to the electronic and DAQ experts: Stéphane Callier,
Slow Control and Run Initialization Byte-wise Environment
Results with the RPC system of OPERA and perspectives
Slow Control and Run Initialization Byte-wise Environment
Budker INP V.Aulchenko1,2, L.Shekhtman1,2, V.Zhulanov1,2
Use of a Diamond BLM System in the LHC Ring
OMEGA3 & COOP The New Pixel Detector of WA97
The timing upgrade project of the TOTEM Roman Pot detectors
Fabio, Francesco, Francesco and Nicola INFN and University Bari
LHC1 & COOP September 1995 Report
TOTEM Collaboration Meeting June 2007
High-Resolution Micromegas Telescope for Pion- and Muon-Tracking
Use of a Diamond BLM System in the LHC Ring
Marcin Chrząszcz Cracow University of Technology Itamar Levy
Saikat Biswas, A. Abuhoza, U. Frankenfeld, C. Garabatos,
PADME L0 Trigger Processor
MPGD Detectors and Electronics at CIAE
Setup for measurements with SCT128 in Ljubljana: SCTA128VG chip
Igor Mandić1, Vladimir Cindro1, Gregor Kramberger1 and Marko Mikuž1,2
The digital read-out for the CSC system of the TOTEM experiment at LHC
The Pixel Hybrid Photon Detectors of the LHCb RICH
University of California Los Angeles
TPC electronics Atsushi Taketani
The digital read-out for the CSC system of the TOTEM experiment at LHC
SKIROC status CERN – CALICE/EUDET electronic & DAQ meeting – 22/03/2007 Presented by Julien Fleury.
Pre-installation Tests of the LHCb Muon Chambers
Jean-Francois Genat – Herve Grabas Mary Heinz – Eric Oberla
Peter Kodyš, Zdeněk Doležal, Jan Brož,
ASPID (Application of Silicon Photomultipliers to Imaging Detectors)
Front-end Electronics for the LHCb Preshower Rémi CORNAT, Gérard BOHNER, Olivier DESCHAMPS, Jacques LECOQ, Pascal PERRET LPC Clermont-Ferrand.
Setup for testing LHCb Inner Tracker Modules
CLAS 12 Status of the test bench Calculation of the time resolution
Igor Mandić1, Vladimir Cindro1, Gregor Kramberger1 and Marko Mikuž1,2
Presentation transcript:

THE USER “POINT OF VIEW” ABOUT THE VFAT2 The first day.... The first week.... The first month.... The first year... But at the end you will be a friend of the v FAT 2 ! But at the end you will be a friend of the v FAT 2 ! Dear Paul, this is obviously a joke. Please, apologize me.

Some consideration about measurements and scans with the VFAT2. All the measurements shown are referred to TOTEM Triple GEM or RD51 test beam Triple GEM E. Oliveri I.N.F.N. Pisa – University of Siena RD51 4 th Collaboration Meeting, CERN

Threshold Scan. GLUED GEM CMS GEM Shielded GLUED GEM Threshold scan results for a quarter of T2 (10 Triple GEM) Threshold scan for one channels of three triple GEM Acquired during the RD51 test beam. The scan is performed changing automatically the threshold for each acquisition step and the results give you a fast information about your noise condition in all the channels of the vfats.

Calibration Pulse Scan. The scan is performed changing automatically the charge injected by the calibration pulse. This measurement can be performed only on few channel per scan, but the result is very precise and it can show you for example the correlation with the capacitance of the readout electrode.

Latency Scan ( with Beam or with the internal calibration pulse). The scan is performed changing automatically the latency fo the vaft (i.e. the memory cell read when a trigger is sent to the VFAT2). (0.4cm (transfer gap)) / (5cm/us)-(0.4cm) / (7cm/us)~ 80ns- 57ns~25ns Considering the different gains and VFAT internal synchronization, this is compatible with the measurement. 50ns Ar/CO2 70/30 Ar/CO2 90/10 One example from the RD51 Test Beam: This scan (performed with beam) is necessary to define the right latency that you have to wrote on the VFAT2 register, but it is also useful to get timing information. Ar/CO2 3.5kV/cm vdrift 7 cm/us Ar/CO2 3kV/cm vdrift 5 cm/us

Playing with threshold and monostable polarity is like playing with your scope with trigger level (thresh.) and negative or positive slope (monost. Pol.)......and if you use them properly you could get information about your signal (the duration is one example) trigger level Neg/Pos Slope Latency scan performed during the RD51 test beam on two Triple GEM in Ar/CO2 70/30 (yellow) and ArCO2 90/10 (orange) respectively. VFAT2 Threshold and Monostable Polarity idem for positive threshold POSITIVE POLARITY: ENDING OF THE SIGNAL NEGATIVE POLARITY: BEGINNING OF THE SIGNAL

Timing Studies: using the fast-OR outputs of the VFAT2... The 8 fast s-bits of the VFAT can be used for an analysis of the timing properties of the detector. Time distribution of the delay between scintillators coincidence and an high level on the s-bit output during a test beam measurements. FAST OR Trigger lines S1...S8

The stretching of the monostable (MSPL): very important for not very fast signals In this example the first MSPL that guarantees that all the signals are collected is a MSPL of 3CLK [75ns]. TDC Measurement: Distribution of the threshold crossing time Integration of the previous distribution at different MSPL and Latency

Again for signal like the ones of GEMs detectors: When you look at the specs of the VFAT2 you have to take into account aspects concerning your signal properties (if they are different from the silicon ones, you have to rescale the specs. properly). One example: the dynamic range and the recovery time.

A curiosity more than a measuremet: VFAT2 & MicroMEGAS E. Oliveri I.N.F.N. Pisa – University of Siena RD51 4 th Collaboration Meeting, CERN

VFAT & MICROMEGAS together for the first time. Faster but dangerous! We loose the channels in the beam zone after a while! An appropriate protection circuit is needed (the one used for GEM is not enough).

The DAQ system for the VFATs readout for the RD51 test beam in H4: A PORTABLE DAQ

VFAT Controller TOTEM Monitor: data analysis CMS/TOTEM TOTEM OS LINUX Available software and reference people Access to TTP, VFAT registers and standard acquisition

Access to TTP Registers Access to VFATs Registers Automated Measurements: Threshold Scan Calibration Pulse Scan Latency Scan Simple Acquisition... and what you want (more or less) CERN TERA INFN Pisa/Siena GDD group OS WINDOWS (LabView) Available software and reference people

TTP: if needed, it can be used also as a tool for an automated chip quality test (Linux OS). T2 hybrids test result for a bunch of ~300 chips Calibration Scan result for a bunch of ~200 chips automatically measured during the testing procedure TTP Hybrids test set up in the INFN Pisa bonding lab. Well, I know that we like to see particles and not to test chips!!! But if you have to do it, you can.

bacKuP thE enD Feel free to contact me (if you can read my address!?!) E. Oliveri INFN Pisa – University of Siena RD51 4 th Collaboration Meeting, CERN If you need it, you could find documents about VFAT2 and TTP on my public dfs area:

The VFAT2 Trigger: the available patterns... the GEM mode channel assignment that in the TOTEM T2 Triple GEM detector gives this trigger pattern Groups of consecutive channels or...