Development of Photon Detectors at UC Davis Daniel Ferenc Eckart Lorenz Alvin Laille Physics Department, University of California Davis
|
|
|
- Phebe Gibbs
- 5 years ago
- Views:
Transcription
1 Development of Photon Detectors at UC Davis Daniel Ferenc Eckart Lorenz Alvin Laille Physics Department, University of California Davis Work supported partly by DOE, National Nuclear Security Administration (NNSA), Office of Nonproliferation Research and Engineering
2 Future particle astrophysics projects to study very rare phenomena - Proton Decay - Neutrino Physics - Neutrino Astrophysics - Gamma-ray Astronomy (low detection threshold & wide acceptance angle) - Ultra-high energy cosmic rays (>10 19 ev) - Neutrinoless Double Beta Decay - WIMP Searches
3 SEARCHING FOR RARE AND/OR WEAK RADIATION SOURCES PARTICLE ASTROPHYSICS (new generation of experiments) MEDICAL IMAGING WIDELY ACCESSIBLE MEDICAL DIAGNOSTICS Industrial Mass-Production of Very-large-area cameras NUCLEAR SECURITY (nonproliferation)
4 small pixels small area SCALE Larger pixels HUGE AREA Small animal PET MEDICAL IMAGING Large animal (human) PET Luggage radiation monitoring MARKETS (STEADY, SUBSTANTIAL) SUPER-K NUCLEAR SECURITY PHYSICS ~CONTAINER, TRUCK etc. monitoring UNO, HYPER-K MEMPHIS
5 OUR GOAL A new Technology for Industrial Mass-Production of large photosensor areas, based on modified existing technologies (e.g. the assembly of modern, plasma and field-emission flat-panel TV screens; low production cost ~$1000 per sq. meter) + REAL (non-physics) MARKETS,
6 Several Unconventional Photosensors Flat-Panel ReFerence Camera Concept (Patented) Light Amplifier - general concept ReFerence panels scintillator (fiber) readout QUASAR or SMART PMT in a modified configuration + Geiger-mode APDs SIMPLE Space Imaging Camera Concept for EUSO, OWL, but also ground-based applications (Patented)
7 The Unbeatable Reality of Mr. Liouville Cherenkov angle in water ~40 degrees Full angular coverage Camera surrounds the detector volume
8
9 Cherenkov angle in air < 1 degree, also well defined observational direction, and small angular spread in the EM shower Liouville s theorem allows significant beam area reduction Camera can have a small area MAGIC Telescope Inauguration, October (Photo-W. Ko)
10 Irreducibly Large Illuminated Area strong internal signal concentration Vacuum ( photon photoelectron no more Liouville )
11 OBJECTIVES 1. Large Photosensor Area Coverage High Quantity High Quality Low Price Industrial Mass Production 2. High Detection Efficiency and S/N (collection and quantum efficiency)
12 OBJECTIVES 1. Large Photosensor Area Coverage High Quantity High Quality Low Price Industrial Mass Production WHY NOT ACCOMPLISHED ALREADY???? 2. High Detection Efficiency and S/N
13 Semiconductor Photosensors developed very successfully (but pixel sizes and areas - too small) Vacuum Photosensors (suitable for large-area applications, strong area reduction) did not develop significantly since mid-1960s Why? Because of the Vacuum?
14 Development of Other Vacuum Devices ~1960 ~2000 Production Cost: < $1,000 per m 2
15 1. Dielectric 2. Patterned Resister Layer 3. Cathode Glass 4. Row Metal 5. Emitter Array 6. Single Emitter Cone & Gate Hole 7. Column Metal 8. Focusing Grid 9. Wall 10. Phosphor 11. Black Matrix 12. Aluminum Layer 13. Pixel On 14. Faceplate Glass Candescent
16
17 Flat Panel Camera wishful thinking: Continuous Hybrid Photon Detector (HPD) PiN, APD, something else window electrons vacuum Reflection-Mode Photocathode
18 Problem #1 Electron Optics e e e This doesn t t work!
19 Problem #2 Mechanical Stability (flat plates need supports)
20 Flat-Panel Pixelized Camera Configuration provided by the ReFerence Photosensor Concept
21 Ideal Light Concentrator (takes the maximum of Liouville!) Photoelectrons Photon Photocath PIN, APD, or CINTILLATOR Optimal Electron Lens
22 Ideal Light Concentrator Very Important: Hexagonal Packing Entrance Aperture Photocathode Optimal Electron Lens
23
24 Flat-Panel Honeycomb Sandwich Camera Construction Industrial Production (no glass blowing etc.) Intrinsic Mechanical Stability, Low Buoyancy,..
25 PROTOTYPE DEVELOPMENT UNSEALED 1-PIXEL SEALED PANELS (7 pixels, 5 inch) CYLINDRIC HEXAGONAL Equipment (Candescent, Litton Night Vision) ~$2M SEALED with In/Au SEALED with SOLDER GLASS
26 7-pixel 5-inch ReFerence Flat-Panel Prototype UHV Transfer System : Photocathode deposition Indium/Au/Cr deposition Vacuum sealing
27
28
29 3 rd ReFerence Prototype 3 diameter, single pixel (successfully tested see below)
30 Ideal Ideal Light Light Concentrator Concentrator = OK! Phosphor Screen Photoelectrons Photon Photocath verify Optimal Electron Lens Optimal Electron Lens
31 Phosphor Screen
32 Photocathode
33 XYZ Motion Stage
34
35
36 Strong signal concentration, factor ~ 1500 (one of our goals)
37 Strong signal concentration, factor ~ 1500 (one of our goals) APD Replaces the entire Dynode Column! Provides ~100% Collection Efficiency! Scintillator + Fiber (both of small and comparable diameter good coupling efficiency)
38 From Tubes to Large Flat Panels
39 ReFerence Panel Prototype (under construction)
40 ReFerence Panel Prototype (under construction)
41
42 Currently Aluminum ultimately GLASS
43
44 Evaporation Chamber Sealing Chamber Load-lock Chamber TRANSFER SYSTEM For 5 prototypes Base pressure ~6x10-11 Torr
45 Mass spectrometer Sb evaporator Cs, Na, K dispensers Photocurrent monitor
46 Cs, Na, K dispensers
47 Photon Absorption (Electron Creation) Probability for an Electron to Reach the Vacuum Surface (Random Walk) Photon Photo-Electron Glass Window Photocathode Vacuum Therefore: QE ~ 10-20%
48 Photon Absorption (Electron Creation) Probability for an Electron to Reach the Vacuum Surface (Random Walk) Photon Photo-Electron Vacuum Photocathode (e.g. Substrate, Reflector, ) LOW PRODUCTION COST!
49 UV Photon Absorption (Electron Creation) Surface UV Photon Photo-Electron Vacuum Photocathode Probability for an Electron to Reach the Vacuum Surface (Random Walk) Thin Photocathode on a Reflector, Interference Multilayer Systems Westinghouse, RCA, ITT ~
50 Reflection Mode vs. Transmission Mode Quantum Efficiency Extension into blue & UV ~30-43 % QE bialkali ~ nm (Hamamatsu side-on PMT R7517) Wavelength
51
52
53 Transmission-Reflection (and also light trap)
54 Number of Detected Photons APD PMT TransReFerenceerence ReFerence HPD Single-Photon Resolution
55 Photocathode Cooling - Diminished Dark Current Thermionic emission [e/sec/cm 2 ] Cooling InGaAs S Carlsbad NM WATER Cooling (Peltier)
56 e.g. UNO with Magnetic Field (???) VERY EFFICIENT MAGNETIC SHIELDING Slow electrons
57 Light Amplifier Concept Scintillators + fiber optics NO electronics in the vacuum READOUT APD array Resolution determined outside!!
58 Light Amplifier Concept Scintillators + fiber optics NO electronics in the vacuum READOUT APD array Resolution determined outside!!
59 SMART PMT, QUASAR
60 SMART PMT, QUASAR Hemispherical LIGHT AMPLIFIER Fiber Plate Scintillator Y2SiO5(Ce) Al (100 nm) Geiger-mode APD array 1 photoelectron >15 photons in APD
61
62
63 SMART PMT, QUASAR Pulsed LED+fiber CURRENT SETUP electron SINGLE Geiger-mode APD, 1x1 mm 2 No face-plate low light Collection Efficiency ~1:150
64 Pulsed LED+fiber Geiger-mode APD ZS-2 from Sadygov, MICRON Coax signal 57.4 V power EXTREMELY SIMPLE!
65
66 Very Simple Electronics 57.4 mv 20 kω 1 photo-electron 200 mv 20 kω ZS-2 from Sadygov, MICRON g = 25 1 kω 50 Ω 1 pe 200 mv
67 A Typical Single-Photon Signal in the Geiger-mode APD Amplitude Time 1 photo-electron 200 mv
68 Superposition of many light pulses in the Geiger-mode APD (signal integrated) Amplitude ~5 photo-electrons 1 V Time
69 Superposition of many light pulses in the Geiger-mode APD (full bandwidth) Amplitude Time Note the individual photon structure and decay spectrum of the scintillator
70 Rotating Light Source (LED) Scintillator 30 cm 1 cm IMAGING (even without fiber coupling)
71 CONCLUSIONS Light Amplifier : LIGHT IN-(VACUUM)-LIGHT OUT - CONCENTRATION (photoelectron focusing) - AMPLIFICATION (photoelectron acceleration) ADVANTAGES : No electronic components in the vacuum Extreme Simplicity & Robustness Low cost, mass production Tested - a QUASAR tube + a Geiger-mode APD
72 Light Amplifier Concept Scintillators + fiber optics NO electronics inside!! READOUT APD array Resolution determined outside!!
73 SMART PMT, QUASAR Spherical LIGHT AMPLIFIER Fiber Plate scintillator Al (100 nm) Geiger-mode APD array 1 photoelectron >15 photons in APD
74
The Light Amplifier Concept
The Light Amplifier Concept Daniel Ferenc 1 Eckart Lorenz 1,2 Daniel Kranich 1 Alvin Laille 1 (1) Physics Department, University of California Davis (2) Max Planck Institute, Munich Work supported partly
Development of New Large-Area Photosensors in the USA
Development of New Large-Area Photosensors in the USA @BURLE classical PMTs (separate talk) @UC Davis: (1) ReFerence Flat Panels for mass production (2) Light Amplifiers (flat and spherical) Daniel Ferenc
Development of New Photosensors for Huge Detectors
Development of New Photosensors for Huge Detectors Daniel Ferenc Physics Department, University of California Davis Work supported by National Nuclear Security Administration (NNSA), Office of Nonproliferation
OPTI510R: Photonics. Khanh Kieu College of Optical Sciences, University of Arizona Meinel building R.626
OPTI510R: Photonics Khanh Kieu College of Optical Sciences, University of Arizona kkieu@optics.arizona.edu Meinel building R.626 Photodetectors Introduction Most important characteristics Photodetector
Light Collection. Plastic light guides
Light Collection Once light is produced in a scintillator it must collected, transported, and coupled to some device that can convert it into an electrical signal (PMT, photodiode, ) There are several
Production of HPDs for the LHCb RICH Detectors
Production of HPDs for the LHCb RICH Detectors LHCb RICH Detectors Hybrid Photon Detector Production Photo Detector Test Facilities Test Results Conclusions IEEE Nuclear Science Symposium Wyndham, 24 th
The HPD DETECTOR. Michele Giunta. VLVnT Workshop "Technical Aspects of a Very Large Volume Neutrino Telescope in the Mediterranean Sea"
The HPD DETECTOR VLVnT Workshop "Technical Aspects of a Very Large Volume Neutrino Telescope in the Mediterranean Sea" In this presentation: The HPD working principles The HPD production CLUE Experiment
Silicon Photomultiplier
Silicon Photomultiplier Operation, Performance & Possible Applications Slawomir Piatek Technical Consultant, Hamamatsu Corp. Introduction Very high intrinsic gain together with minimal excess noise make
Detectors for microscopy - CCDs, APDs and PMTs. Antonia Göhler. Nov 2014
Detectors for microscopy - CCDs, APDs and PMTs Antonia Göhler Nov 2014 Detectors/Sensors in general are devices that detect events or changes in quantities (intensities) and provide a corresponding output,
CHAPTER 9 POSITION SENSITIVE PHOTOMULTIPLIER TUBES
CHAPTER 9 POSITION SENSITIVE PHOTOMULTIPLIER TUBES The current multiplication mechanism offered by dynodes makes photomultiplier tubes ideal for low-light-level measurement. As explained earlier, there
Advances in X-Ray Scintillator Technology Roger D. Durst Bruker AXS Inc.
Advances in X-Ray Scintillator Technology Roger D. Durst Inc. Acknowledgements T. Thorson, Y. Diawara, E. Westbrook, MBC J. Morse, ESRF C. Summers, Georgia Tech/PTCE B. Wagner, Georgia Tech/PTCE V. Valdna,
Pixel 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
Multianode 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,
Scintillation 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,
Chemistry Instrumental Analysis Lecture 7. Chem 4631
Chemistry 4631 Instrumental Analysis Lecture 7 UV to IR Components of Optical Basic components of spectroscopic instruments: stable source of radiant energy transparent container to hold sample device
Use of a Hybrid Photo Detector (HPD) in the MAGIC micro power LIDAR system
Use of a Hybrid Photo Detector (HPD) in the MAGIC micro power LIDAR system Christian Fruck cfruck@ph.tum.de Max-Planck-Institut für Physik LIGHT 11 - Ringberg 03.11.2011 1 / 18 Overview MAGIC uses the
event physics experiments
Comparison between large area PMTs at cryogenic temperature for neutrino and rare Andrea Falcone University of Pavia INFN Pavia event physics experiments Rare event physics experiment Various detectors
Lecture 12 OPTICAL DETECTORS
Lecture 12 OPTICL DETECTOS (eference: Optical Electronics in Modern Communications,. Yariv, Oxford, 1977, Ch. 11.) Photomultiplier Tube (PMT) Highly sensitive detector for light from near infrared ultraviolet
R & 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
5. Scintillation counters
5. Scintillation counters to detect radiation by means of scintillation is among oldest methods of particle detection historical example: particle impinging on ZnS screen -> emission of light flash principle
Properties of Injection-molding Plastic Scinillator for Fiber Readout
Properties of Injection-molding Plastic Scinillator for Fiber Readout Yukihiro Hara Jan. 31th, 2005 Abstract Plastic-scintillator plates with grooves for fibers have been produced by the injectionmolding
5. Scintillation counters
5. Scintillation counters to detect radiation by means of scintillation is among oldest methods of particle detection particle impinging on ZnS screen -> emission of light flash principle of scintillation
A 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
Radiation transducer. ** Modern electronic detectors: Taking the dark current into account, S = kp + bkgnd over the dynamic range.
Radiation transducer ** Radiation transducer (photon detector) Any device that converts an amount of radiation into some other measurable phenomenon. electric signals. - External photoelectric (photomultiplier),
Recent 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
Advancement in development of photomultipliers dedicated to new scintillators studies.
Advancement in development of photomultipliers dedicated to new scintillators studies. Maciej Kapusta, Pascal Lavoutea, Florence Lherbet, Cyril Moussant, Paul Hink INTRODUCTION AND OUTLINE In the validation
Ground-based optical auroral measurements
Ground-based optical auroral measurements FYS 3610 Background Ground-based optical measurements provides a unique way to monitor spatial and temporal variation of auroral activity at high resolution up
Working Towards Large Area, Picosecond-Level Photodetectors
Working Towards Large Area, Picosecond-Level Photodetectors Matthew Wetstein - Enrico Fermi Institute, University of Chicago HEP Division, Argonne National Lab Introduction: What If? Large Water-Cherenkov
CCDS. Lesson I. Wednesday, August 29, 12
CCDS Lesson I CCD OPERATION The predecessor of the CCD was a device called the BUCKET BRIGADE DEVICE developed at the Phillips Research Labs The BBD was an analog delay line, made up of capacitors such
Wavelength-shifting Optical Module (WOM)
Wavelength-shifting Optical Module (WOM) Vincenzo Di Lorenzo HAP Workshop: Advanced Technologies Mainz 2016-02-02 Cherenkov light Increase the energy resolution decreasing the energy threshold Cherenkov
Page 1. Ground-based optical auroral measurements. Background. CCD All-sky Camera with filterwheel. Image intensifier
Ground-based optical auroral measurements FYS 3610 Background Ground-based optical measurements provides a unique way to monitor spatial and temporal variation of auroral activity at high resolution up
Components of Optical Instruments. Chapter 7_III UV, Visible and IR Instruments
Components of Optical Instruments Chapter 7_III UV, Visible and IR Instruments 1 Grating Monochromators Principle of operation: Diffraction Diffraction sources: grooves on a reflecting surface Fabrication:
HF Upgrade Studies: Characterization of Photo-Multiplier Tubes
HF Upgrade Studies: Characterization of Photo-Multiplier Tubes 1. Introduction Photomultiplier tubes (PMTs) are very sensitive light detectors which are commonly used in high energy physics experiments.
Chemistry 985. Some constants: q e 1.602x10 19 Coul, ɛ x10 12 F/m h 6.626x10 34 J-s, c m/s, 1 atm = 760 Torr = 101,325 Pa
Chemistry 985 Fall, 2o17 Distributed: Mon., 17 Oct. 17, 8:30AM Exam # 1 OPEN BOOK Due: 17 Oct. 17, 10:00AM Some constants: q e 1.602x10 19 Coul, ɛ 0 8.854x10 12 F/m h 6.626x10 34 J-s, c 299 792 458 m/s,
EE119 Introduction to Optical Engineering Fall 2009 Final Exam. Name:
EE119 Introduction to Optical Engineering Fall 2009 Final Exam Name: SID: CLOSED BOOK. THREE 8 1/2 X 11 SHEETS OF NOTES, AND SCIENTIFIC POCKET CALCULATOR PERMITTED. TIME ALLOTTED: 180 MINUTES Fundamental
Silicon 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
Development of an atmospheric Cherenkov era for the CANGAROO-III experiment
The Universe Viewed in Gamma-Rays 1 imaging cam- Development of an atmospheric Cherenkov era for the CANGAROO-III experiment S. Kabuki, K. Tsuchiya, K. Okumura, R. Enomoto, T. Uchida, and H. Tsunoo Institute
Tutors 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
Total 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
IV DETECTORS. Daguerrotype of the Moon, John W. Draper. March 26, 1840 New York
IV DETECTORS Lit.: C.R.Kitchin: Astrophysical Techniques, 2009 C.D.Mckay: CCD s in Astronomy, Ann.Rev. A.&A. 24, 1986 G.H.Rieke: Infrared Detector Arrays for Astronomy, Ann.Rev. A&A 45, 2007 up to 1837:
Spectroscopy in the UV and Visible: Instrumentation. Spectroscopy in the UV and Visible: Instrumentation
Spectroscopy in the UV and Visible: Instrumentation Typical UV-VIS instrument 1 Source - Disperser Sample (Blank) Detector Readout Monitor the relative response of the sample signal to the blank Transmittance
PMT tests at UMD. Vlasios Vasileiou Version st May 2006
PMT tests at UMD Vlasios Vasileiou Version 1.0 1st May 2006 Abstract This memo describes the tests performed on three Milagro PMTs in UMD. Initially, pulse-height distributions of the PMT signals were
Design and Simulation of N-Substrate Reverse Type Ingaasp/Inp Avalanche Photodiode
International Refereed Journal of Engineering and Science (IRJES) ISSN (Online) 2319-183X, (Print) 2319-1821 Volume 2, Issue 8 (August 2013), PP.34-39 Design and Simulation of N-Substrate Reverse Type
1.1 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
Contents. 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
O.H.W. Siegmund, Experimental Astrophysics Group, Space Sciences Laboratory, 7 Gauss Way, University of California, Berkeley, CA 94720
O.H.W. Siegmund, a Experimental Astrophysics Group, Space Sciences Laboratory, 7 Gauss Way, University of California, Berkeley, CA 94720 Microchannel Plate Development Efforts Microchannel Plates large
Properties of a Detector
Properties of a Detector Quantum Efficiency fraction of photons detected wavelength and spatially dependent Dynamic Range difference between lowest and highest measurable flux Linearity detection rate
Performance of High Pixel Density Multi-anode Microchannel Plate Photomultiplier tubes
Performance of High Pixel Density Multi-anode Microchannel Plate Photomultiplier tubes Thomas Conneely R&D Engineer, Photek LTD James Milnes, Jon Lapington, Steven Leach 1 page 1 Company overview Founded
Gas scintillation Glass GEM detector for high-resolution X-ray imaging and CT
Gas scintillation Glass GEM detector for high-resolution X-ray imaging and CT Takeshi Fujiwara 1, Yuki Mitsuya 2, Hiroyuki Takahashi 2, and Hiroyuki Toyokawa 2 1 National Institute of Advanced Industrial
Optical Receivers Theory and Operation
Optical Receivers Theory and Operation Photo Detectors Optical receivers convert optical signal (light) to electrical signal (current/voltage) Hence referred O/E Converter Photodetector is the fundamental
Observational Astronomy
Observational Astronomy Instruments The telescope- instruments combination forms a tightly coupled system: Telescope = collecting photons and forming an image Instruments = registering and analyzing the
The HERA-B Ring Imaging Cerenkov ˇ Detector
The HERA-B Ring Imaging Cerenkov ˇ Detector Requirements Physics Genova, July 3, 1998 Jörg Pyrlik University of Houston HERA-B Collaboration Space Limitations Rate Capabilities and Aging Design Radiator
Positron Emission Tomography
Positron Emission Tomography UBC Physics & Astronomy / PHYS 409 1 Introduction Positron emission tomography (PET) is a non-invasive way to produce the functional 1 image of a patient. It works by injecting
Silicon 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
astro-ph/ Nov 1996
Analog Optical Transmission of Fast Photomultiplier Pulses Over Distances of 2 km A. Karle, T. Mikolajski, S. Cichos, S. Hundertmark, D. Pandel, C. Spiering, O. Streicher, T. Thon, C. Wiebusch, R. Wischnewski
Performance of 8-stage Multianode Photomultipliers
Performance of 8-stage Multianode Photomultipliers Introduction requirements by LHCb MaPMT characteristics System integration Test beam and Lab results Conclusions MaPMT Beetle1.2 9 th Topical Seminar
SiPMs 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
NMI3 Meeting JRA8 MUON-S WP1: Fast Timing Detectors High Magnetic Field µsr Spectrometer Project at PSI Status Report
NMI3 - Integrated Infrastructure Initiative for Neutron Scattering and Muon Spectroscopy NMI3 Meeting 26.-29.9.05 JRA8 MUON-S WP1: Fast Timing Detectors High Magnetic Field µsr Spectrometer Project at
Learning Objectives. Understand how light is generated in a scintillator. Understand how light is transmitted to a PMT
Learning Objectives Understand the basic operation of CROP scintillation counters and photomultiplier tubes (PMTs) and their use in measuring cosmic ray air showers Understand how light is generated in
An 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
arxiv:hep-ex/ v1 19 Apr 2002
STUDY OF THE AVALANCHE TO STREAMER TRANSITION IN GLASS RPC EXCITED BY UV LIGHT. arxiv:hep-ex/0204026v1 19 Apr 2002 Ammosov V., Gapienko V.,Kulemzin A., Semak A.,Sviridov Yu.,Zaets V. Institute for High
Silicon 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
A Study of Silicon Photomultiplier Sensor Prototypes for Readout of a Scintillating Fiber / Lead Sheet Barrel Calorimeter
2007 IEEE Nuclear Science Symposium Conference Record N41-6 A Study of Silicon Photomultiplier Sensor Prototypes for Readout of a Scintillating Fiber / Lead Sheet Barrel Calorimeter Carl J. Zorn Abstract:
Advanced Materials Research Vol
Advanced Materials Research Vol. 1084 (2015) pp 162-167 Submitted: 22.08.2014 (2015) Trans Tech Publications, Switzerland Revised: 13.10.2014 doi:10.4028/www.scientific.net/amr.1084.162 Accepted: 22.10.2014
Radionuclide Imaging MII 3073 RADIONUCLIDE IMAGING SYSTEM
Radionuclide Imaging MII 3073 RADIONUCLIDE IMAGING SYSTEM Preamplifiers and amplifiers The current from PMT must be further amplified before it can be processed and counted (the number of electrons yielded
Stato 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
Components of Optical Instruments
Components of Optical Instruments General Design of Optical Instruments Sources of Radiation Wavelength Selectors (Filters, Monochromators, Interferometers) Sample Containers Radiation Transducers (Detectors)
Characterisation of SiPM Index :
Characterisation of SiPM --------------------------------------------------------------------------------------------Index : 1. Basics of SiPM* 2. SiPM module 3. Working principle 4. Experimental setup
Advances in microchannel plate detectors for UV/visible Astronomy
Advances in microchannel plate detectors for UV/visible Astronomy Dr. O.H.W. Siegmund Space Sciences Laboratory, U.C. Berkeley Advances in:- Photocathodes (GaN, Diamond, GaAs) Microchannel plates (Silicon
DETECTORS Important characteristics: 1) Wavelength response 2) Quantum response how light is detected 3) Sensitivity 4) Frequency of response
DETECTORS Important characteristics: 1) Wavelength response 2) Quantum response how light is detected 3) Sensitivity 4) Frequency of response (response time) 5) Stability 6) Cost 7) convenience Photoelectric
Today s Outline - January 25, C. Segre (IIT) PHYS Spring 2018 January 25, / 26
Today s Outline - January 25, 2018 C. Segre (IIT) PHYS 570 - Spring 2018 January 25, 2018 1 / 26 Today s Outline - January 25, 2018 HW #2 C. Segre (IIT) PHYS 570 - Spring 2018 January 25, 2018 1 / 26 Today
High collection efficiency MCPs for photon counting detectors
High collection efficiency MCPs for photon counting detectors D. A. Orlov, * T. Ruardij, S. Duarte Pinto, R. Glazenborg and E. Kernen PHOTONIS Netherlands BV, Dwazziewegen 2, 9301 ZR Roden, The Netherlands
Nano-structured superconducting single-photon detector
Nano-structured superconducting single-photon detector G. Gol'tsman *a, A. Korneev a,v. Izbenko a, K. Smirnov a, P. Kouminov a, B. Voronov a, A. Verevkin b, J. Zhang b, A. Pearlman b, W. Slysz b, and R.
Performance of Microchannel Plates Fabricated Using Atomic Layer Deposition
Performance of Microchannel Plates Fabricated Using Atomic Layer Deposition Andrey Elagin on behalf of the LAPPD collaboration Introduction Performance (timing) Conclusions Large Area Picosecond Photo
ILC 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
CHAPTER 11 HPD (Hybrid Photo-Detector)
CHAPTER 11 HPD (Hybrid Photo-Detector) HPD (Hybrid Photo-Detector) is a completely new photomultiplier tube that incorporates a semiconductor element in an evacuated electron tube. In HPD operation, photoelectrons
Institute for Particle and Nuclear Studies, High Energy Accelerator Research Organization 1-1 Oho, Tsukuba, Ibaraki , Japan
1, Hiroaki Aihara, Masako Iwasaki University of Tokyo 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-0033, Japan E-mail: chojyuro@gmail.com Manobu Tanaka Institute for Particle and Nuclear Studies, High Energy Accelerator
Engineering Medical Optics BME136/251 Winter 2018
Engineering Medical Optics BME136/251 Winter 2018 Monday/Wednesday 2:00-3:20 p.m. Beckman Laser Institute Library, MSTB 214 (lab) *1/17 UPDATE Wednesday, 1/17 Optics and Photonic Devices III: homework
HAPD Status. S. Nishida KEK. Dec 11, st Open Meeting of the SuperKEKB collaboration. HAPD Status. 1st SuperKEKB Meeting 1
S. Nishida KEK 1st Open Meeting of the SuperKEKB collaboration Dec 11, 2008 1 Contents 144ch HAPD Key Issues Summary I. Adachia, R. Dolenecb, K. Harac, T. Iijimac, H. Ikedad, Y. Ishiie, H. Kawaie, S. Korparb,f,
Peculiarities of the Hamamatsu R photomultiplier tubes
Peculiarities of the Hamamatsu R11410-20 photomultiplier tubes Akimov D.Yu. SSC RF Institute for Theoretical and Experimental Physics of National Research Centre Kurchatov Institute 25 Bolshaya Cheremushkinskaya,
X-ray generation by femtosecond laser pulses and its application to soft X-ray imaging microscope
X-ray generation by femtosecond laser pulses and its application to soft X-ray imaging microscope Kenichi Ikeda 1, Hideyuki Kotaki 1 ' 2 and Kazuhisa Nakajima 1 ' 2 ' 3 1 Graduate University for Advanced
PMT Calibration in the XENON 1T Demonstrator. Abstract
PMT Calibration in the XENON 1T Demonstrator Sarah Vickery Nevis Laboratories, Columbia University, Irvington, NY 10533 USA (Dated: August 2, 2013) Abstract XENON Dark Matter Project searches for the dark
System Options. Magnetic Property Measurement System. AC Susceptibility. AC Susceptibility Specifications
System Options AC Susceptibility Magnetic Property Measurement System Many materials display dissipative mechanisms when exposed to an oscillating magnetic field, and their susceptibility is described
Development of a fast EUV movie camera for Caltech spheromak jet experiments
P1.029 Development of a fast EUV movie camera for Caltech spheromak jet experiments K. B. Chai and P. M. Bellan ` California Institute of Technology kbchai@caltech.edu Caltech Spheromak gun 2 Target: study
Highlights 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
Light gathering Power: Magnification with eyepiece:
Telescopes Light gathering Power: The amount of light that can be gathered by a telescope in a given amount of time: t 1 /t 2 = (D 2 /D 1 ) 2 The larger the diameter the smaller the amount of time. If
SPMMicro. SPMMicro. Low Cost High Gain APD. Low Cost High Gain APD. Page 1
SPMMicro Page 1 Overview Silicon Photomultiplier (SPM) Technology SensL s SPMMicro series is a High Gain APD provided in a variety of miniature, easy to use, and low cost packages. The SPMMicro detector
NM Module Section 2 6 th Edition Christian, Ch. 3
NM 4303 Module Section 2 6 th Edition Christian, Ch. 3 Gas Filled Chamber Voltage Gas filled chamber uses Hand held detectors cutie pie Geiger counter Dose calibrators Cutie pie Chamber voltage in Ionization
PoS(PD07)035. Development of 144 Multi-Anode HPD for Belle Aerogel RICH Photon Detector
Development of 144 Multi-Anode HPD for Belle Aerogel RICH Photon Detector a, R. Dolenec b, A. Petelin b, K. Fujita c, A. Gorišek b, K. Hara c, D. Hayashi c, T. Iijima c, T. Ikado c, H. Kawai d, S. Korpar
LaBr 3 :Ce, the latest crystal for nuclear medicine
10th Topical Seminar on Innovative Particle and Radiation Detectors 1-5 October 2006 Siena, Italy LaBr 3 :Ce, the latest crystal for nuclear medicine Roberto Pani On behalf of SCINTIRAD Collaboration INFN
Contens: 1. Important Notes 1.1 Technical Recommendations 1.2 Mechanical Recommendations 2. Operating the CPM 2.1 Selecting Operating Mode 2.2 Calcula
PerkinElmer Optoelectronics GmbH&Co. KG operating instruction Wenzel-Jaksch-Straße 31 65199 Wiesbaden, Germany Phone: +49 (6 11) 4 92-0 Fax: +49 (6 11) 4 92-159 http://www.perkinelmer.com Heimann Opto
High Performance Thin Film Optical Coatings Technical Reference Document 09/13. Coatings Capabilities. Heat Control - Hot Mirror Filters
Heat Control - Hot Mirror Filters A hot mirror is in essence a thin film coating applied to substrates in an effort to reflect infra-red radiation either as a means to harness the reflected wavelengths
Infrared Detectors an overview
Infrared Detectors an overview Mariangela Cestelli Guidi Sinbad IR beamline @ DaFne EDIT 2015, October 22 Frederick William Herschel (1738 1822) was born in Hanover, Germany but emigrated to Britain at
Status of the large area MCP-PMT in China
1 Feng Gao, Sen Qian Ɨ, Shulin Liu, Zhe Ning, Yifang Wang, Tianchi Zhao, Yuekun Heng, Institute of High Energy Physics, Chinese Academy of Sciences Beijing 100049, China E-mail: qians@ihep.ac.cn Hulin
RF Time Measuring Technique With Picosecond Resolution and Its Possible Applications at JLab. A. Margaryan
RF Time Measuring Technique With Picosecond Resolution and Its Possible Applications at JLab A. Margaryan 1 Contents Introduction RF time measuring technique: Principles and experimental results of recent
arxiv: v1 [astro-ph.im] 6 Aug 2013
![arxiv: v1 [astro-ph.im] 6 Aug 2013](/thumbs/84/89701208.jpg "arxiv: v1 [astro-ph.im] 6 Aug 2013")
Photosensor Characterization for the Cherenkov Telescope Array: Silicon Photomultiplier versus Multi-Anode Photomultiplier Tube A. Bouvier *,1, L. Gebremedhin 1, C. Johnson 1, A. Kuznetsov 1, D. A. Williams
Characterization of 18mm Round and 50mm Square MCP-PMTs
Characterization of 18mm Round and 50mm Square MCP-PMTs Paul Hink, Robert Caracciolo, John Martin, Scott Moulzolf, Charlie Tomasetti, Joseph Wright BURLE INDUSTRIES, INC. 3 rd Beaune Conference New Developments
The equipment used share any common features regardless of the! being measured. Electronic detection was not always available.
The equipment used share any common features regardless of the! being measured. Each will have a light source sample cell! selector We ll now look at various equipment types. Electronic detection was not
Astro-photography. Daguerreotype: on a copper plate
AST 1022L Astro-photography 1840-1980s: Photographic plates were astronomers' main imaging tool At right: first ever picture of the full moon, by John William Draper (1840) Daguerreotype: exposure using
Improvements of the PLD (Pulsed Laser Deposition) Method for Fabricating Photocathodes in ICMOS (Intensified CMOS) Sensors
, pp.46-50 http://dx.doi.org/10.14257/astl.2018.150.12 Improvements of the PLD (Pulsed Laser Deposition) Method for Fabricating Photocathodes in ICMOS (Intensified CMOS) Sensors Dae-Hee Lee 1,2*, Youngsik