Introduction to the physics of the SiPM

Slides:



Advertisements
Similar presentations
Liverpool Group presentation 22/07/2009
Advertisements

Scintillator Tile Hadronic Calorimeter Prototype (analog or semidigital) M.Danilov ITEP(Moscow) CALICE Collaboration LCWS04, Paris.
Study of Silicon Photomultipliers Joëlle Barral, MPI, 25th June 2004.
Special Focus Workshop “Towards 10 ps single soft photon detectors” 2013 IEEE NSS/MIC/RTSD Seoul Sunday Oct 27, 2013.
EE 230: Optical Fiber Communication Lecture 11 From the movie Warriors of the Net Detectors.
PID Nagoya univ1 The possibility of improving TOP counter Nagoya university Yuji Enari.
Fiber-Optic Communications
Semiconductor Optical Single-Photon Diode
Chapter 6 Photodetectors.
V. Semiconductor Photodetectors (PD)
Introduction on SiPM devices
Photon detection Visible or near-visible wavelengths
Single Photon Detectors
Chapter 5 Optical Detector.
Venugopala Rao Dept of CSE SSE, Mukka Electronic Circuits 10CS32.
CHIPP Plenary Meeting, PSI, Oct Dieter Renker PAUL SCHERRER INSTITUT R&D on Photosensors.
Characterization of Silicon Photomultipliers for beam loss monitors Lee Liverpool University weekly meeting.
References Hans Kuzmany : Solid State Spectroscopy (Springer) Chap 5 S.M. Sze: Physics of semiconductor devices (Wiley) Chap 13 PHOTODETECTORS Detection.
H.-G. Moser Max-Planck-Institut for Physics, Munich CALOR 06 Chicago June 5-9, 2006 Silicon Photomultiplier, a new device for low light level photon detection.
PH4705 & ET4305: Digital Sensors
Fast Detectors for Medical and Particle Physics Applications Wilfried Vogel Hamamatsu Photonics France March 8, 2007.
Detector development and physics studies in high energy physics experiments Shashikant Dugad Department of High Energy Physics Review, 3-9 Jan 2008.
Salvatore Tudisco The new generation of SPAD Single Photon Avalanche Diodes arrays I Workshop on Photon Detection - Perugia 2007 LNS LNS.
SiPM: Development and Applications
ALCPG, UT-Arlington January 10th 2003 Preliminary Investigations of Geiger-mode Avalanche Photodiodes for use in HEP Detectors David Warner, Robert J.
Photodetection EDIT Internal photoelectric effect in Si Band gap (T=300K) = 1.12 eV (~1100 nm) More than 1 photoelectron can be created by light in silicon.
References Hans Kuzmany : Solid State Spectroscopy (Springer) Chap 5 S.M. Sze Physics of semiconductor devices (Wiley) Chap 13 PHOTODETECTORS.
9 September 2009 Beam Loss Monitoring with Optical Fibers for Particle Accelerators Joint QUASAR and THz Group Workshop.
R&D of MPPC for T2K experiment PD07 : Photosensor Workshop /6/28 (Thu) S.Gomi T.Nakaya M.Yokoyama H.Kawamuko ( Kyoto University ) T.Nakadaira.
1 SiPM Gain Test SiPM Multiple APD pixels operating at Geiger mode. Output is the sum of the outputs from all APD pixels. Advantages Compact size High.
Study of the MPPC for the GLD Calorimeter readout Satoru Uozumi (Shinshu University) for the GLD Calorimeter Group May 29 – Jun 4 DESY Introduction.
1 Development of Multi-Pixel Photon Counters (1) S.Gomi, T.Nakaya, M.Yokoyama, M.Taguchi, (Kyoto University) T.Nakadaira, K.Yoshimura, (KEK) Oct
1 Stephen SchultzFiber Optics Fall 2005 Semiconductor Optical Detectors.
Photodetectors What is photodetector (PD)? Photodetector properties
10 th Pisa Meeting on Advanced Detectors, Isola d’Elba, May 2006 Development of the first prototypes of Silicon Photomultiplier at ITC-irst N. Dinu, R.
D. Renker, PSI - Vertex 2006 Overview of Developments of Silicon Photomultiplier Detectors Dieter Renker Dieter Renker.
Optical Receivers Theory and Operation
Multipixel Geiger mode photo-sensors (MRS APD’s) Yury Kudenko ISS meeting, KEK, 25 January 2006 INR, Moscow.
Prospects to Use Silicon Photomultipliers for the Astroparticle Physics Experiments EUSO and MAGIC A. Nepomuk Otte Max-Planck-Institut für Physik München.
A.Olchevski, JINR (Dubna) Test Beam studiesof COMPASS ECAL0 Test Beam studies of COMPASS ECAL0 module prototype with MAPD readout ECAL0 Team, JINR, DUBNA.
Study and Development of the Multi-Pixel Photon Counter for the GLD Calorimeter Satoru Uozumi (Shinshu, Japan) on behalf of the GLD Calorimeter Group Oct-9.
CMS ELECTROMAGNETIC CALORIMETER Jean-Pierre Ernenwein OVERVIEW 6th international conference on advanced technology and particle physics Villa Olmo, Como,
Silicon Photomultiplier Development at GRAPES-3 K.C.Ravindran T.I.F.R, OOTY WAPP 2010 Worshop On behalf of GRAPES-3 Collaboration.
Study of the MPPC for the GLD Calorimeter Readout Satoru Uozumi (Shinshu University) for the GLD Calorimeter Group Kobe Introduction Performance.
M.Taguchi and T.Nobuhara(Kyoto) HPK MPPC(Multi Pixel Photon Counter) status T2K280m meeting.
Study of the Radiation Damage of Hamamatsu Silicon Photo Multipliers Wander Baldini Istituto Nazionale di Fisica Nucleare and Universita’ degli Studi di.
D. Renker, PSI G-APD Workshop GSI, PAUL SCHERRER INSTITUT Problems in the Development of Geiger- mode Avalanche Photodiodes Dieter Renker Paul Scherrer.
P. Lecoq CERN2 February ENVISION WP2 Meeting CERN Group contribution to ENVISION WP2 Paul Lecoq CERN, Geneva.
LAL – RAPA- Sept 2008 Vincent CHAUMAT Présentation SiPM. Sommaire : 1- Vue d’ensemble des photo-détecteurs 2- Généralités sur les SiPMs. 3- Caractérisation.
Performance of 1600-pixel MPPC for the GLD Calorimeter Readout Jan. 30(Tue.) Korea-Japan Joint Shinshu Univ. Takashi Maeda ( Univ. of Tsukuba)
Development of Multi-Pixel Photon Counters (1)
Activities at SMI/Vienna in testing the performance of SiPMs
Optical Emitters and Receivers
Electronics & Communication Engineering
Progress report on SiPM development and its applications
Frontier Detectors for Frontier Physics
Theory of the P-N junction
Photo Detectors.
Applications and Circuits
Photodetectors.
V. Semiconductor Photodetectors (PD)
Proof of feasibility of VSiPMT (Vacuum Silicon PhotoMultiplier Tube)
Optical Receivers Theory and Operation
R&D of MPPC for T2K experiment
Optical Receivers 1. Photo Detectors
PRINCIPLE AND WORKING OF A SEMICONDUCTOR LASER
ELECTROMAGNETIC CALORIMETER
T2Kロシアグループに向けたMPPC(SiPM)の性能評価
R&D of MPPC in kyoto M.taguchi.
The MPPC Study for the GLD Calorimeter Readout
Presentation transcript:

Introduction to the physics of the SiPM Angela Intermite Liverpool Group Meeting 28.10.2009

Optical fiber sensor for beam loss monitoring SiPMs Angela Intermite 28.10.2009 2/10 2

Overview What is a Geiger mode avalanche photodiode? How to quench an avalanche? What are the main sources of noise? Dark count Cross talk Afterpulsing Are there some good reasons for preferring SiPM? Angela Intermite 28.10.2009 3/10 3

A reverse p-n junction The operation of a rev p-n junction includes: carrier generation carrier transport and/or multiplication extractions of carriers. Angela Intermite 28.10.2009 4/10

How to quench the avalanche Passive Quenching Advantage - Cheap, very simple circuitry Disadavantage - Slow recovery time Active Quenching Advantage - Very fast transitions Disadavantage - Expensive especially for SiPM with high N Cova et alt. Angela Intermite 28.10.2009 5/10 5

Sources of noise: Dark count Band to band recombination or radiative recombination Trap assisted recombination, also called Shockley Read Hall effect Auger recombination Angela Intermite 28.10.2009 6/10 6

Sources of noise: Cross-talk and Afterpulsing Direct cross-talk Inside the depletion layer. Through reflection Afterpulsing It depends on: Trap concentration in the junction depletion layer number of carriers generated during a Geiger pulse. Angela Intermite 28.10.2009 7/10 7

Some good reasons for choosing SiPM...   VACUUM TECHNOLOGY SOLID-STATE PMT MCP-PMT HPD PN, PIN APD SiPM Photon detection efficiency Blue 20 % 60 % 50 % 30% Green-yellow 40 % 80-90 % 60-70 % 50% Red  6 % 90-100 % 80 % 40% Timing / 10 ph.e  100 ps  10 ps tens ns few ns tens of ps Gain 106-107 106 – 107 3 - 8x103 1  200 105 – 106 Operation voltage 1 kV 3 kV 20 kV 10-100V 100-500V  100 V Operation in the magnetic field  10-3 T Axial magnetic field 2 T  4 T No sensitivity Threshold sensitivity (S/N1) 1 ph. e 100 ph. e 10 ph.e 1 ph.e Shape characteristics sensible bulky compact sensible, bulky robust, compact, mechanically rugged Radiation hardness? Angela Intermite 28.10.2009 8/10

Conclusions Physics of SiPM Quenching circuitry Main sources of noise: Dark count Cross talk Afterpulsing Differences between SiPM, PMT and APD Angela Intermite 28.10.2009 9/10

Thank You !