On the origin of Differential Crosstalk in segmented detectors

Slides:



Advertisements
Similar presentations
Detector Characterisation Group
Advertisements

Advanced GAmma Tracking Array
GRAPE(Gamma-Ray detector Array with Position and Energy sensitivity) Developed at CNS for in-beam  -ray spectroscopy with High Resolution M.
Figure 1.17 Model of an electronic amplifier, including input resistance Ri and output resistance Ro. © 2000 Prentice Hall Inc.
Pulse Shape Analysis with Segmented Germanium Detector Xiang Liu, Max-Planck-Institut für Physik 1.Motivation 2.Pulse properties 3.Analysis procedure 4.Some.
OVERVIEW NEDA Introduction to the Simulations – Geometry The Simulations Conclusions 3.7% This work summarizes the introduction to the simulations of.
EELE 461/561 – Digital System Design Module #5 Page 1 EELE 461/561 – Digital System Design Module #5 – Crosstalk Topics 1.Near-End and Far-End Crosstalk.
AGATA Core - upgraded front end electronics
RlRl A R fb C fb C ac +Bias A R fb C fb A R bf C fb v0v0 v1v1 v2v2 V 0,out V 1,out V 2,out A simple detector model to describe crosstalk in segmented detectors.
Update on the RICH Beamtest The RICH Group M. Artuso, S. Blusk, C. Boulahouache, J. Butt, O. Dorjkhaidav, A. Kanan, N. Menaa, R. Mountain, H. Muramatsu,
FEE Perugia. A. Rivetti A FAST LARGE DYNAMIC RANGE SHAPING AMPLIFIER FOR PARTICLE DETECTOR FRONT-END A.Rivetti – P Delaurenti INFN – Sezione di Torino.
Depletion Region Dynamics of an AGATA Detector Steven Moon University of Liverpool UNTF 2010, University of Salford 14 th -16 nd April 2010.
TRACKING TEAM Introduction What has been done What still needs to be done.
AGATA 2 nd Prototype Detector Initial Measurements & Evaluation Andrew Boston, Matthew Dimmock, Laura Nelson, Sarah Rigby.
Characterisation & PSA Team Meeting Presentations –Liverpool Status, Andy Boston/Matt Dimmock (Liverpool) –Crosstalk properties of AGATA detectors, Bart.
Workshop on Physics on Nuclei at Extremes, Tokyo Institute of Technology, Institute for Nuclear Research and Nuclear Energy Bulgarian Academy.
AIDA design review Davide Braga Steve Thomas ASIC Design Group 9 June 2009.
Laura Gonella ATLAS-CMS Power Working Group, 08/02/2011
Detectors and Preamplifiers Detector deliveries Customer Acceptance Tests Available detectors AGATA triple detectors Scanning program P. Reiter IKP University.
COMMUNICATION SYSTEM EEEB453 Chapter 2 AMPLITUDE MODULATION Dept of Electrical Engineering Universiti Tenaga Nasional.
B.Satyanarayana. B.Satyanarayana INO Weekly meeting June 8, Rise time: 2 to 3ns Pulse height: mV.
July 10, 2001LArg Meeting1 Electronic Simulation Work at Victoria and TRIUMF Victoria: Erica Muzzerall, Dr. Richard Keeler TRIUMF: Dr. Chris Oram.
On the origin of Differential Crosstalk in segmented detectors B. Bruyneel for the AGATA week, Uppsala, Sweden July 2008.
Simonetta Gentile, LCWS10, March 2010, Beijing,China. G-APD Photon detection efficiency Simonetta Gentile 1 F.Meddi 1 E.Kuznetsova 2 [1]Università.
Analysis of S002 scan data Bart Bruyneel and Benedikt Birkenbach – IKP Cologne At the 7 th AGATA week, Uppsala July S003.
 -tracking uses segmented detectors which are characterized by xTalk  Traces are modified in shape and amplitude  Energy effects: peak shifts and resolution.
DESPEC A Algora IFIC (Valencia) for the Ge array working group.
Chromaticity dependence of the vertical effective impedance in the PS Chromaticity dependence of the vertical effective impedance in the PS S. Persichelli.
AHCAL Electronics. SPIROC2 and HBU measurement results Mathias Reinecke CALICE main meeting Univ. HASSAN II, Casablanca, Morocco Sept. 23rd, 2010.
New research activity “Silicon detectors modeling in RD50”: goals, tasks and the first steps Vladimir Eremin Ioffe Phisical – technical institute St. Petresburg,
 Digitisation P.Medina  Pre-processing I.Lazarus GTSM.Bellato GTSM.Bellato  PSA P.Desesquelle R.Gernhäuser 7 th AGATA Week, Uppsala, July 8-11, 2008.
Timing in Thick Silicon Detectors Andrej Studen, University of Michigan, CIMA collaboration.
 Number of signals used  Type of signals  Tests with regular and irregular grids  Last results  New idea for minimization function Roberto Venturelli.
Chapter 0 – Week 2 Combinational Logic Design. What have been discussed Design hierarchy –Top – down –Bottom – up CAD HDL Logic synthesis.
GE1/1-III GEM Cluster Size and Resolution Studies with the FNAL Beam Test Data Aiwu Zhang, Vallary Bhopatkar, Marcus Hohlmann Florida Institute of Technology.
PPAC in ZDC for Trigger and Luminosity Edwin Norbeck University of Iowa Luminosity Workshop November 5, 2004.
M. TWEPP071 MAPS read-out electronics for Vertex Detectors (ILC) A low power and low signal 4 bit 50 MS/s double sampling pipelined ADC M.
PSA: ADAPTIVE GRID SEARCH The Method Experimental Results Optimization aspects Roberto Venturelli (INFN Padova - IPSIA “Giorgi” Verona) SACLAY, 05-may-06.
Steven Moon, A.J. Boston, H. Boston, J. Cresswell, L. Harkness, D. Judson, P.J. Nolan PSD9, Aberystwyth, Wales th September 2011 Compton imaging.
Simulating the position sensitivity of the iThemba LABS segmented clover detector S. P. Noncolela 1, 2, T. D. Bucher 1, E. A. Lawrie 1, O. Shirinda 1,
Advanced Implantation Detector Array (AIDA): Update & Issues Tom Davinson School of Physics The University of Edinburgh presented by Tom Davinson on behalf.
DC bias circuit effects in CV measurements A.Chilingarov, D.Campbell Lancaster University, UK 9 th RD50 Workshop CERN,
Status of front-end electronics for the OPERA Target Tracker
Status of ULE-HPGe Experiment for WIMP Search in YangYang
AGATA Pulse Shape Analysis Implementation
A Digital Pulse Processing System Dedicated to CdZnTe Detectors
Efficiency versus energy resolution
Detectors and Preamplifiers
G. Tamulaitis, A. Augulis, V. Gulbinas, S. Nargelas, E. Songaila, A
Status of 100Mo based DBD experiment
Cross-section Measurements of (n,xn) Threshold Reactions
Performance of the Medipix and Timepix devices for the recognition of electron-gamma radiation fields C. Teyssier1,3, J. Bouchami1, F. Dallaire1, J. Idarraga1,
CAT of AGATA detectors &
Sr-84 0n EC/b+ decay search with SrCl2 crystal
HCAL Commissioning and Related Activities
SIGMA: a detector for γ-ray spectroscopy & imaging Dr Laura AGATA/GRETINA Collaboration Meeting
K. Sedlak, A. Stoykov, R. Scheuermann
A Fast Binary Front - End using a Novel Current-Mode Technique
Status of n-XYTER read-out chain at GSI
Preliminary Compton Imaging results of the AGATA C001 detector
BESIII EMC electronics
AGATA week Uppsala, July 2008
Status report Detector team
Adapted from D. Bazzacco 2012 EGAN school lecture
Daily Warm up Draw an example of two lines intersecting. Describe the way that two lines intersect. Draw an example of two lines not intersecting. Describe.
Identify the equipment such as detector, electronics modules and NIM bin. Note down detector type, size, operating voltage.
Efficiency versus energy resolution
Benchmarking Tracking by Doppler Reconstruction
Aras Papadelis NIKHEF Vertex 2005, Nikko, Japan
Werner Riegler, Christian Lippmann CERN Introduction
Presentation transcript:

On the origin of Differential Crosstalk in segmented detectors B. Bruyneel for the AGATA week , Uppsala, Sweden July 2008

Cross talk analysis: Motivation Crosstalk is present in any segmented detector Influences energy: Creates strong energy shifts proportional to fold Influences PSA: Crosstalk mixes with transient signals Fast and accurate crosstalk detection and energy correction methods developed To Do : Crosstalk measurement and correction in PSA Sum of segment Energies vs fold Xtalk signal: For the last part of my talk, I would like to draw the attention to a problem common to any segmented detector : namely cross talk. This creates strong energy shifts in the segment sum energy, and this proportional to the hit multiplicity: Doubles are shifted compared to singles. Three folds even more, and so on. >> If one analyzes the doubles, one observes that it does not simply consists of a single peak, but: By sorting the two folds into all possible twofold combinations, one observes that the centroids of these peaks are individually shifting according to a regular patten. The same happens in the core,however there is no such offset observed as is in the segments. There is thus real physics behind this phenomenon. >>

Crosstalk in all its forms Proportional Xtalk (50s decay)  Energy Differential Xtalk (only during risetime)  PSA Pure Xtalk signal: PA V0,out V1,out Zin Z01 Xtalk ~ Zin / Z01 Proportional Xtalk model : Zin = Miller = 1/sACfb But: Miller does not explain risetime of preamplifier…!

Preamp model describing risetime PA Vout Vin Vout/Iin = Zfb Iin Zin = Vin/Iin Zin = Zfb/A + Rcold “Cold Resistor” : - E. Gatti and P. Manfredi – Il Nuovo Cimento vol. 9 serie 3 (1986) - “Analogue circuits techniques Part II ” F. Anghinolfi , CERN (2002) – (available online)

Xtalk extension With Zin = 1/sACfb + Rcold Zin PA V0,out V1,out Zin Z01 With Zin = 1/sACfb + Rcold Xtalk ~ Zin / Z01 = C01/ACfb + s . Rcold C01 Proportional + Differential Xtalk Example : Rcold = 1k; C01 = 10pF Differential Xtalk = 1000%ns Warning: Other ways possible to create Derivative Xtalk !

Realistic simulation (Multisim) PA V0,out V0,out 10pF PA V1,out Realistic Preamp model V1,out

Differential Xtalk from Proportional Xtalk? Segment labeling: Sectors: A...F Rings: 1...6 Core to seg capacity Seg to seg capacities? A2..A6 B1 F1 X Differential Xtalk will show up in adjacent segments and within same sector

How to measure …? B. Bruyneel et al. NIM A 569 (2006) 774-789 / MGS workshop (April 2005) / AGATA week (Nov 2005)

“Differential Analysis” using mirror interaction points: How to measure…? (2) “Pulse Shape Characterization and Simulation for the TIGRESS Gamma-ray Detector “ Thesis Robin Prest TRIUMF 2005 http://www.physics.uoguelph.ca/Nucweb/tigress.htm Simulated signal (green) compared to experimental signal (red) suffering from cross-talk 5 6 8 7 (a,b) •(b,a) Differential analysis. for simulation (green) and experiment (red) “Differential Analysis” using mirror interaction points: “differences from transients of mirror interactions are pure”