Lifetime measurements of DBR and nondbr photocathodes at high laser intensities



Similar documents
Short overview of TEUFEL-project

PUMPED Nd:YAG LASER. Last Revision: August 21, 2007

Radiation Transfer in Environmental Science


Austin Peay State University Department of Chemistry Chem The Use of the Spectrophotometer and Beer's Law

A More Efficient Way to De-shelve 137 Ba +

Towards large dynamic range beam diagnostics and beam dynamics studies. Pavel Evtushenko

THE BOHR QUANTUM MODEL

Lecture 1: Basic Concepts on Absorption and Fluorescence

Recording the Instrument Response Function of a Multiphoton FLIM System

PHOTOELECTRIC EFFECT AND DUAL NATURE OF MATTER AND RADIATIONS

hsfc pro 12 bit ultra speed intensified imaging

Instytut Fizyki Doświadczalnej Wydział Matematyki, Fizyki i Informatyki UNIWERSYTET GDAŃSKI

Computer Vision: Machine Vision Filters. Computer Vision. Optical Filters. 25 August 2014

Improved predictive modeling of white LEDs with accurate luminescence simulation and practical inputs

GRID AND PRISM SPECTROMETERS

Raman Spectroscopy. 1. Introduction. 2. More on Raman Scattering. " scattered. " incident

Recent Measurements and Plans for the SLAC Compton X- Ray Source

Single photon detection with H8500 MAPMTs for the CBM RICH detector*

Silicon, the test mass substrate of tomorrow? Jerome Degallaix The Next Detectors for Gravitational Wave Astronomy Beijing

Spectroscopy and Regions of the Spectrum

INFITEC - A NEW STEREOSCOPIC VISUALISATION TOOL BY WAVELENGTH MULTIPLEX IMAGING

Herausforderungen in der Produktion von Receivern für Parabolrinnenkraftwerke

High Brightness Fiber Coupled Pump Laser Development

Helium-Neon Laser. Figure 1: Diagram of optical and electrical components used in the HeNe laser experiment.

Fundamentals of modern UV-visible spectroscopy. Presentation Materials

Limiting factors in fiber optic transmissions

Characterizing Quantum Dots and Color Centers in Nanodiamonds as Single Emitters

Laser Based Micro and Nanoscale Manufacturing and Materials Processing

# 33. Estimating Laser Diode Lifetimes and Activation Energy

How To Understand Light And Color

Diode-pumped Nd:YAG laser

Molecular Spectroscopy

Laser safety in the lab

Wavelength stabilized high-power diode laser modules

Lab 9: The Acousto-Optic Effect

Client: RENOLIT Italia Srl. Work completion: 01/10/2008 (or after receipt of the weathered samples) Notes: Preliminary Report

A Guide to Acousto-Optic Modulators

Ti:Sapphire Lasers. Tyler Bowman. April 23, 2015

SURFACE MOUNT LED LAMP STANDARD BRIGHT 0606

O6: The Diffraction Grating Spectrometer

5. Scanning Near-Field Optical Microscopy 5.1. Resolution of conventional optical microscopy

BPW34. Silicon PIN Photodiode VISHAY. Vishay Semiconductors

High-Reliability Diode Lasers for Gesture Recognition. Applying Telecommunications Reliability Design to Consumer Electronics

2 Absorbing Solar Energy

The Industry s Most Advanced Sun-Sensing, Adaptive-Tinting Technology For Dynamic Windows

Calculating particle properties of a wave

TIL311 HEXADECIMAL DISPLAY WITH LOGIC

Experiment 5. Lasers and laser mode structure

Blackbody radiation derivation of Planck s radiation low

LASERS in Ophthalmology. Health Care Technology Unit ORBIS Flying Eye Hospital

Blackbody Radiation References INTRODUCTION

Modification of Pd-H 2 and Pd-D 2 thin films processed by He-Ne laser

Excited state interaction in P-OLEDS implications for efficiency and lifetime

Incoherent beam combining using stimulated Brillouin scattering in multimode fibers

Undergraduate Research Academy (URA) Cover Sheet

Fibre Bragg Grating Sensors An Introduction to Bragg gratings and interrogation techniques

Spectral Measurement Solutions for Industry and Research

Reliability investigations Lifetime measurements and degradation mechanisms

Sun to Fiber: a thin film optical funnel for energy conversion and storage

UV/VIS/IR SPECTROSCOPY ANALYSIS OF NANOPARTICLES

Experiment #5: Qualitative Absorption Spectroscopy

Efficiency of a Light Emitting Diode

Recent developments in high bandwidth optical interconnects. Brian Corbett.

Problem Set 6 UV-Vis Absorption Spectroscopy Express the following absorbances in terms of percent transmittance:

Chapter 5. Second Edition ( 2001 McGraw-Hill) 5.6 Doped GaAs. Solution

Atomic Structure: Chapter Problems

Does Quantum Mechanics Make Sense? Size

- thus, the total number of atoms per second that absorb a photon is

GREEN NANOTECHNOLOGY. Geoffrey. Energy in the Built Environment. Solutions for Sustainability and. B. Smith Claes G. Granqvist.

Components for Infrared Spectroscopy. Dispersive IR Spectroscopy

Development of the Extreme Ultraviolet Spectrometer: EXCEED

Raman Scattering Theory David W. Hahn Department of Mechanical and Aerospace Engineering University of Florida

Application Note (A5)

Reflectance Characteristics of Accuflect Light Reflecting Ceramic

Opus: University of Bath Online Publication Store

Zero Width Glass Cutting with CO 2 Laser

Understanding Laser Beam Parameters Leads to Better System Performance and Can Save Money

Advances in Oxide-Confined Vertical Cavity Lasers. Photonics Research Department. Albuquerque, NM (505) phone (505) FAX

Raman Spectroscopy Basics

ELECTRON SPIN RESONANCE Last Revised: July 2007

Major LED manufacturing trends and challenges to support the general lighting application

In In situ study of multilayers reflectivity upon heat treatment under synchrotron radiation. 27th september 2005 ICXOM_05 Frascati 1

Quadrature frequency doubling

Qualifying Photonics for the Space Environment

Designing and Manufacturing Femtoseconds Ultra-broadband Lasers: Proven, Hands-free Reliability

Single Photon Counting Module COUNT -Series

High-Performance Wavelength-Locked Diode Lasers

SLLP G PRODUCT DATASHEET. RoHS Compliant

LBS-300 Beam Sampler for C-mount Cameras. YAG Focal Spot Analysis Adapter. User Notes

Applications of confocal fluorescence microscopy in biological sciences

Air-Cooled, Direct-Diode Laser System. IDL Series

IR Edixeon Emitter. 1W Edixeon

Silicon PIN Photodiode

Data Sheet. HLMP-Yxxx T-1 (3 mm) AlInGaP LED Lamps. Description. Features. Applications. Package Dimension

LZC-00MC40. LedEngin, Inc. High Luminous Efficacy RGB LED Emitter. Key Features. Typical Applications. Description

Silicon NPN Phototransistor

Darrick Chang ICFO The Institute of Photonic Sciences Barcelona, Spain. April 2, 2014

Graphite Furnace AA, Page 1 DETERMINATION OF METALS IN FOOD SAMPLES BY GRAPHITE FURNACE ATOMIC ABSORPTION SPECTROSCOPY (VERSION 1.

Transcription:

Lifetime measurements of DBR and nondbr photocathodes at high laser intensities PST 2009 - Ferrara Eric J. Riehn Collaboration B2 Institut für Kernphysik Johannes Gutenberg-Universität Mainz September 10, 2009

Table of contents 1 Introduction 2 Reflectivity Measurements 3 Heating Experiments 4 Summary & Outlook

Photo current photo current laser power Definition of the quantum yield: QY (λ) = N e = h c N hν e I photo λ laser P laser (1) N e : number of electrons N hν : number of photons I photo : photo current λ laser : wavelength of laser light P laser : power of laser light h, c, e : fundamental constants

Heating of nondbr photo cathodes caused by irradiation Figure: Plot taken from K. Winkler (2002; Mainz)

Structure of a nondbr - photocathode Figure: Structure of SL 7-395 (nondbr)

Structure of a nondbr - photocathode Figure: Structure of SL 7-395 (nondbr)

Structure of a nondbr - photocathode Figure: Structure of SL 7-395 (nondbr)

Structure of a DBR - photocathode Figure: Structure of SL 7-396 (DBR)

Experimental Setup Figure: Setup of the polarized test source PKAT

Determination of the reflectivity in vacuo Reflectivity of the cathode: r cathode = P D1 r glas P D2 (1 r glas ) 2 (2) Reflectivity of the glas: r glas = P D2 P 0 (3)

Determination of the reflectivity in vacuo Reflectivity of the cathode: r cathode = P D1 r glas P D2 (1 r glas ) 2 (2) Reflectivity of the glas: r glas = P D2 P 0 (3)

Results Figure: Reflectivity curves for DBR and nondbr cathodes

Results Figure: Reflectivity curves for DBR and nondbr cathodes

DBR - photocathode as Fabry-Pérot-Interferometer Figure: Structure of SL 7-396 (DBR)

Spectral Quantum Yield Figure: DBR-related resonance features in Quantum Yield

Heating Experiments In a specific wavelength region (here: 780 nm to 860 nm) DBR photo cathodes should not heat as much as a corresponding crystal without mirror and therefore have an extended lifetime.

Lifetime Figure: Lifetime of DBR SL 7-396H @ 600 mw

Special features to pay attention to The Plateau: no decrease in quantum yield during the first hours/days after activation

Special features to pay attention to The Bump: temporary rise of the quantum yield after increasing the irradiation power

Special features to pay attention to The Drop-Off: continuing (even accelerated) decrease of the quantum yield after decreasing the irradiation power

Lifetime Measurements Figure: Results from irradiation measurements

Lifetime Measurements Figure: Results from irradiation measurements

Lifetime Measurements Figure: Results from irradiation measurements

Summary & Outlook DBR-crystals show a resonance caused enhancement of the quantum yield at the working point no difference in polarisation between DBR and nondbr samples Effects of highly intense laser irradiation on DBR-crystals lifetime of DBR-crystals is 6 times higher in comparison to the nondbr-crystals respectively laser power can be increased without reducing the lifetime that much DBR s are a very promising addition to active cooling

Summary & Outlook DBR-crystals show a resonance caused enhancement of the quantum yield at the working point no difference in polarisation between DBR and nondbr samples Effects of highly intense laser irradiation on DBR-crystals lifetime of DBR-crystals is 6 times higher in comparison to the nondbr-crystals respectively laser power can be increased without reducing the lifetime that much DBR s are a very promising addition to active cooling

Summary & Outlook DBR-crystals show a resonance caused enhancement of the quantum yield at the working point no difference in polarisation between DBR and nondbr samples Effects of highly intense laser irradiation on DBR-crystals lifetime of DBR-crystals is 6 times higher in comparison to the nondbr-crystals respectively laser power can be increased without reducing the lifetime that much DBR s are a very promising addition to active cooling

Summary & Outlook DBR-crystals show a resonance caused enhancement of the quantum yield at the working point no difference in polarisation between DBR and nondbr samples Effects of highly intense laser irradiation on DBR-crystals lifetime of DBR-crystals is 6 times higher in comparison to the nondbr-crystals respectively laser power can be increased without reducing the lifetime that much DBR s are a very promising addition to active cooling

Appendix Nonlinear Q.Y. at different laser powers

Appendix Comparison of DBR and nondbr (St. Petersburg)

Appendix Asymmetry Figure: Asymmetry of SL 7-395 and SL 7-395H vs. Wavelenght

Appendix Quantum Yield Figure: Quantum Yield of SL 7-395 and SL 7-395H vs. Wavelenght

Appendix Lifetime of the Cleaning Effekt Figure: QE @ 630 nm vs. the Number of Preparations

Appendix First own Results with Spectrometer

Appendix Thermal Conductivity of the Mount Figure: Standard cathode Mount