'Dark current' presentation slideshows

Detectors

Detectors. RIT Course Number 1051-465 Lecture CMOS Detectors . Aims for this lecture. To describe CMOS hybrid and monolithic detectors physical principles operation and performance of CMOS detectors Given modern examples of CMOS detectors . Lecture Outline. CMOS detector definition

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??????? Novel Metal-Insulator-Semiconductor Photodetector

??????? Novel Metal-Insulator-Semiconductor Photodetector. ???????? ?? ?????? ????????????. Introduction LPD Oxynitride Recessed Oxynitride Dots on Self-assembled Ge Quantum Dots Ge/Si Quantum Dot MOS Photodetectors for Optical Communication

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Near-Infrared Astronomy

Near-Infrared Astronomy. 0.8-5 ? m How is it different from the optical? Night sky & thermal emission Atmospheric absorption Detectors Instruments What does this mean? Beam switching/nodding/chopping Careful calibration of data Some data Imaging Spectroscopy. >7.5 magnitudes!.

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CCD based Vertex Detector for GLC

CCD based Vertex Detector for GLC. Yasuhiro Sugimoto KEK KEK/Niigata/Tohoku/Toyama Collaboration @VERTEX2003, Sep. 16, 2003. Outline. Project Overview of GLC Accelerator Detector CCD Vertex Detector Merit/Demerit of CCD at GLC/TESLA R&D Status

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EE 230: Optical Fiber Communication Lecture 11

EE 230: Optical Fiber Communication Lecture 11. Detectors. From the movie Warriors of the Net. Detector Technologies. Features. Layer Structure. Simple, Planar, Low Capacitance Low Quantum Efficiency. MSM (Metal Semiconductor Metal) PIN APD Waveguide. Semiinsulating GaAs.

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EE 230: Optical Fiber Communication Lecture 11

EE 230: Optical Fiber Communication Lecture 11. Detectors. From the movie Warriors of the Net. Detector Technologies. Features. Layer Structure. Simple, Planar, Low Capacitance Low Quantum Efficiency. MSM (Metal Semiconductor Metal) PIN APD Waveguide. Semiinsulating GaAs.

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Photoinjector for the ILC test facility at Fermilab

Photoinjector for the ILC test facility at Fermilab. Sergei Nagaitsev Fermilab May 24, 2007. Fermilab NML plans. Fermilab is constructing the NML facility at the existing building (called New Muon Lab) for the ILC tests and generic accelerator research

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Silicon Microstrip detector Single sided and double sided

Silicon Microstrip detector Single sided and double sided. K.Kameswara rao , Tariq Aziz , Chendvankar , M.R.Patil Tata institute of fundamental research , Mumbai , India Y.P.Prabhakara Rao ? Y. Rejeena Rani Bharat Electronics limited , Bangalore , India. ????????????????????????.

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Contents

An overview of Teledyne DALSA Professional Imaging CCD capabilities Jan Bosiers Teledyne DALSA Professional Imaging High Tech Campus 27, 5656AE Eindhoven, The Netherlands jan.bosiers@teledynedalsa.com. Contents. Introduction to Teledyne DALSA Professional Imaging (TDPI) TDPI CCD Technology

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LYRA Tests and Calibration

LYRA Tests and Calibration. LYRA Meeting Davos 05/06 Oct 2006. Contents. I. From Model to Configuration II. BESSY Campaigns a. Flux Linearity b. Stability, Drift c. LEDs, Dark Current d. Spectral Responsivity e. Homogeneity, Flatfield f. Cadence, Response Time

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BESIII RPC Detector

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Selected experiences of 6 years Rossendorf SRF Gun

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Dark Current, Beam Loss, and Collimation in the LCLS

LCLS. Dark Current, Beam Loss, and Collimation in the LCLS J. Wu , D. Dowell, P. Emma, C. Limborg, J. Schmerge, H. Vincke LCLS FAC Meeting April 7, 2005. Thanks to M. Borland for Elegant code changes in support of these studies. Description of the Study.

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Calculation of radiation produced by dark current in the Cornell ERL

Calculation of radiation produced by dark current in the Cornell ERL. Lisa Nash, University of North Carolina at Chapel Hill Advisor: Val Kostroun. Motivation. Radiation fields from dark current in unknown Measurements will be taken later this month

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Intensified CCDs

Intensified CCDs. seeing the invisible. Intro. The CCD sensor was invented in 1969 by Willard Boyle and George E. Smith of AT&T Bell Labs. Originally intended as a memory device. Terminology. Pixel: Picture Element CCD: Charge-Coupled Device CMOS: Complimentary Metal-Oxide Semiconductor

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Status of the LHCb RPC detector

Status of the LHCb RPC detector. G.C. Roma 2. Changes with respect to Note 2000-053 6 cm strips instead of 3 cm (cost optimization) All gaps same size (standardization) Sensitive area defined by graphite paint GaAs discarded in favor of CMS chip for F/E. Ongoing/planned tests

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Design and development of thin double side silicon microstrip sensors for CBM experiment

Design and development of thin double side silicon microstrip sensors for CBM experiment. Mikhail Merkin Skobeltsyn Institute of Nuclear Physics Moscow State University. 3rd Work Meeting of the CBM-MPD STS Consortium. 3rd Work Meeting of the CBM-MPD STS Consortium. Sensor Geometry.

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Summary of Tests of SIC and SEM as Beam Loss Devices at CTF3

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Using GaP Avalanche Photodiodes for Photon Detection

Using GaP Avalanche Photodiodes for Photon Detection. Abigail Lubow EE Senior Project Fall 2001 and Spring 2002 Advisor: Professor Woodall. Pictures from http://www.roithner-laser.com/UV-PD.html. Background. Avalanche photodiodes (APDs) are high gain photodetectors.

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Ongoing, Upcoming and Planned Experiments in the DC Spark Lab

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