IRST SiPM characterizations and Application Studies
|
|
- Elvin Willis
- 5 years ago
- Views:
Transcription
1 IRST SiPM characterizations and Application Studies G. Pauletta for the FACTOR collaboration Outline 1. Introduction (who and where) 2. Objectives and program (what and how) 3. characterizations 4. Applications 28 June 2007 G. Pauletta: PD07, Kobe, Japan 1
2 FACTOR 3-year project ( ) funded by INFN Participants: INFN laboratories and/or universities at:trieste, Udine, Messina collaborating with ITC (now Bruno Kessler Foundation) -IRST Trento, Italy Background: 2005: INFN funds project (DASiPM) for the development of SiPM devices, mainly for PET application 2007: INFN funds continuation of DASIPM and expands development to other applications (FACTOR) INFN-Trieste has a long standing collaboration with IRST in the development of Silicon-based detectors for application in accelerator, underground and space based experimental particle physics. 28 June 2007 G. Pauletta: PD07, Kobe, Japan 2
3 Motivations The FACTOR collaboration interested in the development of the device and in its optimization for application to: Present application interests: Calorimetry with fiber-based optical readout Large area scintillator based muon counters Scintillating fiber based tracking future space experiments for detection of UHECR FEL studies and instrumentation future large area, ground based x-ray telescopes Action Plan: comparative studies for detailed understanding of device characteristics Application tests Optimization of properties as a function of application 28 June 2007 G. Pauletta: PD07, Kobe, Japan 3
4 Present IRST technology* *C. Piemonte A new Silicon Photomultiplier structure for blue light detection NIMA 568 (2006) 20 n + p 7E+05 Shallow-Junction SiPM n+ π epi Doping conc. (10^) [1/cm^3] Doping Field 6E+05 5E+05 4E+05 3E+05 2E+05 1E+05 E field (V/cm) p+ subst depth (um) 0E+00 Distinguishing characteristics: 1) Very shallow junction 2) ARC optimized for short wavelenghts (~400nm) 3) polysilicon quenching resistors 28 June 2007 G. Pauletta: PD07, Kobe, Japan 4
5 Development History Development started at the beginning of 2005 Baseline geometry 1mm SiPM structure: - 25x25 cells - microcell size: 40x40mm 2 1mm Development has continued over last two years: several succeeding production runs to to develop geometries for different applications and to optmize operational characteristics Geometry of baseline model NOT optimized formaximum PDE ( fill factor ~20%). 28 June 2007 G. Pauletta: PD07, Kobe, Japan 5
6 Principal characteristics of interest Gain Noise dark count afterpulsing optical cross-talk PhotoDetection Efficiency (PDE) Dynamic Range Time characteristics rise time, resolution, recovery time Radiation hardness Sensitivity to magnetic fiels Packaging Readout electronics Other considerations 28 June 2007 G. Pauletta: PD07, Kobe, Japan 6
7 Device characterization 1,2 Static measurents: IV measurements for rapid test of device properties, uniformity and stability Dynamic tests: Output signal characterization and stability using noise signals in the dark Signal rise time and fall time Gain Dark count Optical cross talk Afterpulsing PhotoDetection Efficiency 1)All characterizations reported here are for 1mm 2 devices 2) for a thorough characterization of the first SiPM prototypes fabricated at ITC-irst see C. Piemonte, IEEE TNS, February June 2007 G. Pauletta: PD07, Kobe, Japan 7
8 Current (A) Static measurements-1 1µ 100n 10n 1n 100p I bd IRST 00 IRST 02 IRST 08 IRST 11 IRST 03 Baseline version reverse Voltage (V) SiPM Vbd (V) Ibd (na) IRST-00 32,5 3,6 IRST-02 33,0 3,6 IRST-03 33,0 3,1 IRST-08 33,5 3,2 IRST-11 33,5 3,8 V BD I tot I leak Rapid check functionality & uniformity IRST 1mm 2 second batch Sensitive to principal characteristics dark current is prop. to gain G and since I I I dc I and dark count G. G V, dc dc = V tot 2 I leak ( DC) IRST devices generally very uniform DC V ( DC) 28 June 2007 G. Pauletta: PD07, Kobe, Japan 8
9 Static measurements-2 100µ 10µ Blue enhanced 3x3 SiPM PHOT 18 PHOT 19 PHOT 20 10µ 1µ blue enhanced 1x1 SiPM PHOT 21 PHOT 22 PHOT 23 Current (A) 1µ 100n Current (A) 100n 10n 10n 1n 1n reverse Voltage (V) 100p SiPM Vbd (V) Ibd (na) Phot-18 52,5 125,8 Phot-19 49,5 260,6 Phot-20 49,0 98,7 Phot-21 51,0 6,5 Phot-22 53,0 6,9 Phot-23 55,0 6, reverse Voltage (V) Photonique 9mm 2 Blue sensitive Photonique 1mm 2 Green-red sensitive 28 June 2007 G. Pauletta: PD07, Kobe, Japan 9
10 Current (A) Static measurements-3 1,8m 1,6m 1,4m 1,2m 1,0m 800,0µ 600,0µ 400,0µ 200,0µ 0,0 IRST 00 IRST 02 IRST 03 IRST 08 IRST 11 Current (A) 250,0µ 200,0µ 150,0µ 100,0µ 50,0µ 0,0 Phot 21 Phot 22 Phot ,0µ -0,2 0,0 0,2 0,4 0,6 0,8 1,0 1,2 1,4 1,6 1,8 direct Voltage (V) direct Voltage (V) SiPM Rq (Ohm) IRST IRST IRST IRST IRST kΩ IRST 1mm 2 second batch SiPM Rq (kohm) Phot-18 2,29 Phot-19 1,52 Phot-20 1,24 Phot-21 39,8 Phot-22 17,4 Phot-23 37,8 Photonique 9mm 2 Blue sensitive Photonique 1mm 2 Green-red sensitive 28 June 2007 G. Pauletta: PD07, Kobe, Japan 10
11 Capacitance (F) 450,0p 400,0p 350,0p 300,0p 250,0p 200,0p 150,0p IRST 00 IRST 02 IRST 03 IRST 08 IRST 11 Capacitance (F) 90,0p 85,0p 80,0p 75,0p 70,0p 65,0p 60,0p Static measurements-4 Photo 21 Photo 22 Photo ,0p 55,0p 50,0p 50,0p 0, reverse Voltage (V) 45,0p reverse Voltage (V) SiPM Vdep (V) Cdep (pf) IRST IRST IRST IRST IRST ff 28 June 2007 G. Pauletta: PD07, Kobe, Japan 11
12 dynamic measurements-1 Amplifier used for fast characterization of SiPMs: Agilent ABA GHz RFIC Amplifier (economic, compact, internally 50-Ω matched, gain ~ 20 db) Dimensions 1.8 x 1.8 mm2 Orange trace: input from pulse generator, FWHM = 0.9 ns, tr = tf = 300 ps Red trace: amplifier s output 28 June 2007 G. Pauletta: PD07, Kobe, Japan 12
13 dynamic measurements-2 IRST :recovery time ~70 ns Formitech F1: R recovery time 400ns q 0.9 MΩ, MRS SiPMs have 2.5 to 50 times larger Rq values than IRST (polysilicon) devices longer recovery rimes 28 June 2007 G. Pauletta: PD07, Kobe, Japan 13
14 dynamic measurements-4 1 mm 2 type A VBD 33 V D.C.(ΔV=2V) 1.5 MHz Linear fit intercept with V-axis gives VBD = V 28 June 2007 G. Pauletta: PD07, Kobe, Japan 14
15 dynamic measurements-4 1 mm2 MRS devices VBD 20 V D.C.(ΔV=2V) 2 MHz 1 mm2 MRS device VBD 41 V D.C.(ΔV=2V) 2.2 MHz 28 June 2007 G. Pauletta: PD07, Kobe, Japan 15
16 dynamic measurements-5 type A, D.C.(ΔV=2V) 1.5 MHz type B, D.C.(ΔV=2V) 2-3 MHz type D, D.C.(ΔV=2V) 1 MHz 28 June 2007 G. Pauletta: PD07, Kobe, Japan 16
17 dynamic measurements-6 Temperature Dependences - 1 Measurements performed in a climatic chamber (with humidity control) The amplifier was located outside the chamber, connection via a special 18 GHz ft 50 Ω cable dv BD /dt 78 mv/c 28 June 2007 G. Pauletta: PD07, Kobe, Japan 17
18 dynamic measurements-7 Temperature Dependences - 2 dv BD /dt 72 mv/c 28 June 2007 G. Pauletta: PD07, Kobe, Japan 18
19 dynamic measurements-8 Temperature dependences June 2007 G. Pauletta: PD07, Kobe, Japan 19
20 The following are static measurements performed at ITC-IRST and reported on at a recent (June 13 th 2007) workshop at Perugia 28 June 2007 G. Pauletta: PD07, Kobe, Japan 20
21 Signal properties 100ns 100ns 100ns Charge spectra T int =100ns C. Piemonte et al. Characterization of the first prototypes of SiPM fabricated at ITC-irst IEEE TNS, February 2007 Normalized Count T=22 o C s d a -2.0E E E E E+00 Charve (V*s) Well defined peak of the single pulses. Gaussian distribution width determined by: - noise of the system - tiny gain non-uniformities Tails due to: optical cross-talk + afterpulse 28 June 2007 G. Pauletta: PD07, Kobe, Japan 21 C. Piemonte: June 13 th, 2007, Perugia
22 Dark count 31 Gain & Dark count Performed in the climatic chamber. Devices from the third batch 3.0E E E E E E E+00-5 C 5 C 15 C 25 C DC Over-voltage (V) Gain 4.0E E E E E E E E E+00-5 C 5 C 15 C 25 C 2.50E+06 G Ampl Bias voltage (V) E+06 VBD (V) Vbd 1.50E+06 Gain 1.00E+06 y = x + 2E E+05 y = x E Temp. (C) Gain 28 June 2007 G. Pauletta: PD07, Kobe, Japan 22 C. Piemonte: June 13 th, 2007, Perugia
23 Gain & Dark count (uniformity) 3.0E+06 G AMPL 2.5E E+06 Gain 1.5E+06 Dark Count (Hz) 1.0E E E E E E E E E E E E Over-voltage (V) DC Over-voltage (V) Gain and Dark count measured on devices from the same wafer 28 June 2007 G. Pauletta: PD07, Kobe, Japan 23 C. Piemonte: June 13 th, 2007, Perugia
24 Optical cross-talk Short integration time only single/double/.pulses are counted Counts double peak 35.5V 33.5V ΔV = 4.5V 1.5V Number of events with optical cross-talk increases with voltage Cross-talk below 5% at 4V over-voltage. 0-8E E E E E+00 0 QDC Charge (a.u.) 28 June 2007 G. Pauletta: PD07, Kobe, Japan 24 C. Piemonte: June 13 th, 2007, Perugia
25 0.05 After-pulsing Voltage (V) E E E E E-08 Time (s) After-pulse probability vs bias It increases following a parabolic law: P a = linear with Vbias P c P 01 linear with Vbias Afterpulse/pulse Events with after-pulse measured on a single micropixel. The amplitude of the after-pulse increases as the cell recovers to its opertional condition Tint = 60ns Tint = 100ns y = x x y = x x Voltage (V) 28 June 2007 G. Pauletta: PD07, Kobe, Japan 25 C. Piemonte: June 13 th, 2007, Perugia
26 Photo-detection efficiency DC curr with light DC curr. wo light dark pulses light pulses 28 June 2007 G. Pauletta: PD07, Kobe, Japan 26 C. Piemonte: June 13 th, 2007, Perugia
27 PDE (%) PDE 1.60E E E E E E E E E+00 Photodetection efficiency 3.5V 3V 2.5V ΔV=2V Wavelength (nm) short λ: low PDE because avalanche triggered by holes 4V Area efficiency ~ 20% long λ: low PDE because low QE C. Piemonte: June 13 th, 2007, Perugia Measured on a diode 80 by ARC 28 June 2007 G. Pauletta: PD07, Kobe, Japan 27 36V 36.5V 37V 37.5V 38V QE (%) Reduced PDE=QE*Pt*Ae QE=quantum eff. P t =avalanche prob. A e =area eff. QE vs Wavelength 0V -2V Simul Simul ARC Reduced by small epi thickness Wavelength (nm)
28 last batch 1x1mm 2x2mm 3x3mm (3600 cells) 4x4mm (6400 cells) increased fill factor: 40x40mm => 44% 50x50mm => 50% 100x100mm => 76%; Circular (1.2 mm diameter) C. Piemonte: June 13 th, 2007, Perugia Array 28 June 2007 G. Pauletta: PD07, Kobe, Japan 28
29 First signal and noise characteristics of the last devices 3.5E E E E E E E E+00 5C GAIN 5C Dark Coun Noise and charge resolution 1x1mm 2 SiPM with 40x40μm 2 cells 5.0E E E E E E+00 T=5C T=20C 20C GAIN 20C Dark count C. Piemonte: June 13 th, 2007, Perugia 28 June 2007 G. Pauletta: PD07, Kobe, Japan Charge spectra at different Voltages with the same light Intensity (pulsed) 9.5p.e. 8p.e. 6.5p.e. 5p.e. 3.5p.e E E E E+00 Pulse Area (Vs) resolution limited by electronic noise
30 applications 28 June 2007 G. Pauletta: PD07, Kobe, Japan 30
31 Characterization of SiPMs (1 mm 2 from second batch) used for preliminary at Fnal test beam Visual inspectons (SiDet) and dynamic tests at lab 6 prior to use of SiPMs in Test Beam yielded results compatible with IRST measurements: V B = 34.1 V Gains between ~1 and 2 x 10 6 dark count vs. bias 28 June 2007 G. Pauletta: PD07, Kobe, Japan 31
32 Preliminary study of Scint. Strip viewed by IRST SiPM at the FNAL test beam T956 neutron counter arrays Counter readout on both ends by SiPMs Beam (12 GeV protons) Bias = -36V (ΔV=2V) Data with 120 Gev proton - beam N p. e. ε = 99% N d. c. 6.5 p. e. 1.5MHz G June 2007 G. Pauletta: PD07, Kobe, Japan 32
33 T956 neutron counter arrays: 64 scint strips each (read out by wls fiber and MAPMTs) Beam (p,π,e) Future work at fnal Add one plane of scint strips read out by Wls fiber and SiPMs Whole assembly mounted on movable (x,y) support Scintillator strips : 4cm x 1cm x (1 2 m), read out by wls fiber. Groove for fiber extruded with scintillator 28 June 2007 G. Pauletta: PD07, Kobe, Japan 33
34 28 June 2007 G. Pauletta: PD07, Kobe, Japan 34
35 28 June 2007 G. Pauletta: PD07, Kobe, Japan 35
36 28 June 2007 G. Pauletta: PD07, Kobe, Japan 36
FACTOR: first results on SiPM characterization
FACTOR: first results on SiPM characterization Valter Bonvicini INFN Trieste OUTLINE: 1. Motivations and program of the FACTOR project 2. Types of devices tested, measurements performed and set-up used
More informationCharacterization of a prototype matrix of Silicon PhotoMultipliers (SiPM s)
Characterization of a prototype matrix of Silicon PhotoMultipliers (SiPM s) N. Dinu, P. Barrillon, C. Bazin, S. Bondil-Blin, V. Chaumat, C. de La Taille, V. Puill, JF. Vagnucci Laboratory of Linear Accelerator
More informationSilicon Photo Multiplier SiPM. Lecture 13
Silicon Photo Multiplier SiPM Lecture 13 Photo detectors Purpose: The PMTs that are usually employed for the light detection of scintillators are large, consume high power and are sensitive to the magnetic
More informationA tracking detector to study O(1 GeV) ν μ CC interactions
A tracking detector to study O(1 GeV) ν μ CC interactions Laura Pasqualini on behalf of the mm-tracker Collaboration IPRD16, 3-6 October 2016, Siena Motivations ν/μ Tracking system for a light magnetic
More informationCharacteristics of a prototype matrix of Silicon PhotoMultipliers (SiPM)
Journal of Instrumentation OPEN ACCESS Characteristics of a prototype matrix of Silicon PhotoMultipliers (SiPM) To cite this article: N Dinu et al View the article online for updates and enhancements.
More informationSiPM development within the FBK/INFN collaboration. G. Ambrosi INFN Perugia
SiPM development within the FBK/INFN collaboration G. Ambrosi INFN Perugia 2 FBK Trento (IT) Clean room «Detectors»: - 500m2-6 wafers - Equipped with: ion implanter 8 furnaces wet etching dry etching lithography
More informationarxiv: v1 [astro-ph.im] 19 Nov 2014
Measurements and tests on FBK silicon sensors with an optimized electronic design for a CTA camera arxiv:1411.5241v1 [astro-ph.im] 19 Nov 214 G. Ambrosi (1), M. Ambrosio (2), C. Aramo (2), E. Bissaldi
More informationReview of Solidstate Photomultiplier. Developments by CPTA & Photonique SA
Review of Solidstate Photomultiplier Developments by CPTA & Photonique SA Victor Golovin Center for Prospective Technologies & Apparatus (CPTA) & David McNally - Photonique SA 1 Overview CPTA & Photonique
More informationDevelopment of the first prototypes of Silicon PhotoMultiplier (SiPM) at ITC-irst
Nuclear Instruments and Methods in Physics Research A 572 (2007) 422 426 www.elsevier.com/locate/nima Development of the first prototypes of Silicon PhotoMultiplier (SiPM) at ITC-irst N. Dinu a,,1, R.
More informationTutors Dominik Dannheim, Thibault Frisson (CERN, Geneva, Switzerland)
Danube School on Instrumentation in Elementary Particle & Nuclear Physics University of Novi Sad, Serbia, September 8 th 13 th, 2014 Lab Experiment: Characterization of Silicon Photomultipliers Dominik
More informationRecent Development and Study of Silicon Solid State Photomultiplier (MRS Avalanche Photodetector)
Recent Development and Study of Silicon Solid State Photomultiplier (MRS Avalanche Photodetector) Valeri Saveliev University of Obninsk, Russia Vienna Conference on Instrumentation Vienna, 20 February
More informationirst: process development, characterization and first irradiation studies
3D D detectors at ITC-irst irst: process development, characterization and first irradiation studies S. Ronchin a, M. Boscardin a, L. Bosisio b, V. Cindro c, G.-F. Dalla Betta d, C. Piemonte a, A. Pozza
More informationarxiv: v2 [physics.ins-det] 14 Jan 2009
Study of Solid State Photon Detectors Read Out of Scintillator Tiles arxiv:.v2 [physics.ins-det] 4 Jan 2 A. Calcaterra, R. de Sangro [], G. Finocchiaro, E. Kuznetsova 2, P. Patteri and M. Piccolo - INFN,
More informationSilicon Photomultiplier
Silicon Photomultiplier Operation, Performance & Possible Applications Slawomir Piatek Technical Consultant, Hamamatsu Corp. Introduction Very high intrinsic gain together with minimal excess noise make
More informationCharacterisation of SiPM Index :
Characterisation of SiPM --------------------------------------------------------------------------------------------Index : 1. Basics of SiPM* 2. SiPM module 3. Working principle 4. Experimental setup
More informationDevelopment of 3D detectors and
Development of 3D detectors and SiPM @ ITC-irst Maurizio Boscardin boscardi@itc.it ITC-irst ITC (Istituto Trentino di Cultura) is a public research institute in Trento mainly funded by the local government
More informationJ-Series High PDE and Timing Resolution, TSV Package
High PDE and Timing Resolution SiPM Sensors in a TSV Package SensL s J-Series low-light sensors feature a high PDE (photon detection efficiency) that is achieved using a high-volume, P-on-N silicon foundry
More informationTotal Absorption Dual Readout Calorimetry R&D
Available online at www.sciencedirect.com Physics Procedia 37 (2012 ) 309 316 TIPP 2011 - Technology and Instrumentation for Particle Physics 2011 Total Absorption Dual Readout Calorimetry R&D B. Bilki
More informationSiPMs for solar neutrino detector? J. Kaspar, 6/10/14
SiPMs for solar neutrino detector? J. Kaspar, 6/0/4 SiPM is photodiode APD Geiger Mode APD V APD full depletion take a photo-diode reverse-bias it above breakdown voltage (Geiger mode avalanche photo diode)
More informationThermal and electrical characterization of silicon photomultiplier
University of Wollongong Research Online Faculty of Engineering and Information Sciences - Papers: Part A Faculty of Engineering and Information Sciences 2008 Thermal and electrical characterization of
More informationP ILC A. Calcaterra (Resp.), L. Daniello (Tecn.), R. de Sangro, G. Finocchiaro, P. Patteri, M. Piccolo, M. Rama
P ILC A. Calcaterra (Resp.), L. Daniello (Tecn.), R. de Sangro, G. Finocchiaro, P. Patteri, M. Piccolo, M. Rama Introduction and motivation for this study Silicon photomultipliers ), often called SiPM
More informationStatus of ITC-irst activities in RD50
Status of ITC-irst activities in RD50 M. Boscardin ITC-irst, Microsystem Division Trento, Italy Outline Materials/Pad Detctors Pre-irradiated silicon INFN Padova and Institute for Nuclear Research of NASU,
More informationA BaF2 calorimeter for Mu2e-II
A BaF2 calorimeter for Mu2e-II I. Sarra, on behalf of LNF group Università degli studi Guglielmo Marconi Laboratori Nazionali di Frascati NEWS General Meeting 218 13 March 218 Proposal (1) q This technological
More informationCALICE AHCAL overview
International Workshop on the High Energy Circular Electron-Positron Collider in 2018 CALICE AHCAL overview Yong Liu (IHEP), on behalf of the CALICE collaboration Nov. 13, 2018 CALICE-AHCAL Progress, CEPC
More informationGeiger-mode APDs (2)
(2) Masashi Yokoyama Department of Physics, University of Tokyo Nov.30-Dec.4, 2009, INFN/LNF Plan for today 1. Basic performance (cont.) Dark noise, cross-talk, afterpulsing 2. Radiation damage 2 Parameters
More informationIntroduction to silicon photomultipliers (SiPMs) White paper
Introduction to silicon photomultipliers (SiPMs) White paper Basic structure and operation The silicon photomultiplier (SiPM) is a radiation detector with extremely high sensitivity, high efficiency, and
More informationDirect Measurement of Optical Cross-talk in Silicon Photomultipliers Using Light Emission Microscopy
Direct Measurement of Optical Cross-talk in Silicon Photomultipliers Using Light Emission Microscopy Derek Strom, Razmik Mirzoyan, Jürgen Besenrieder Max-Planck-Institute for Physics, Munich, Germany ICASiPM,
More informationA Prototype Amplifier-Discriminator Chip for the GLAST Silicon-Strip Tracker
A Prototype Amplifier-Discriminator Chip for the GLAST Silicon-Strip Tracker Robert P. Johnson Pavel Poplevin Hartmut Sadrozinski Ned Spencer Santa Cruz Institute for Particle Physics The GLAST Project
More informationDirect Measurement of Optical Cross-talk in Silicon Photomultipliers Using Light Emission Microscopy
Direct Measurement of Optical Cross-talk in Silicon Photomultipliers Using Light Emission Microscopy Derek Strom, Razmik Mirzoyan, Jürgen Besenrieder Max-Planck-Institute for Physics, Munich, Germany 14
More informationContents. The AMADEUS experiment at the DAFNE collider. The AMADEUS trigger. SiPM characterization and lab tests
Contents The AMADEUS experiment at the DAFNE collider The AMADEUS trigger SiPM characterization and lab tests First trigger prototype; tests at the DAFNE beam Second prototype and tests at PSI beam Conclusions
More informationSINPHOS SINGLE PHOTON SPECTROMETER FOR BIOMEDICAL APPLICATION
-LNS SINPHOS SINGLE PHOTON SPECTROMETER FOR BIOMEDICAL APPLICATION Salvatore Tudisco 9th Topical Seminar on Innovative Particle and Radiation Detectors 23-26 May 2004 Siena, Italy Delayed Luminescence
More informationLow Dark Count UV-SiPM: Development and Performance Measurements P. Bérard, M. Couture, P. Deschamps, F. Laforce H. Dautet and A.
Low Dark Count UV-SiPM: Development and Performance Measurements P. Bérard, M. Couture, P. Deschamps, F. Laforce H. Dautet and A. Barlow LIGHT 11 Workshop on the Latest Developments of Photon Detectors
More informationMonolithic Pixel Sensors in SOI technology R&D activities at LBNL
Monolithic Pixel Sensors in SOI technology R&D activities at LBNL Lawrence Berkeley National Laboratory M. Battaglia, L. Glesener (UC Berkeley & LBNL), D. Bisello, P. Giubilato (LBNL & INFN Padova), P.
More informationCharacterization of SiPMs for Large Scale Applications
SiPM KETEK SiPM Characterization of SiPMs for Large Scale Applications Eugen Engelmann (eugen.engelmann@ketek.net) 1 SiPM KETEK Family-owned enterprise, founded in 1989 by Dr. Josef Kemmer Number of employees:
More informationGain and Breakdown Voltage Measurements
Gain and Breakdown Voltage Measurements CLICdp: ECAL Lab Meeting (CERN) Magdalena Munker March 2, 215 Setup for study of Scintillator tiles with SiPM Readout Setup in cooled dark room ( temperature about
More informationHigh granularity scintillating fiber trackers based on Silicon Photomultiplier
High granularity scintillating fiber trackers based on Silicon Photomultiplier A. Papa Paul Scherrer Institut, Villigen, Switzerland E-mail: angela.papa@psi.ch Istituto Nazionale di Fisica Nucleare Sez.
More informationSilicon Photomultipliers
Silicon Photomultipliers a new device for frontier detectors in HEP, astroparticle physics, nuclear medical and industrial applications Nepomuk Otte MPI für Physik, Munich Outline Motivation for new photon
More informationNovel scintillation detectors. A. Stoykov R. Scheuermann
Novel scintillation detectors for µsr-spectrometers A. Stoykov R. Scheuermann 12 June 2007 SiPM Silicon PhotoMultiplier AMPD (MAPD) Avalanche Microchannel / Micropixel PhotoDiode MRS APD Metal-Resistive
More informationAndrea WILMS GSI, Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
GSI, Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany E-mail: A.Wilms@gsi.de During the last years the experimental demands on photodetectors used in several HEP experiments have increased
More informationScintillator/WLS Fiber Readout with Geiger-mode APD Arrays
Scintillator/WLS Fiber Readout with Geiger-mode APD Arrays David Warner, Robert J. Wilson, Qinglin Zeng, Rey Nann Ducay Department of Physics Colorado State University Stefan Vasile apeak 63 Albert Road,
More informationAN ADVANCED STUDY OF SILICON PHOTOMULTIPLIER
AN ADVANCED STUDY OF SILICON PHOTOMULTIPLIER P. Buzhan, B. Dolgoshein, A. Ilyin, V. Kantserov, V. Kaplin, A. Karakash, A. Pleshko, E. Popova, S. Smirnov, Yu. Volkov Moscow Engineering and Physics Institute,
More informationNON-AMPLIFIED PHOTODETECTOR USER S GUIDE
NON-AMPLIFIED PHOTODETECTOR USER S GUIDE Thank you for purchasing your Non-amplified Photodetector. This user s guide will help answer any questions you may have regarding the safe use and optimal operation
More informationAn innovative detector concept for hybrid 4D-PET/MRI Imaging
Piergiorgio Cerello (INFN - Torino) on behalf of the 4D-MPET* project *4 Dimensions Magnetic compatible module for Positron Emission Tomography INFN Perugia, Pisa, Torino; Polytechnic of Bari; University
More informationILC Prototype Muon Scintillation Counter Tests
ILC Prototype Muon Scintillation Counter Tests Robert Abrams Indiana University August 23, 2005 ALCPG R.J. Abrams 1 Update on Testing At FNAL New Test Setup in Lab 6 with Fermilab Support Testing Two New
More informationA Measurement of the Photon Detection Efficiency of Silicon Photomultipliers
A Measurement of the Photon Detection Efficiency of Silicon Photomultipliers A. N. Otte a,, J. Hose a,r.mirzoyan a, A. Romaszkiewicz a, M. Teshima a, A. Thea a,b a Max Planck Institute for Physics, Föhringer
More informationSTART as the detector of choice for large-scale muon triggering systems
START as the detector of choice for large-scale muon triggering systems A. Akindinov a, *, G. Bondarenko b, V. Golovin c, E. Grigoriev d, Yu. Grishuk a, D. Mal'kevich a, A. Martemiyanov a, A. Nedosekin
More informationPoS(PhotoDet 2012)058
Absolute Photo Detection Efficiency measurement of Silicon PhotoMultipliers Vincent CHAUMAT 1, Cyril Bazin, Nicoleta Dinu, Véronique PUILL 1, Jean-François Vagnucci Laboratoire de l accélérateur Linéaire,
More informationStudies of Scintillator Tile Geometries for direct SiPM Readout of Imaging Calorimeters
Studies of Scintillator Tile Geometries for direct SiPM Readout of Imaging Calorimeters Frank Simon MPI for Physics & Excellence Cluster Universe Munich, Germany for the CALICE Collaboration Outline The
More informationThe Calice Analog Scintillator-Tile Hadronic Calorimeter Prototype
SNIC Symposium, Stanford, California -- 3-6 April 26 The Calice Analog Scintillator-Tile Hadronic Calorimeter Prototype M. Danilov Institute of Theoretical and Experimental Physics, Moscow, Russia and
More informationSILICON PHOTOMULTIPLIERS: FROM 0 TO IN 1 NANOSECOND. Giovanni Ludovico Montagnani polimi.it
SILICON PHOTOMULTIPLIERS: FROM 0 TO 10000 IN 1 NANOSECOND Giovanni Ludovico Montagnani Giovanniludovico.montagnani@ polimi.it LESSON OVERVIEW 1. Motivations: why SiPM are useful 2. SiPM applications examples
More informationRed, Green, Blue (RGB) SiPMs
Silicon photomultipliers (SiPMs) from First Sensor are innovative solid-state silicon detectors with single photon sensitivity. SiPMs are a valid alternative to photomultiplier tubes. The main benefits
More informationPerformance of the Hall D Tagger Microscope as a Function of Rate
Performance of the Hall D Tagger Microscope as a Function of Rate R.T. Jones University of Connecticut, Storrs, CT December 30, 2010 Abstract The Hall D tagger microscope is responsible for determining
More informationNear Ultraviolet (NUV) SiPMs
Silicon photomultipliers (SiPMs) from First Sensor are innovative solid-state silicon detectors with single photon sensitivity. SiPMs are a valid alternative to photomultiplier tubes. The main benefits
More informationA Novel Design of a High-Resolution Hodoscope for the Hall D Tagger Based on Scintillating Fibers
A Novel Design of a High-Resolution Hodoscope for the Hall D Tagger Based on Scintillating Fibers APS Division of Nuclear Physics Meeting October 25, 2008 GlueX Photon Spectrum Bremsstrahlung in diamond
More informationThe PERDaix Detector. Thomas Kirn I. Physikalisches Institut B. July 5 th 2011, 6 th International Conference on New Developments In Photodetection
Proton Electron Radiation Detector Aix la Chapelle The PERDaix Detector Thomas Kirn I. Physikalisches Institut B July 5 th 2011, 6 th International Conference on New Developments In Photodetection Motivation
More informationarxiv: v3 [astro-ph.im] 17 Jan 2017
A novel analog power supply for gain control of the Multi-Pixel Photon Counter (MPPC) Zhengwei Li a,, Congzhan Liu a, Yupeng Xu a, Bo Yan a,b, Yanguo Li a, Xuefeng Lu a, Xufang Li a, Shuo Zhang a,b, Zhi
More informationSilicon Carbide Solid-State Photomultiplier for UV Light Detection
Silicon Carbide Solid-State Photomultiplier for UV Light Detection Sergei Dolinsky, Stanislav Soloviev, Peter Sandvik, and Sabarni Palit GE Global Research 1 Why Solid-State? PMTs are sensitive to magnetic
More informationTest and Simulation of Plastic Scintillator Strips readout by Silicon Photomultipliers
Test and Simulation of Plastic Scintillator Strips readout by Silicon Photomultipliers Tosi Nicolò, Balbi G., Boldini M., Cafaro V., Dallavalle G.M., D Antone I., Fabbri F., Giordano V., Lax I., Montanari
More informationRedefining Measurement ID101 OEM Visible Photon Counter
Redefining Measurement ID OEM Visible Photon Counter Miniature Photon Counter for OEM Applications Intended for large-volume OEM applications, the ID is the smallest, most reliable and most efficient single-photon
More informationAIDA-2020 Advanced European Infrastructures for Detectors at Accelerators. Milestone Report
AIDA-2020-MS15 AIDA-2020 Advanced European Infrastructures for Detectors at Accelerators Milestone Report Design specifications of test stations for irradiated silicon sensors and LHC oriented front-end
More informationThe CMS Outer HCAL SiPM Upgrade.
The CMS Outer HCAL SiPM Upgrade. Artur Lobanov on behalf of the CMS collaboration DESY Hamburg CALOR 2014, Gießen, 7th April 2014 Outline > CMS Hadron Outer Calorimeter > Commissioning > Cosmic data Artur
More informationSimulation and test of 3D silicon radiation detectors
Simulation and test of 3D silicon radiation detectors C.Fleta 1, D. Pennicard 1, R. Bates 1, C. Parkes 1, G. Pellegrini 2, M. Lozano 2, V. Wright 3, M. Boscardin 4, G.-F. Dalla Betta 4, C. Piemonte 4,
More informationHow to Evaluate and Compare Silicon Photomultiplier Sensors. October 2015
The Silicon Photomultiplier (SiPM) is a single-photon sensitive light sensor that combines performance characteristics that exceed those of a PMT, with the practical advantages of a solid state sensor.
More informationScintillation Counters
PHY311/312 Detectors for Nuclear and Particle Physics Dr. C.N. Booth Scintillation Counters Unlike many other particle detectors, which exploit the ionisation produced by the passage of a charged particle,
More informationFast Timing for Collider Detectors
Fast Timing for Collider Detectors Chris Tully (Princeton University) CERN Academic Training Lectures (2/3) 11 May 2017 Outline Detector technologies with fast timing capabilities Readout methods for fast
More informationDesign and Simulation of a Silicon Photomultiplier Array for Space Experiments
Journal of the Korean Physical Society, Vol. 52, No. 2, February 2008, pp. 487491 Design and Simulation of a Silicon Photomultiplier Array for Space Experiments H. Y. Lee, J. Lee, J. E. Kim, S. Nam, I.
More informationPlans for RPC DHCAL Prototype. David Underwood Argonne National Laboratory
Plans for RPC DHCAL Prototype David Underwood Argonne National Laboratory Linear Collider Meeting, SLAC 7-10 January 2004 Outline Collaborators Goals Motivation Mechanical Structure Chamber Description
More informationApplication of Silicon Photomultipliers to Positron Emission Tomography
Annals of Biomedical Engineering, Vol. 39, No. 4, April 2011 (Ó 2011) pp. 1358 1377 DOI: 10.1007/s10439-011-0266-9 Application of Silicon Photomultipliers to Positron Emission Tomography EMILIE RONCALI
More informationPRELIMINARY RESULTS OF PLASTIC SCINTILLATORS DETECTOR READOUT WITH SILICON PHOTOMULTIPLIERS FOR COSMIC RAYS STUDIES *
Romanian Reports in Physics, Vol. 64, No. 3, P. 831 840, 2012 PRELIMINARY RESULTS OF PLASTIC SCINTILLATORS DETECTOR READOUT WITH SILICON PHOTOMULTIPLIERS FOR COSMIC RAYS STUDIES * D. STANCA 1,2 1 National
More informationNuclear Instruments and Methods in Physics Research A
Nuclear Instruments and Methods in Physics Research A ] (]]]]) ]]] ]]] Contents lists available at SciVerse ScienceDirect Nuclear Instruments and Methods in Physics Research A journal homepage: www.elsevier.com/locate/nima
More informationSeminar. BELLE II Particle Identification Detector and readout system. Andrej Seljak advisor: Prof. Samo Korpar October 2010
Seminar BELLE II Particle Identification Detector and readout system Andrej Seljak advisor: Prof. Samo Korpar October 2010 Outline Motivation BELLE experiment and future upgrade plans RICH proximity focusing
More informationStato del progetto RICH di LHCb. CSN1 Lecce, 24 settembre 2003
Stato del progetto RICH di LHCb CSN1 Lecce, 24 settembre 2003 LHCb RICH detectors Particle ID over 1 100 GeV/c provided by 2 RICH detectors RICH2: No major changes since RICH TDR PRR in february 2003 Superstructure
More informationRAPSODI RAdiation Protection with Silicon Optoelectronic Devices and Instruments
RAPSODI RAdiation Protection with Silicon Optoelectronic Devices and Instruments Massimo Caccia Universita dell Insubria Como (Italy) on behalf of The RAPSODI collaboration 11th Topical Seminar on Innovative
More informationSIGNAL RECOVERY: Sensors, Signals, Noise and Information Recovery
SIGNAL RECOVERY: Sensors, Signals, Noise and Information Recovery http://home.deib.polimi.it/cova/ 1 Signal Recovery COURSE OUTLINE Scenery preview: typical examples and problems of Sensors and Signal
More informationRadiation hardness and precision timing study of Silicon Detectors for the CMS High Granularity Calorimeter (HGC)
Radiation hardness and precision timing study of Silicon Detectors for the CMS High Granularity Calorimeter (HGC) Esteban Currás1,2, Marcos Fernández2, Christian Gallrapp1, Marcello Mannelli1, Michael
More informationPCS-150 / PCI-200 High Speed Boxcar Modules
Becker & Hickl GmbH Kolonnenstr. 29 10829 Berlin Tel. 030 / 787 56 32 Fax. 030 / 787 57 34 email: info@becker-hickl.de http://www.becker-hickl.de PCSAPP.DOC PCS-150 / PCI-200 High Speed Boxcar Modules
More informationHighlights of Poster Session I: SiPMs
Highlights of Poster Session I: SiPMs Yuri Musienko* FNAL(USA)/INR(Moscow) NDIP 2011, Lyon, 5.07.2011 Y. Musienko (Iouri.Musienko@cern.ch) 1 Poster Session I 21 contributions on SiPM characterization and
More informationMCP-PMT status. Samo Korpar. University of Maribor and Jožef Stefan Institute, Ljubljana Super KEKB - 3st Open Meeting, 7-9 July 2009
, Ljubljana, 7-9 July 2009 Outline: MCP aging waveform readout (MPPC) summary (slide 1) Aging preliminary news from Photonis Old information: Current performance (no Al protection layer): 50% drop of efficiency
More informationSiPMs as detectors of Cherenkov photons
SiPMs as detectors of Cherenkov photons Peter Križan University of Ljubljana and J. Stefan Institute Light07, September 26, 2007 Contents Photon detection for Ring Imaging CHerenkov counters Can G-APDs
More informationMultianode Photo Multiplier Tubes as Photo Detectors for Ring Imaging Cherenkov Detectors
Multianode Photo Multiplier Tubes as Photo Detectors for Ring Imaging Cherenkov Detectors F. Muheim a edin]department of Physics and Astronomy, University of Edinburgh Mayfield Road, Edinburgh EH9 3JZ,
More informationPixel hybrid photon detectors
Pixel hybrid photon detectors for the LHCb-RICH system Ken Wyllie On behalf of the LHCb-RICH group CERN, Geneva, Switzerland 1 Outline of the talk Introduction The LHCb detector The RICH 2 counter Overall
More informationMuons & Particle ID. Muon/PID Studies
Muons & Particle ID Muon/PID Studies Global Simulation Software Dev. - A. Maciel - NIU - Tracking/ID w/µ, π, bb events C. Milstene NIU/FNAL Scintillator Module R&D Overview G. Fisk FNAL MAPMT Tests/Calib/FE
More informationNON-AMPLIFIED HIGH SPEED PHOTODETECTOR USER S GUIDE
NON-AMPLIFIED HIGH SPEED PHOTODETECTOR USER S GUIDE Thank you for purchasing your Non-amplified High Speed Photodetector. This user s guide will help answer any questions you may have regarding the safe
More informationCosmic Rays induced Single Event Effects in Power Semiconductor Devices
Cosmic Rays induced Single Event Effects in Power Semiconductor Devices Giovanni Busatto University of Cassino ITALY Outline Introduction Cosmic rays in Space Cosmic rays at Sea Level Radiation Effects
More informationarxiv: v2 [physics.ins-det] 17 Oct 2015
arxiv:55.9v2 [physics.ins-det] 7 Oct 25 Performance of VUV-sensitive MPPC for Liquid Argon Scintillation Light T.Igarashi, S.Naka, M.Tanaka, T.Washimi, K.Yorita Waseda University, Tokyo, Japan E-mail:
More informationAn Introduction to the Silicon Photomultiplier
An Introduction to the Silicon Photomultiplier The Silicon Photomultiplier (SPM) addresses the challenge of detecting, timing and quantifying low-light signals down to the single-photon level. Traditionally
More informationImplementation of A Nanosecond Time-resolved APD Detector System for NRS Experiment in HEPS-TF
Implementation of A Nanosecond Time-resolved APD Detector System for NRS Experiment in HEPS-TF LI Zhen-jie a ; MA Yi-chao c ; LI Qiu-ju a ; LIU Peng a ; CHANG Jin-fan b ; ZHOU Yang-fan a * a Beijing Synchrotron
More informationPoS(PhotoDet 2012)022
SensL New Fast Timing Silicon Photomultiplier Kevin O`Neill 1 SensL Technologies Limited 6800 Airport Business Park, Cork, Ireland E-mail: koneill@sensl.com Nikolai Pavlov SensL Technologies Limited 6800
More informationSingle Sided and Double Sided Silicon MicroStrip Detector R&D
Single Sided and Double Sided Silicon MicroStrip Detector R&D Tariq Aziz Tata Institute, Mumbai, India SuperBelle, KEK December 10-12, 2008 Indian Effort Mask Design at TIFR, Processing at BEL Single Sided
More informationCOURSE OUTLINE. Introduction Signals and Noise Filtering Sensors: PD6 Single-Photon Avalanche Diodes. Sensors, Signals and Noise 1
Sensors, Signals and Noise 1 COURSE OUTLINE Introduction Signals and Noise Filtering Sensors: PD6 Single-Photon Avalanche Diodes Single-Photon Counting and Timing with Avalanche Diodes 2 Sensitivity limits
More informationAVALANCHE PHOTODIODES FOR THE CMS ELECTROMAGNETIC CALORIMETER
AVALANCHE PHOTODIODES FOR THE CMS ELECTROMAGNETIC CALORIMETER B. Patel, R. Rusack, P. Vikas(email:Pratibha.Vikas@cern.ch) University of Minnesota, Minneapolis, U.S.A. Y. Musienko, S. Nicol, S.Reucroft,
More information1.1 The Muon Veto Detector (MUV)
1.1 The Muon Veto Detector (MUV) 1.1 The Muon Veto Detector (MUV) 1.1.1 Introduction 1.1.1.1 Physics Requirements and General Layout In addition to the straw chambers and the RICH detector, further muon
More informationPractical Guide to Using SiPMs Stefan Gundacker
Practical Guide to Using SiPMs Stefan Gundacker 7th of June 2015 The Silicon Photo Multiplier (SiPM) Array of self quenched Geiger-mode APDs (microcells, SPADs) connected in parallel. Microcell or single
More informationCalibration of Scintillator Tiles with SiPM Readout
EUDET Calibration of Scintillator Tiles with SiPM Readout N. D Ascenzo, N. Feege,, B. Lutz, N. Meyer,, A. Vargas Trevino December 18, 2008 Abstract We report the calibration scheme for scintillator tiles
More informationarxiv: v2 [physics.ins-det] 22 Sep 2011
Silicon Photomultipliers for High Energy Physics Detectors Erika Garutti a a Deutsches Elektronen-Synchrotron (DESY), Hamburg, Germany arxiv:1108.3166v2 [physics.ins-det] 22 Sep 2011 Abstract In this paper
More informationDHCAL Prototype Construction José Repond Argonne National Laboratory
DHCAL Prototype Construction José Repond Argonne National Laboratory Linear Collider Workshop Stanford University March 18 22, 2005 Digital Hadron Calorimeter Fact Particle Flow Algorithms improve energy
More informationInGaAs SPAD BIOMEDICAL APPLICATION INDUSTRIAL APPLICATION ASTRONOMY APPLICATION QUANTUM APPLICATION
InGaAs SPAD The InGaAs Single-Photon Counter is based on InGaAs/InP SPAD for the detection of Near-Infrared single photons up to 1700 nm. The module includes a pulse generator for gating the detector,
More informationHIGH SPEED FIBER PHOTODETECTOR USER S GUIDE
HIGH SPEED FIBER PHOTODETECTOR USER S GUIDE Thank you for purchasing your High Speed Fiber Photodetector. This user s guide will help answer any questions you may have regarding the safe use and optimal
More informationMDS-3 EVALUATION SYSTEM FOR METHANE DETECTION INSTRUCTION MANUAL
MDS-3 EVALUATION SYSTEM FOR METHANE DETECTION INSTRUCTION MANUAL rev. 281014 TABLE OF CONTENTS General Information 3 Application 3 Packaging arrangement 3 Operation conditions 3 Brief Overview of the Components
More informationR & D for Aerogel RICH
1 R & D for Aerogel RICH Ichiro Adachi KEK Proto-Collaboration Meeting March 20, 2008 2 1 st Cherenkov Image detected by 3 hybrid avalanche photon detectors from a beam test About 3:00 AM TODAY Clear image
More information