Optical absorption measurements in sapphire

Similar documents
Optical absorption measurements in sapphire

S.M.A.- VIRGO. Large sapphire substrate absorption measurements for LIGO SMA. Université Claude Bernard LYON I IPNL - IN2P3 CNRS.

Highly Efficient and Anomalous Charge Transfer in van der Waals Trilayer Semiconductors

Photothermal Deflection in a Synthetic Sapphire Crystal

Effects of Ultraviolet Irradiation on LIGO Mirror Coating

The study of photo-thermal lensing system and its applications

Final Report for AOARD grant FA Measurement of the third-order nonlinear susceptibility of graphene and its derivatives

Optical Microscopy Study of Topological Insulators Using Ellipsometry

arxiv:gr-qc/ v1 12 Feb 2002

Second-Harmonic Generation Studies of Silicon Interfaces

Supplementary Figures

Near-Infrared Spectroscopy of Nitride Heterostructures EMILY FINAN ADVISOR: DR. OANA MALIS PURDUE UNIVERSITY REU PROGRAM AUGUST 2, 2012

High Optical Power Cavity with an Internal Sapphire Substrate Thermal lensing, thermal compensation & three modes interactions

High-power Cryogenic Yb:YAG Lasers and Optical Particle Targeting for EUV Sources *

Advanced LIGO Status Report

GROUND-STATE HANLE RESONANCES IN CESIUM VAPOR CONFINED IN NANOSCOPIC THIN CELL (progress report)

CHAPTER 7 SUMMARY OF THE PRESENT WORK AND SUGGESTIONS FOR FUTURE WORK

High-power Cryogenic Yb:YAG Lasers and Optical Particle Targeting for EUV Sources *

New Concept of DPSSL

The generation of terahertz frequency radiation by optical rectification

79110 Freiburg, Germany

Observing the Doppler Absorption of Rubidium Using a Tunable Laser Diode System

Next Generation Interferometers

Saturated Absorption Spectroscopy (Based on Teachspin manual)

γ irradiation induced effects on bismuth active centres and related photoluminescence properties of Bi/Er co-doped optical fibers

Spectroscopy tools for PAT applications in the Pharmaceutical Industry

Data collection Strategy. Apurva Mehta

Ultrafast laser-based metrology for micron-scale measurements of thermal transport, coefficient of thermal expansion, and temperature

Basic Photoexcitation and Modulation Spectroscopy

Size-selected Metal Cluster Deposition on Oxide Surfaces: Impact Dynamics and Supported Cluster Chemistry

Laboratory 3&4: Confocal Microscopy Imaging of Single-Emitter Fluorescence and Hanbury Brown and Twiss setup for Photon Antibunching

Measurement of thermal lensing in GaAs induced by 100-W Tm:fier laser

Research Article Photostability of Uranine via Crossed-Beam Thermal Lens Technique

Optogalvanic spectroscopy of the Zeeman effect in xenon

Industrial Applications of Ultrafast Lasers: From Photomask Repair to Device Physics

Some optical properties of hydroxide catalysis bonds

Optical Properties of Thin Semiconductor Films

Elastic Constants and Microstructure of Amorphous SiO 2 Thin Films Studied by Brillouin Oscillations

Supplementary Information. Back-Contacted Hybrid Organic-Inorganic Perovskite Solar Cells

Resonantly Pumped Er:YAG and Er:YAP Lasers

Intraband emission of GaN quantum dots at λ =1.5 μm via resonant Raman scattering

Optical Gain and Multi-Quantum Excitation in Optically Pumped Alkali Atom Rare Gas Mixtures

Temperature coefficient of refractive index of sapphire substrate at cryogenic temperature for interferometric gravitational wave detectors

Transformation dependence of lead zirconate titanate (PZT) as shown by PiezoAFM surface mapping of Sol-gel produced PZT on various substrates.

Sean Corum. Augustana College. Stanford Linear Accelerator Center. Menlo Park, CA. August 13,2002

Timing Applications and User Equipment R. Michael Garvey. Time and Frequency Services with Galileo Workshop. 5-6 December 2005

PD233: Design of Biomedical Devices and Systems

Experimental measurements of coating mechanical loss factors

Very High Third-Order Nonlinear Optical Activities of Intrazeolite PbS Quantum Dots. Supporting Information

Parametric down-conversion

Survey on Laser Spectroscopic Techniques for Condensed Matter

l* = 109 nm Glycerol Clean Water Glycerol l = 108 nm Wavelength (nm)

INTERFEROMETRIC METHOD FOR THE STUDY OF SPATIAL PHASE MODULATION INDUCED BY LIGHT IN DYE-DOPED DNA COMPLEXES

2 Steady-state absorption spectroscopy measurements

Hidden Interfaces and High-Temperature Magnetism in Intrinsic Topological Insulator - Ferromagnetic Insulator Heterostructures

Citation for published version (APA): Mollema, A. K. (2008). Laser cooling, trapping and spectroscopy of calcium isotopes s.n.

Development of measurement technique to evaluate thermal conductivity of thermoelectric Bi 2 Te 3 submicron thin films by photothermal radiometry

NUCLEAR TRANSMUTATION IN DEUTERED PD FILMS IRRADIATED BY AN UV LASER

Graphene Based Saturable Absorber Modelockers at 2µm

Simple strategy for enhancing terahertz emission from coherent longitudinal optical phonons using undoped GaAs/n-type GaAs epitaxial layer structures

The gravitational waves detection: 20 years of research to deliver the LIGO/VIRGO mirrors. Christophe MICHEL on behalf of LMA Team

J. Price, 1,2 Y. Q. An, 1 M. C. Downer 1 1 The university of Texas at Austin, Department of Physics, Austin, TX

6. Laser Doppler Anemometry. Introduction to principles and applications

HYPER-RAYLEIGH SCATTERING AND SURFACE-ENHANCED RAMAN SCATTERING STUDIES OF PLATINUM NANOPARTICLE SUSPENSIONS

Confocal Microscopy Imaging of Single Emitter Fluorescence and Hanbury Brown and Twiss Photon Antibunching Setup

Coherent Raman imaging with fibers: From sources to endoscopes

Slow Light in Crystals

Nanoscale Chemical Imaging with Photo-induced Force Microscopy

AXIOMA experiment. Measurements on Er 3+ :YLF. Guarise Marco. Padova INFN. June 29, 2016

Multiphoton microscopy

Technique of the experiment

Phase Sensitive Faraday Rotation in. and various Diamagnetic liquid Samples

Laser Diodes. Revised: 3/14/14 14: , Henry Zmuda Set 6a Laser Diodes 1

Spectroscopy at nanometer scale

Graphene photodetectors with ultra-broadband and high responsivity at room temperature

Continuous room-temperature operation of optically pumped InGaAs/InGaAsP microdisk lasers

GEO 600: Advanced Techniques in Operation

Laser Excitation Dynamics of Argon Metastables Generated in Atmospheric Pressure Flows by Microwave Frequency Microplasma Arrays

Potassium Titanyl Phosphate(KTiOPO 4, KTP)

Spectroscopy Problem Set February 22, 2018

OPTI 511L Fall A. Demonstrate frequency doubling of a YAG laser (1064 nm -> 532 nm).

Nature Protocols: doi: /nprot Supplementary Figure 1

Ultrafast Dynamics and Single Particle Spectroscopy of Au-CdSe Nanorods

Supporting Information. Optical Scattering Spectral Thermometry and Refractometry of a Single Gold Nanoparticle under CW laser excitation

Structure of Surfaces

Nonlinear ultrafast fiber optic devices based on Carbon Nanotubes

Ruby crystals and the first laser A spectroscopy experiment

Behavior and Energy States of Photogenerated Charge Carriers

Thermal Corrective Devices for Advanced Gravitational Wave Interferometers

WP-3: HHG and ultrafast electron imaging

Plasma Formation and Self-focusing in Continuum Generation

SECOND HARMONIC GENERATION IN PERIODICALLY POLED NONLINEAR CRYSTALS WITH 1064 nm GAUSSIAN LASER PULSES

Real-time ppb CO 2 Impurity Detection by an Advanced FTIR- UVF System

Crystals NLO Crystals LBO

Squeezed Light and Quantum Imaging with Four-Wave Mixing in Hot Atoms

A Photonic Crystal Laser from Solution Based. Organo-Lead Iodide Perovskite Thin Films

SURFACE-DISPLACEMENT IMAGING USING OPTICAL BEAM DEFLECTION. S.E. McBride* and G.C. Wetsel, Jr.* Southern Methodist University Dallas, Texas 75275

Periodic Poling of Stoichiometric Lithium Tantalate for High-Average Power Frequency Conversion

FMM, 15 th Feb Simon Zihlmann

ISA QATAR : 90 th Seminar

Transcription:

Optical absorption measurements in sapphire Alexei Alexandrovski Martin Fejer Roger Route Ginzton Laboratory, Stanford University LIGO-G000242-00-D

Optical absorption measurements in sapphire OUTLINE ¾Background ¾Photothermal technique ¾As-grown sapphire ¾Annealed sapphire ¾How to go below 40 ppm/cm ¾Prospects

Space resolution sample 2w 0 2w 1 probe L eff L β pump L eff = π 2 w 0 sin β α = κ P L eff

Space resolution: surface-to-surface scan Translation Probe Pump Sample ABSORPTION SIGNAL (arb.un) 10 8 6 4 2 0 0 2 4 6 DISTANCE (mm) Example: 3 mm-thick neutral filter, 15%-absorbing Leff = 0.25 mm

Photothermal Common-path Interferometer (PCI) Probe Pump Projecting lens Chopper Sample PD Dump Pump waist 50 µ Chopping frequency 380 Hz (10Hz - 2 khz) Probe waist 120 µ Crossing angle 1 o - 20 o (in air) Pump power 5 W Probe power 0.5 mw ac-component of probe distortion is detected by photodiode + lock-in absorption coefficient of 10-7 cm -1 can be detected with a 5 W pump crossed beams help to avoid false signals from optics and surfaces of the sample

Data on sapphire crystals (1998) Crystal α (ppm/cm) 532nm 1064nm Scattering Fluorescenc e Window 3mmthick 1400* 81 No 2 x 10-3 F, Ti 3+ CS White #0 415* (bulk, anomaly near the surface) 41 (bulk, anomaly near the surface) Large near the surface 1 x 10-3 F, Ti 3+ (bulk) CS White #1 1600 84 No 3 x 10-4 F CS White #2 1310 72 Weak band in the 1 x 10-3 F bulk CS White 1910 129 Yes, broad band 3 x 10-3 F (Perth) near one face CS Hemex 1150 188 No 1 x 10-4 F Ultra 0.1% Ti-doped (reference #2) 0.68/cm (total) 0.145/cm 6400 Yes, macrodefects F, Ti 3+ 0.05% Ti-doped laser rod (reference #1) (thermal part) - 19000** - 0.7F, Ti 3+ * 514 nm ** Absorption measured directly Relative fluorescence brightness estimated with calibrated neutral filters, Ti-doped reference #2 brightness denoted as F

Data on sapphire crystals (1999) Crystal CS White, H 2 - annealed CS White, O 2 - annealed α (ppm/cm) 514nm 1064nm Scattering Fluorescence 605 53 No 2 x 10-4 F 600 (bulk, anomaly near the surface) 47 (bulk, anomaly near the surface) Large near the surface 2 x 10-4 F (bulk) Substrate (TRW) - 66 No - Window 3mmthick 1400* 81 No 2 x 10-3 F, Ti 3+ 0.1% Ti-doped (reference #2) 6400 Yes, macrodefects F, Ti 3+ 0.68/cm (total) 0.145/cm (thermal part) Relative fluorescence brightness estimated with calibrated neutral filters, Ti-doped reference #2 brightness denoted as F

Data on sapphire crystals (2000) Crystal Systems, Inc. Crystal α (ppm/cm) 514nm 1064nm Scattering Fluorescence 1T 1730 124 No 10 x10-5 F 1M 1800 103 No 5 x 10-5 F 1B 1430 91 No 2.5 x 10-5 F 2T 900 57 No 4 x 10-4 F 2M 900 87 No 10 x 10-4 F 2B 1410 92 No 40 x 10-4 F 3T 920 62 No 10 x10-5 F 3M 1470 121 No 5 x 10-5 F 3B 840 66 No 5 x 10-5 F 4T 830 46 No 10 x 10-4 F 4M 1200 126 No 2 x 10-4 F 4B 1200 94 No 1 x 10-4 F Nuclear Research Center Negev, ISRAEL Crystal α (ppm/cm) 514nm 1064nm Scattering Fluorescence 1579 1570 147 No 2 x 10-3 F 1958 1600 140 No 2 x 10-3 F 1741 1560 211 No 2 x 10-3 F

Annealed sapphire data 20 mm-long, H 2 -annealed sample Absorption at 1064 nm, scan from surface to surface 80 70 absorption (ppm/cm) 60 50 40 30 20 53 ppm/cm 10 0 0 100 200 300 400 500 600 distance (a.u.) Reference sample: Ti-doped sapphire with the absorption of 6400 ppm/cm at 1064 nm

Annealed sapphire data 20 mm-long, H 2 -annealed sample Absorption at 514 nm, scan from surface to surface 800 absorption (ppm/cm) 700 600 500 400 300 200 605 ppm/cm 100 0 0 100 200 300 400 500 600 distance (a.u.)

Annealed sapphire data 20 mm-long, O 2 -annealed sample Absorption at 1064 nm, scan from surface to surface 250 absorption (ppm/cm) 200 150 100 50 47 ppm/cm 0 0 100 200 300 400 500 distance (a.u.)

Annealed sapphire data 20 mm-long, O 2 -annealed sample Absorption at 1064 nm, scan from surface to surface 250 absorption (ppm/cm) 200 150 100 50 47 ppm/cm 0 0 100 200 300 400 500 distance (a.u.)

Annealed sapphire data 20 mm-long, O 2 -annealed sample Absorption at 514 nm, scan from surface to surface 1400 1200 absorption (ppm/cm) 1000 800 600 400 200 600 ppm/cm 0 0 100 200 300 400 500 distance (a.u.)

Annealed sapphire data 20 mm-long, O 2 -annealed sample Absorption at 514 nm, scan from surface to surface 1400 1200 absorption (ppm/cm) 1000 800 600 400 200 0 0 100 200 300 400 500 distance (a.u.)

Model O 2 -annealed sample Wrap: no fluorescence, scattering, enhanced absorption Line of scan Core: red fluorescence, no scattering, normal absorption Transition layer: low absorption

Conclusions The best as-grown sapphire shows 40 ppm/cm of absorption at 1064 nm H 2 -annealed sapphire shows no change in absorption, fluorescence or scattering O 2 -annealed sapphire shows a complex response to oxidation with local decrease of both IR and green absorption Defects responsible for current IR and green absorption levels are yet to be identified Proper annealing may offer means to reach the 10-15 ppm/cm level. Further decreases will depend on the ability to identify and eliminate specific defects