Stability and Tuning with -S models

Size: px
Start display at page:

Download "Stability and Tuning with -S models"

Transcription

1 Stability and Tuning with -S models where innovation never stops Achieving Stability without Breaking Your Budget

2 Stabilized lasers from Access Laser Company are made from Invar or other materials with high thermal mechanical stability. They also employ a feedback control system regulating the temperature of the laser resonator.

3 Bad news becomes good news Typical CO2 lasers line hop, from one wavelength to another, causing instability in spectrum and power. Reason: the length of the laser cavity drifts constantly under normal ambient conditions. Solution: Control the drift and we will control wavelength and achieve power stability.

4 How it works: Gratingless tuned Take advantage of the interaction between the molecular line spectrum and resonator modes by actively controlling the cavity length of the laser. Tune into single wavelength and stay. Method of tuning: Micrometer Temperature Piezo actuator

5 Spectral Distribution: Gratingless tunable Laser resonators are tightly controlled to force the laser to stay in the desired wavelength μm or μm ( 13 CO2)

6 Warming Up To Stability When the laser is first turned on it heats up. As a result the length of the cavity expands, and the laser goes through a sequence of lines before it is stabilized. This is the warm-up process, which typically takes minutes.

7 Features Common to All -S Models All S model lasers can operate in single longitudinal mode and single transverse mode All S model lasers can operate in a single line You can minimize wavelength and power instability by tuning to the middle of the temperature range for a specific line. The more lines an S model laser can achieve the less temperature range each line has. Lines with a wide range of temperature are easier to achieve and are more stable, and vise versa.

8 Power & Spectrum Considerations to fit your application The smaller the laser the lower the power. The L3S is the shortest with 400mw of output power, and the L20S is the biggest at 20 watts. The smaller the laser, the more lines you ll have (you should notice this trend in the following pages). L3S has lines typically, while L20S has 3-6. It is not practical to stay on one spectral line that has a very narrow range of temperature. Typical applications for S model lasers require one stable line around center of the wavelength band (P20 or R20). -S models offer best spectral purity and frequency stability when water cooled with a good chiller. For L4SL the measured line width is less than 100kHz. Frequency drift is less than 5MHz/min. Line Tracker is an option available for all S models, which improves power stability to ±1%, and enhances frequency stability.

9 Wavelength table of a typical model L3S, 400 mw laser, 14 lines.

10 Wavelength table of a typical model L4S, 1 W laser, 9 lines.

11 Wavelength table of a typical model MeritS, 8 W laser, 6 lines.

12 Wavelength table of a typical model L20-S, 20 W laser, 4 lines

13 The Line Table The line table, which goes with most S lasers is only for reference. In practice you may not achieve the desired line at the given temperature. This is because this table is recorded during ramp up of laser temperature after turn-on. Once the laser stabilizes it temperature range is shifted. The customer, if desire a particular wavelength, will need to find out exactly where that line is in his/her own ambient working environment, by experiment. If the laser is equipped with piezo actuator, then the table is obtained with the piezo set at a single ramp up when the laser is stabilized at a certain room temperature. The most important, and accurate information from a line table is the relative range of spectral lines. The wider the range the more stable the laser can be operating on a line. The range can be temperature or piezo voltage, depending on the specific laser model and options. Another piece of highly useful information is the sequence of spectral lines. Most spectral lines will appear in the sequence as recorded in rising temperature or piezo voltage.

14 Example of Using Line Table Looking at the line table of MeritS on Page 11, we find that 10P20 have the widest range of temperature from 82.3 to 87.5 F. Therefore we chose this line. Suppose by setting the laser body temperature at 84.9 degrees, which should be the middle of the range for 10P20 from the line table, we actually achieved 10P22. The line table shows that 10P22 appears at a lower temperature than 10P20. Therefore we increase the temperature setting to go for 10P20. Once the laser operates in one single wavelength its power is most stable. If the laser operates in a few lines at the same time it can negatively impact its power stability, in addition to compromised spectral purity.

15 Pick the Right Tool for Your Work Do you need linear polarization? L20S is by default linearly polarized in the horizontal direction. Linearly polarization is not default in other models, but can be added to L4S and MeritS Do you want to achieve even better stability? Consider Line Tracker, which provides closed loop feedback. Feel free to us at or call

Wavelength Control and Locking with Sub-MHz Precision

Wavelength Control and Locking with Sub-MHz Precision Wavelength Control and Locking with Sub-MHz Precision A PZT actuator on one of the resonator mirrors enables the Verdi output wavelength to be rapidly tuned over a range of several GHz or tightly locked

More information

L4 Series Operator Manual

L4 Series Operator Manual L4 Series Operator Manual Access Laser Company 917 134 th St SW, Suite A1 Everett, WA 98204 425.582.8674 www.accesslaser.com L4 Series Operator Manual_Rev_J TABLE OF CONTENTS Section Page Company Statement...

More information

Operating longitudinal mode Several Polarization ratio > 100:1. Power. Warranty. 30 <1.5 <5% Near TEM ~4.0 one year

Operating longitudinal mode Several Polarization ratio > 100:1. Power. Warranty. 30 <1.5 <5% Near TEM ~4.0 one year DL CW Blue Violet Laser, 405nm 405 nm Operating longitudinal mode Several Applications: DNA Sequencing Spectrum analysis Optical Instrument Flow Cytometry Interference Measurements Laser lighting show

More information

UNMATCHED OUTPUT POWER AND TUNING RANGE

UNMATCHED OUTPUT POWER AND TUNING RANGE ARGOS MODEL 2400 SF SERIES TUNABLE SINGLE-FREQUENCY MID-INFRARED SPECTROSCOPIC SOURCE UNMATCHED OUTPUT POWER AND TUNING RANGE One of Lockheed Martin s innovative laser solutions, Argos TM Model 2400 is

More information

THE TUNABLE LASER LIGHT SOURCE C-WAVE. HÜBNER Photonics Coherence Matters.

THE TUNABLE LASER LIGHT SOURCE C-WAVE. HÜBNER Photonics Coherence Matters. THE TUNABLE LASER LIGHT SOURCE HÜBNER Photonics Coherence Matters. FLEXIBILITY WITH PRECISION is the tunable laser light source for continuous-wave (cw) emission in the visible and near-infrared wavelength

More information

Power. Warranty. 30 <1.5 <3% Near TEM ~4.0 one year. 50 <1.5 <5% Near TEM ~4.0 one year

Power. Warranty. 30 <1.5 <3% Near TEM ~4.0 one year. 50 <1.5 <5% Near TEM ~4.0 one year DL CW Blue Violet Laser, 405nm 405 nm Operating longitudinal mode Several Applications: DNA Sequencing Spectrum analysis Optical Instrument Flow Cytometry Interference Measurements Laser lighting show

More information

Concepts for High Power Laser Diode Systems

Concepts for High Power Laser Diode Systems Concepts for High Power Laser Diode Systems 1. Introduction High power laser diode systems is a new development within the field of laser diode systems. Pioneer of such laser systems was SDL, Inc. which

More information

Continuous-Wave (CW) Single-Frequency IR Laser. NPRO 125/126 Series

Continuous-Wave (CW) Single-Frequency IR Laser. NPRO 125/126 Series Continuous-Wave (CW) Single-Frequency IR Laser NPRO 125/126 Series www.lumentum.com Data Sheet The Lumentum NPRO 125/126 diode-pumped lasers produce continuous-wave (CW), singlefrequency output at either

More information

taccor Optional features Overview Turn-key GHz femtosecond laser

taccor Optional features Overview Turn-key GHz femtosecond laser taccor Turn-key GHz femtosecond laser Self-locking and maintaining Stable and robust True hands off turn-key system Wavelength tunable Integrated pump laser Overview The taccor is a unique turn-key femtosecond

More information

First Time User Manual

First Time User Manual Fiber Fabry-Perot Tunable Filter FFP-TF2 First Time User Manual Micron Optics Inc. 1852 Century Place NE Atlanta, GA 30345 USA phone 404 325 0005 fax 404 325 4082 www.micronoptics.com Copyright 2009 Micron

More information

Continuous Wave (CW) Single-Frequency IR Laser NPRO 125/126 Series

Continuous Wave (CW) Single-Frequency IR Laser NPRO 125/126 Series COMMERCIAL LASERS Continuous Wave (CW) Single-Frequency IR Laser NPRO 125/126 Series Key Features 1319 or 1064 nm outputs available Fiber-coupled output Proven nonplanar ring oscillator (NPRO) design Superior

More information

Fabry Perot Resonator (CA-1140)

Fabry Perot Resonator (CA-1140) Fabry Perot Resonator (CA-1140) The open frame Fabry Perot kit CA-1140 was designed for demonstration and investigation of characteristics like resonance, free spectral range and finesse of a resonator.

More information

High-Power Femtosecond Lasers

High-Power Femtosecond Lasers High-Power Femtosecond Lasers PHAROS is a single-unit integrated femtosecond laser system combining millijoule pulse energies and high average power. PHAROS features a mechanical and optical design optimized

More information

Optical phase-locked loop for coherent transmission over 500 km using heterodyne detection with fiber lasers

Optical phase-locked loop for coherent transmission over 500 km using heterodyne detection with fiber lasers Optical phase-locked loop for coherent transmission over 500 km using heterodyne detection with fiber lasers Keisuke Kasai a), Jumpei Hongo, Masato Yoshida, and Masataka Nakazawa Research Institute of

More information

Fast Widely-Tunable CW Single Frequency 2-micron Laser

Fast Widely-Tunable CW Single Frequency 2-micron Laser Fast Widely-Tunable CW Single Frequency 2-micron Laser Charley P. Hale and Sammy W. Henderson Beyond Photonics LLC 1650 Coal Creek Avenue, Ste. B Lafayette, CO 80026 Presented at: 18 th Coherent Laser

More information

Single-mode lasing in PT-symmetric microring resonators

Single-mode lasing in PT-symmetric microring resonators CREOL The College of Optics & Photonics Single-mode lasing in PT-symmetric microring resonators Matthias Heinrich 1, Hossein Hodaei 2, Mohammad-Ali Miri 2, Demetrios N. Christodoulides 2 & Mercedeh Khajavikhan

More information

Single Frequency Laser/Single Longitudinal Mode Laser

Single Frequency Laser/Single Longitudinal Mode Laser Single Frequency Laser/Single Longitudinal Mode Laser MSL series lasers with the characteristics of ultra compact, long lifetime, low cost and easy operating, which are used in DNA sequencing, flow cytometry,

More information

High Power and Energy Femtosecond Lasers

High Power and Energy Femtosecond Lasers High Power and Energy Femtosecond Lasers PHAROS is a single-unit integrated femtosecond laser system combining millijoule pulse energies and high average powers. PHAROS features a mechanical and optical

More information

SPECIFICATIONS. Tunable Single-Frequency Laser Box. DL-BF12-CLSwwwB-Sxxxx-yy-zz

SPECIFICATIONS. Tunable Single-Frequency Laser Box. DL-BF12-CLSwwwB-Sxxxx-yy-zz DENSELIGHT SEMICONDUCTORS PTE. LTD. 6 Changi North St. 2, S498831 SINGAPORE Tel: (65) 64154488 Fax: (65) 64157988 www.denselight.com SPECIFICATIONS Tunable Single-Frequency Laser Box DenseLight Semiconductors

More information

Narrow line diode laser stacks for DPAL pumping

Narrow line diode laser stacks for DPAL pumping Narrow line diode laser stacks for DPAL pumping Tobias Koenning David Irwin, Dean Stapleton, Rajiv Pandey, Tina Guiney, Steve Patterson DILAS Diode Laser Inc. Joerg Neukum Outline Company overview Standard

More information

R. J. Jones Optical Sciences OPTI 511L Fall 2017

R. J. Jones Optical Sciences OPTI 511L Fall 2017 R. J. Jones Optical Sciences OPTI 511L Fall 2017 Semiconductor Lasers (2 weeks) Semiconductor (diode) lasers are by far the most widely used lasers today. Their small size and properties of the light output

More information

RFID Systems: Radio Architecture

RFID Systems: Radio Architecture RFID Systems: Radio Architecture 1 A discussion of radio architecture and RFID. What are the critical pieces? Familiarity with how radio and especially RFID radios are designed will allow you to make correct

More information

Actively Stabilized Scanning Single-Frequency. Ti:Sa /Dye Ring Laser External Doubling Ring Ti:Sa /Dye Standing Wave Laser

Actively Stabilized Scanning Single-Frequency. Ti:Sa /Dye Ring Laser External Doubling Ring Ti:Sa /Dye Standing Wave Laser Actively Stabilized Scanning Single-Frequency Ti:Sa /Dye Ring Laser External Doubling Ring Ti:Sa /Dye Standing Wave Laser Ring Laser with the following options Broadband Ring Laser Passively Stabilized

More information

Fiber Coupled Laser Sources

Fiber Coupled Laser Sources Fiber Coupled Laser Sources Operating Manual FIBER LASER SOURCE LD PWR ADJ. OFF mw LASER APERTURE ENABLE LASER POWER FIBER DFB LASER SOURCE LD PWR ADJ. TEMP. ADJUST OFF LASER APERTURE POWER ENABLE LASER

More information

FFP-TF2 Fiber Fabry-Perot Tunable Filter Technical Reference

FFP-TF2 Fiber Fabry-Perot Tunable Filter Technical Reference FFP-TF2 Fiber Fabry-Perot Tunable Filter MICRON OPTICS, INC. 1852 Century Place NE Atlanta, GA 3345 Tel. (44) 325-5 Fax. (44) 325-482 Internet: www.micronoptics.com Email: sales@micronoptics.com Rev_A

More information

Tunable Laser. PZT Cavity Tuning

Tunable Laser. PZT Cavity Tuning Coherent Specialty CO 2 Laser Tunable Laser GEM Select 100 Specialty CO 2 Waveguide Laser The GEM Select 100 Advantage The GEM Select 100 Specialty laser brings fieldproven technology for both laboratory

More information

Laser Diode. Photonic Network By Dr. M H Zaidi

Laser Diode. Photonic Network By Dr. M H Zaidi Laser Diode Light emitters are a key element in any fiber optic system. This component converts the electrical signal into a corresponding light signal that can be injected into the fiber. The light emitter

More information

A new picosecond Laser pulse generation method.

A new picosecond Laser pulse generation method. PULSE GATING : A new picosecond Laser pulse generation method. Picosecond lasers can be found in many fields of applications from research to industry. These lasers are very common in bio-photonics, non-linear

More information

Powerful Single-Frequency Laser System based on a Cu-laser pumped Dye Laser

Powerful Single-Frequency Laser System based on a Cu-laser pumped Dye Laser Powerful Single-Frequency Laser System based on a Cu-laser pumped Dye Laser V.I.Baraulya, S.M.Kobtsev, S.V.Kukarin, V.B.Sorokin Novosibirsk State University Pirogova 2, Novosibirsk, 630090, Russia ABSTRACT

More information

Aurora II Integra OPO Integrated Nd:YAG Pumped Type II BBO OPO

Aurora II Integra OPO Integrated Nd:YAG Pumped Type II BBO OPO L i t r o n T o t a l L a s e r C a p a b i l i t y Aurora II Integra OPO Integrated Nd:YAG Pumped Type II BBO OPO The Litron Aurora II Integra is an innovative, fully motorised, type II BBO OPO and Nd:YAG

More information

Chapter 1 Introduction

Chapter 1 Introduction Chapter 1 Introduction 1-1 Preface Telecommunication lasers have evolved substantially since the introduction of the early AlGaAs-based semiconductor lasers in the late 1970s suitable for transmitting

More information

Tapered Amplifiers. For Amplification of Seed Sources or for External Cavity Laser Setups. 750 nm to 1070 nm COHERENT.COM DILAS.

Tapered Amplifiers. For Amplification of Seed Sources or for External Cavity Laser Setups. 750 nm to 1070 nm COHERENT.COM DILAS. Tapered Amplifiers For Amplification of Seed Sources or for External Cavity Laser Setups 750 nm to 1070 nm COHERENT.COM DILAS.COM Welcome DILAS Semiconductor is now part of Coherent Inc. With operations

More information

FFP-C Fiber Fabry-Perot Controller OPERATING INSTRUCTIONS. Version 1.0 MICRON OPTICS, INC.

FFP-C Fiber Fabry-Perot Controller OPERATING INSTRUCTIONS. Version 1.0 MICRON OPTICS, INC. FFP-C Fiber Fabry-Perot Controller OPERATING INSTRUCTIONS Version 1.0 MICRON OPTICS, INC. 1852 Century Place NE Atlanta, GA 30345 USA Tel (404) 325-0005 Fax (404) 325-4082 www.micronoptics.com Page 2 Table

More information

SodiumStar 20/2 High Power cw Tunable Guide Star Laser

SodiumStar 20/2 High Power cw Tunable Guide Star Laser SodiumStar 20/2 High Power cw Tunable Guide Star Laser Laser Guide Star Adaptive Optics Facilities LIDAR Atmospheric Monitoring Laser Cooling SodiumStar 20/2 High Power cw Tunable Guide Star Laser Existing

More information

CO2 laser heating system for thermal compensation of test masses in high power optical cavities. Submitted by: SHUBHAM KUMAR to Prof.

CO2 laser heating system for thermal compensation of test masses in high power optical cavities. Submitted by: SHUBHAM KUMAR to Prof. CO2 laser heating system for thermal compensation of test masses in high power optical cavities. Submitted by: SHUBHAM KUMAR to Prof. DAVID BLAIR Abstract This report gives a description of the setting

More information

A Narrow-Band Tunable Diode Laser System with Grating Feedback

A Narrow-Band Tunable Diode Laser System with Grating Feedback A Narrow-Band Tunable Diode Laser System with Grating Feedback S.P. Spirydovich Draft Abstract The description of diode laser was presented. The tuning laser system was built and aligned. The free run

More information

AN X-BAND FREQUENCY AGILE SOURCE WITH EXTREMELY LOW PHASE NOISE FOR DOPPLER RADAR

AN X-BAND FREQUENCY AGILE SOURCE WITH EXTREMELY LOW PHASE NOISE FOR DOPPLER RADAR AN X-BAND FREQUENCY AGILE SOURCE WITH EXTREMELY LOW PHASE NOISE FOR DOPPLER RADAR H. McPherson Presented at IEE Conference Radar 92, Brighton, Spectral Line Systems Ltd England, UK., October 1992. Pages

More information

IST IP NOBEL "Next generation Optical network for Broadband European Leadership"

IST IP NOBEL Next generation Optical network for Broadband European Leadership DBR Tunable Lasers A variation of the DFB laser is the distributed Bragg reflector (DBR) laser. It operates in a similar manner except that the grating, instead of being etched into the gain medium, is

More information

venteon Ultra-short pulse oscillators

venteon Ultra-short pulse oscillators venteon Ultra-short pulse oscillators Few-cycle femtosecond pulses Stable performance with minimal intervention Measured pulses approaching transform limit Broadest spectral bandwidth commercially available

More information

CHAPTER 5 FINE-TUNING OF AN ECDL WITH AN INTRACAVITY LIQUID CRYSTAL ELEMENT

CHAPTER 5 FINE-TUNING OF AN ECDL WITH AN INTRACAVITY LIQUID CRYSTAL ELEMENT CHAPTER 5 FINE-TUNING OF AN ECDL WITH AN INTRACAVITY LIQUID CRYSTAL ELEMENT In this chapter, the experimental results for fine-tuning of the laser wavelength with an intracavity liquid crystal element

More information

Stable dual-wavelength oscillation of an erbium-doped fiber ring laser at room temperature

Stable dual-wavelength oscillation of an erbium-doped fiber ring laser at room temperature Stable dual-wavelength oscillation of an erbium-doped fiber ring laser at room temperature Donghui Zhao.a, Xuewen Shu b, Wei Zhang b, Yicheng Lai a, Lin Zhang a, Ian Bennion a a Photonics Research Group,

More information

Designing for Femtosecond Pulses

Designing for Femtosecond Pulses Designing for Femtosecond Pulses White Paper PN 200-1100-00 Revision 1.1 July 2013 Calmar Laser, Inc www.calmarlaser.com Overview Calmar s femtosecond laser sources are passively mode-locked fiber lasers.

More information

Tunable Laser Kits. Features

Tunable Laser Kits. Features Thorlabs' Tunable Laser Kits are designed for superior cavity construction flexibility and high-stability performance. Available in either a Littrow or Littman configuration, these external cavity laser

More information

Ph 77 ADVANCED PHYSICS LABORATORY ATOMIC AND OPTICAL PHYSICS

Ph 77 ADVANCED PHYSICS LABORATORY ATOMIC AND OPTICAL PHYSICS Ph 77 ADVANCED PHYSICS LABORATORY ATOMIC AND OPTICAL PHYSICS Diode Laser Characteristics I. BACKGROUND Beginning in the mid 1960 s, before the development of semiconductor diode lasers, physicists mostly

More information

visibility values: 1) V1=0.5 2) V2=0.9 3) V3=0.99 b) In the three cases considered, what are the values of FSR (Free Spectral Range) and

visibility values: 1) V1=0.5 2) V2=0.9 3) V3=0.99 b) In the three cases considered, what are the values of FSR (Free Spectral Range) and EXERCISES OF OPTICAL MEASUREMENTS BY ENRICO RANDONE AND CESARE SVELTO EXERCISE 1 A CW laser radiation (λ=2.1 µm) is delivered to a Fabry-Pérot interferometer made of 2 identical plane and parallel mirrors

More information

LRS-0532-PF SERIES INFORMATION SHEET

LRS-0532-PF SERIES INFORMATION SHEET 216-5 ADRIAN AVE. TORONTO, ON, CANADA M6N5G4 T. 1.416.729.7976 F. 1.480.247.4864 SALES@LASERGLOW.COM LRS-0532-PF SERIES INFORMATION SHEET The LRS-0532 Series of Diode-Pumped Solid-State (DPSS) Lasers are

More information

First step in the industry-based development of an ultra-stable optical cavity for space applications

First step in the industry-based development of an ultra-stable optical cavity for space applications First step in the industry-based development of an ultra-stable optical cavity for space applications B. Argence, E. Prevost, T. Levêque, R. Le Goff, S. Bize, P. Lemonde and G. Santarelli LNE-SYRTE,Observatoire

More information

ignis TECHNICAL DATA SHEET high specification red laser CW 660nm laser Extremely low noise Power 500mW

ignis TECHNICAL DATA SHEET high specification red laser CW 660nm laser Extremely low noise Power 500mW CW 660nm laser Extremely low noise Power 500mW TECHNICAL DATA SHEET The high specification 660nm laser Overview The at 660nm and 500mW is among the most powerful and compact red lasers available today

More information

US-Patent 5,867,512 US-Patent 6,297,066 Power and Stability High Powered Littman / Metcalf External Cavity Diode Laser http://www.sacher-laser.com How does our Laser achieve high stability? Initial State

More information

Low Noise High Power Ultra-Stable Diode Pumped Er-Yb Phosphate Glass Laser

Low Noise High Power Ultra-Stable Diode Pumped Er-Yb Phosphate Glass Laser Low Noise High Power Ultra-Stable Diode Pumped Er-Yb Phosphate Glass Laser R. van Leeuwen, B. Xu, L. S. Watkins, Q. Wang, and C. Ghosh Princeton Optronics, Inc., 1 Electronics Drive, Mercerville, NJ 8619

More information

Actively Stabilized Scanning Single Frequency. Ti:Sa /Dye Ring Laser

Actively Stabilized Scanning Single Frequency. Ti:Sa /Dye Ring Laser Actively Stabilized Scanning Single Frequency Ti:Sa /Dye Ring Laser Ring Laser with the following options Broadband Ring Laser Passive Stabilized Scanning Single Frquency Ring Laser Activel Stabilized

More information

PGx11 series. Transform Limited Broadly Tunable Picosecond OPA APPLICATIONS. Available models

PGx11 series. Transform Limited Broadly Tunable Picosecond OPA APPLICATIONS. Available models PGx1 PGx3 PGx11 PT2 Transform Limited Broadly Tunable Picosecond OPA optical parametric devices employ advanced design concepts in order to produce broadly tunable picosecond pulses with nearly Fourier-transform

More information

Pound-Drever-Hall Locking of a Chip External Cavity Laser to a High-Finesse Cavity Using Vescent Photonics Lasers & Locking Electronics

Pound-Drever-Hall Locking of a Chip External Cavity Laser to a High-Finesse Cavity Using Vescent Photonics Lasers & Locking Electronics of a Chip External Cavity Laser to a High-Finesse Cavity Using Vescent Photonics Lasers & Locking Electronics 1. Introduction A Pound-Drever-Hall (PDH) lock 1 of a laser was performed as a precursor to

More information

VCSELs With Enhanced Single-Mode Power and Stabilized Polarization for Oxygen Sensing

VCSELs With Enhanced Single-Mode Power and Stabilized Polarization for Oxygen Sensing VCSELs With Enhanced Single-Mode Power and Stabilized Polarization for Oxygen Sensing Fernando Rinaldi and Johannes Michael Ostermann Vertical-cavity surface-emitting lasers (VCSELs) with single-mode,

More information

CA92009-O O Band (1260 ~ 1360 nm) Tunable Laser Source

CA92009-O O Band (1260 ~ 1360 nm) Tunable Laser Source CA92009-O O Band (1260 ~ 1360 nm) Tunable Laser Source Specification Ver 1.00 (Nov., 2016) www.ali-us.com Product Description This specification describes and defines Advanced Lab Instruments CA92009-O

More information

Two-Mode Frequency Stabilization of an Internal-Mirror 612 nm He-Ne Laser

Two-Mode Frequency Stabilization of an Internal-Mirror 612 nm He-Ne Laser Proc. Natl. Sci. Counc. ROC(A) Vol. 24, No. 4, 2000. pp. 274-278 Two-Mode Frequency Stabilization of an Internal-Mirror 612 nm He-Ne Laser TONG-LONG HUANG *,**, YI-SHI CHEN *, JOW-TSONG SHY *,, AND HAI-PEI

More information

An Optical Characteristic Testing System for the Infrared Fiber in a Transmission Bandwidth 9-11μm

An Optical Characteristic Testing System for the Infrared Fiber in a Transmission Bandwidth 9-11μm An Optical Characteristic Testing System for the Infrared Fiber in a Transmission Bandwidth 9-11μm Ma Yangwu *, Liang Di ** Center for Optical and Electromagnetic Research, State Key Lab of Modern Optical

More information

DESIGN OF COMPACT PULSED 4 MIRROR LASER WIRE SYSTEM FOR QUICK MEASUREMENT OF ELECTRON BEAM PROFILE

DESIGN OF COMPACT PULSED 4 MIRROR LASER WIRE SYSTEM FOR QUICK MEASUREMENT OF ELECTRON BEAM PROFILE 1 DESIGN OF COMPACT PULSED 4 MIRROR LASER WIRE SYSTEM FOR QUICK MEASUREMENT OF ELECTRON BEAM PROFILE PRESENTED BY- ARPIT RAWANKAR THE GRADUATE UNIVERSITY FOR ADVANCED STUDIES, HAYAMA 2 INDEX 1. Concept

More information

High Peak Power Fiber Seeds & Efficient Stabilized Pumps

High Peak Power Fiber Seeds & Efficient Stabilized Pumps High Peak Power Fiber Seeds & Efficient Stabilized Pumps Features Ultra Narrow Spectral Bandwidth (< 100kHz Instantaneous for single mode diodes) Ultra Track Linear Tracking Photodiode Temperature Stabilized

More information

gem TECHNICAL DATA SHEET CW 532nm laser Extremely low noise Power from 50mW - 750mW 532nm high spec OEM laser

gem TECHNICAL DATA SHEET CW 532nm laser Extremely low noise Power from 50mW - 750mW 532nm high spec OEM laser gem CW 532nm laser Extremely low noise Power from 50mW - 750mW TECHNICAL DATA SHEET gem The high specification CW 532nm laser Overview The gem is the jewel in the Laser Quantum collection. Its small and

More information

L25 Series Operator Manual

L25 Series Operator Manual L25 Series Operator Manual L25 899-07001-000 L25P 899-07005-000 L25D 899-07002-000 Access Laser Company 917 134 th St SW Ste A1 Everett, WA 98204 425.582.8674 www.accesslaser.com REVISION J TABLE OF CONTENTS

More information

High-Frequency Electro-Optic Phase Modulators

High-Frequency Electro-Optic Phase Modulators USER S GUIDE High-Frequency Electro-Optic Phase Modulators Models 442x, 443x, & 485x U.S. Patent # 5,414,552 3635 Peterson Way Santa Clara, CA 95054 USA phone: (408) 980-5903 fax: (408) 987-3178 e-mail:

More information

Slide Title. Bulleted Text

Slide Title. Bulleted Text Slide Title 1 Slide Outline Title Brief view of the C-AD Complex Review of the RHIC LLRF Upgrade Platform Generic Implementation of a Feedback Loop RHIC Bunch by Bunch Longitudinal Damper Cavity Controller

More information

SA210-Series Scanning Fabry Perot Interferometer

SA210-Series Scanning Fabry Perot Interferometer 435 Route 206 P.O. Box 366 PH. 973-579-7227 Newton, NJ 07860-0366 FAX 973-300-3600 www.thorlabs.com technicalsupport@thorlabs.com SA210-Series Scanning Fabry Perot Interferometer DESCRIPTION: The SA210

More information

10 Things to Consider when Acquiring a Nanopositioning System

10 Things to Consider when Acquiring a Nanopositioning System 10 Things to Consider when Acquiring a Nanopositioning System There are many factors to consider when looking for nanopositioning piezo stages. This article will help explain some items that are important

More information

Stabilizing injection-locked lasers through active feedback. Ethan Welch

Stabilizing injection-locked lasers through active feedback. Ethan Welch Stabilizing injection-locked lasers through active feedback. Ethan Welch A senior thesis submitted to the faculty of Brigham Young University in partial fulfillment of the requirements for the degree of

More information

Self-organizing laser diode cavities with photorefractive nonlinear crystals

Self-organizing laser diode cavities with photorefractive nonlinear crystals Institut d'optique http://www.iota.u-psud.fr/~roosen/ Self-organizing laser diode cavities with photorefractive nonlinear crystals Nicolas Dubreuil, Gilles Pauliat, Gérald Roosen Nicolas Huot, Laurent

More information

SPECIFICATIONS. Tunable Single-Frequency Laser Box. DL-BF11-CLSxxxB-Syyyy-zz

SPECIFICATIONS. Tunable Single-Frequency Laser Box. DL-BF11-CLSxxxB-Syyyy-zz DENSELIGHT SEMICONDUCTORS PTE. LTD. 6 Changi North St. 2, S498831 SINGAPORE Tel: (65) 64154488 Fax: (65) 64157988 www.denselight.com SPECIFICATIONS Tunable Single-Frequency Laser Box DenseLight Semiconductors

More information

Single Frequency DPSS Lasers

Single Frequency DPSS Lasers Single Frequency DPSS Lasers Any wavelength from NIR to UV using a single engineering platform based on our proprietary patented BRaMMS DPSS Laser technology. We develop and produce Single Frequency DPSS

More information

Advanced Features of InfraTec Pyroelectric Detectors

Advanced Features of InfraTec Pyroelectric Detectors 1 Basics and Application of Variable Color Products The key element of InfraTec s variable color products is a silicon micro machined tunable narrow bandpass filter, which is fully integrated inside the

More information

Features. Applications. Optional Features

Features. Applications. Optional Features Features Compact, Rugged Design TEM Beam with M 2 < 1.2 Pulse Rates from Single Shot to 15 khz IR, Green, UV, and Deep UV Wavelengths Available RS232 Computer Control Patented Harmonic Generation Technology

More information

Intra-cavity active optics in lasers

Intra-cavity active optics in lasers Intra-cavity active optics in lasers W. Lubeigt, A. Kelly, V. Savitsky, D. Burns Institute of Photonics, University of Strathclyde Wolfson Centre,106 Rottenrow Glasgow G4 0NW, UK J. Gomes, G. Brown, D.

More information

R. J. Jones College of Optical Sciences OPTI 511L Fall 2017

R. J. Jones College of Optical Sciences OPTI 511L Fall 2017 R. J. Jones College of Optical Sciences OPTI 511L Fall 2017 Active Modelocking of a Helium-Neon Laser The generation of short optical pulses is important for a wide variety of applications, from time-resolved

More information

GaSb based high power single spatial mode and distributed feedback lasers at 2.0 μm

GaSb based high power single spatial mode and distributed feedback lasers at 2.0 μm GaSb based high power single spatial mode and distributed feedback lasers at 2.0 μm Clifford Frez 1, Kale J. Franz 1, Alexander Ksendzov, 1 Jianfeng Chen 2, Leon Sterengas 2, Gregory L. Belenky 2, Siamak

More information

High brightness semiconductor lasers M.L. Osowski, W. Hu, R.M. Lammert, T. Liu, Y. Ma, S.W. Oh, C. Panja, P.T. Rudy, T. Stakelon and J.E.

High brightness semiconductor lasers M.L. Osowski, W. Hu, R.M. Lammert, T. Liu, Y. Ma, S.W. Oh, C. Panja, P.T. Rudy, T. Stakelon and J.E. QPC Lasers, Inc. 2007 SPIE Photonics West Paper: Mon Jan 22, 2007, 1:20 pm, LASE Conference 6456, Session 3 High brightness semiconductor lasers M.L. Osowski, W. Hu, R.M. Lammert, T. Liu, Y. Ma, S.W. Oh,

More information

LIGO-P R. High-Power Fundamental Mode Single-Frequency Laser

LIGO-P R. High-Power Fundamental Mode Single-Frequency Laser LIGO-P040053-00-R High-Power Fundamental Mode Single-Frequency Laser Maik Frede, Ralf Wilhelm, Dietmar Kracht, Carsten Fallnich Laser Zentrum Hannover, Hollerithallee 8, 30419 Hannover, Germany Phone:+49

More information

External cavities for controling spatial and spectral properties of SC lasers. J.P. Huignard TH-TRT

External cavities for controling spatial and spectral properties of SC lasers. J.P. Huignard TH-TRT External cavities for controling spatial and spectral properties of SC lasers. J.P. Huignard TH-TRT Bright Er - Partners. WP 3 : External cavities approaches for high brightness. - RISOE TUD Dk - Institut

More information

Conductively cooled 1-kHz single-frequency Nd:YAG laser for remote sensing

Conductively cooled 1-kHz single-frequency Nd:YAG laser for remote sensing Conductively cooled 1-kHz single-frequency Nd:YAG laser for remote sensing Juntao Wang ( ), Ren Zhu (ý ), Jun Zhou ( ), Huaguo Zang ( ÙÁ), Xiaolei Zhu (ý ), and Weibiao Chen (í Á) Shanghai Key Laboratory

More information

Novel laser power sensor improves process control

Novel laser power sensor improves process control Novel laser power sensor improves process control A dramatic technological advancement from Coherent has yielded a completely new type of fast response power detector. The high response speed is particularly

More information

High-Frequency Electro-Optic Phase Modulators

High-Frequency Electro-Optic Phase Modulators USER S GUIDE High-Frequency Electro-Optic Phase Modulators Models 442X, 443X, 444X, 446X, 48XX U.S. Patent #5,414,552 3635 Peterson Way Santa Clara, CA 95054 USA phone: (408) 980-5903 fax: (408) 987-3178

More information

OPTI 511L Fall (Part 1 of 2)

OPTI 511L Fall (Part 1 of 2) Prof. R.J. Jones OPTI 511L Fall 2016 (Part 1 of 2) Optical Sciences Experiment 1: The HeNe Laser, Gaussian beams, and optical cavities (3 weeks total) In these experiments we explore the characteristics

More information

Genesis CX STM-Series

Genesis CX STM-Series Coherent s unique Optically Pumped Semiconductor Laser (OPSL) technology powers the Genesis CX-STM Series, providing up to 250 mw of UV laser light or up to 10W of visible laser light from either OEM or

More information

3550 Aberdeen Ave SE, Kirtland AFB, NM 87117, USA ABSTRACT 1. INTRODUCTION

3550 Aberdeen Ave SE, Kirtland AFB, NM 87117, USA ABSTRACT 1. INTRODUCTION Beam Combination of Multiple Vertical External Cavity Surface Emitting Lasers via Volume Bragg Gratings Chunte A. Lu* a, William P. Roach a, Genesh Balakrishnan b, Alexander R. Albrecht b, Jerome V. Moloney

More information

Optical Phase Lock Loop (OPLL) with Tunable Frequency Offset for Distributed Optical Sensing Applications

Optical Phase Lock Loop (OPLL) with Tunable Frequency Offset for Distributed Optical Sensing Applications Optical Phase Lock Loop (OPLL) with Tunable Frequency Offset for Distributed Optical Sensing Applications Vladimir Kupershmidt, Frank Adams Redfern Integrated Optics, Inc, 3350 Scott Blvd, Bldg 62, Santa

More information

High-power semiconductor lasers for applications requiring GHz linewidth source

High-power semiconductor lasers for applications requiring GHz linewidth source High-power semiconductor lasers for applications requiring GHz linewidth source Ivan Divliansky* a, Vadim Smirnov b, George Venus a, Alex Gourevitch a, Leonid Glebov a a CREOL/The College of Optics and

More information

Construction and Characterization of a Prototype External Cavity Diode Laser

Construction and Characterization of a Prototype External Cavity Diode Laser Construction and Characterization of a Prototype External Cavity Diode Laser Joshua Wienands February 8, 2011 1 1 Introduction 1.1 Laser Cooling Cooling atoms with lasers is achieved through radiation

More information

Beam Diagnostics, Low Level RF and Feedback for Room Temperature FELs. Josef Frisch Pohang, March 14, 2011

Beam Diagnostics, Low Level RF and Feedback for Room Temperature FELs. Josef Frisch Pohang, March 14, 2011 Beam Diagnostics, Low Level RF and Feedback for Room Temperature FELs Josef Frisch Pohang, March 14, 2011 Room Temperature / Superconducting Very different pulse structures RT: single bunch or short bursts

More information

Calibration of an Automatic System Using a Laser Signature

Calibration of an Automatic System Using a Laser Signature Calibration of an Automatic System Using a aser Signature Edward F. PISKI*, Antoni IZWORSKI**, Jerzy S. WITKOWSKI* Wroclaw University of Technology *Institute of Telecommunications and Acoustics, **Institute

More information

Lecture 6 Fiber Optical Communication Lecture 6, Slide 1

Lecture 6 Fiber Optical Communication Lecture 6, Slide 1 Lecture 6 Optical transmitters Photon processes in light matter interaction Lasers Lasing conditions The rate equations CW operation Modulation response Noise Light emitting diodes (LED) Power Modulation

More information

Thermal treatment method for tuning the lasing wavelength of a DFB fiber laser using coil heaters

Thermal treatment method for tuning the lasing wavelength of a DFB fiber laser using coil heaters Thermal treatment method for tuning the lasing wavelength of a DFB fiber laser using coil heaters Ha Huy Thanh and Bui Trung Dzung National Center for Technology Progress (NACENTECH) C6-Thanh Xuan Bac-Hanoi-Vietnam

More information

FIBER EVO. Miniaturized laser module complete with controller and USB power supply all within an incredibly small package

FIBER EVO. Miniaturized laser module complete with controller and USB power supply all within an incredibly small package Miniaturized laser module complete with controller and USB power supply all within an incredibly small package KEY FEATURES: Incredibly small yet fully featured Output powers up to 75 mw Powered by USB:

More information

Progress on High Power Single Frequency Fiber Amplifiers at 1mm, 1.5mm and 2mm

Progress on High Power Single Frequency Fiber Amplifiers at 1mm, 1.5mm and 2mm Nufern, East Granby, CT, USA Progress on High Power Single Frequency Fiber Amplifiers at 1mm, 1.5mm and 2mm www.nufern.com Examples of Single Frequency Platforms at 1mm and 1.5mm and Applications 2 Back-reflection

More information

Sometimes the axis of the I-U-dependence are shown in reverse order. In this case the graph shows the stabilized current and measured voltage.

Sometimes the axis of the I-U-dependence are shown in reverse order. In this case the graph shows the stabilized current and measured voltage. 2. Electrical and other parameters 2.1. absolute maximum ratings are a listing of the environmental and electrical stresses that may be applied to a device without resulting in short term or catastrophic

More information

Feb. 1, 2013 TEC controller design experts offer tips to lower the cost and simplify the design of the devices, and to increase their ease of use.

Feb. 1, 2013 TEC controller design experts offer tips to lower the cost and simplify the design of the devices, and to increase their ease of use. Thermoelectric Cooler Controller Design Made Simpler Gang Liu, Can Li and Fang Liu, Analog Technologies, Inc. Feb. 1, 2013 TEC controller design experts offer tips to lower the cost and simplify the design

More information

High-frequency tuning of high-powered DFB MOPA system with diffraction limited power up to 1.5W

High-frequency tuning of high-powered DFB MOPA system with diffraction limited power up to 1.5W High-frequency tuning of high-powered DFB MOPA system with diffraction limited power up to 1.5W Joachim Sacher, Richard Knispel, Sandra Stry Sacher Lasertechnik GmbH, Hannah Arendt Str. 3-7, D-3537 Marburg,

More information

FLASH II. FLASH II: a second undulator line and future test bed for FEL development.

FLASH II. FLASH II: a second undulator line and future test bed for FEL development. FLASH II FLASH II: a second undulator line and future test bed for FEL development Bart.Faatz@desy.de Outline Proposal Background Parameters Layout Chalenges Timeline Cost estimate Personnel requirements

More information

Temporal coherence characteristics of a superluminescent diode system with an optical feedback mechanism

Temporal coherence characteristics of a superluminescent diode system with an optical feedback mechanism VI Temporal coherence characteristics of a superluminescent diode system with an optical feedback mechanism Fang-Wen Sheu and Pei-Ling Luo Department of Applied Physics, National Chiayi University, Chiayi

More information

Recent advances in high-performance 2.X µm Vertical External Cavity Surface Emitting Laser (VECSEL)

Recent advances in high-performance 2.X µm Vertical External Cavity Surface Emitting Laser (VECSEL) Recent advances in high-performance 2.X µm Vertical External Cavity Surface Emitting Laser (VECSEL) Joachim Wagner*, M. Rattunde, S. Kaspar, C. Manz, A. Bächle Fraunhofer-Institut für Angewandte Festkörperphysik

More information

DPSS 266nm Deep UV Laser Module

DPSS 266nm Deep UV Laser Module DPSS 266nm Deep UV Laser Module Specifications: SDL-266-XXXT (nm) 266nm Ave Output Power 1-5mW 10~200mW Peak power (W) ~10 ~450 Average power (mw) Average power (mw) = Single pulse energy (μj) * Rep. rate

More information

arxiv: v1 [physics.ins-det] 16 Oct 2017

arxiv: v1 [physics.ins-det] 16 Oct 2017 arxiv:1710.05742v1 [physics.ins-det] 16 Oct 2017 Antireflection Coated Semiconductor Laser Amplifier Vasiliki Bolpasi 1, a) 1, b) and Wolf von Klitzing IESL - FORTH (Dated: 17 October 2017) This paper

More information