The High-finesse Fabry-Perot Cavity

Slides:



Advertisements
Similar presentations
Cavity Locking by Piezo-Driven Mirror Botao Jia Duke University Advisor: Dr. Nanda Sirish HAPPEX Collaboration Meeting Dec 1, 2006.
Advertisements

PPLN Frequency- Doubling Project Diana Parno Hall A Parity Collaboration Meeting May 17, 2007.
Green cavity progress Botao Jia May Advisors: Dr. Nanda Sirish, Dr. Wu Ying HAPPEX Collab. Mtg. May 17-18, 2007.
Thomas Jefferson National Accelerator Facility S. Nanda, July 28, Hall A Compton Polarimeter Upgrade Sirish Nanda Jefferson Laboratory PRex Collboration.
CAVITY LOCK ELECTRONICS Dan Sexton, Sirish Nanda, and Abdurahim Rakhman.
Hall A Collaboration meeting January 5 th 2007 A. Camsonne Compton Polarimeter Status Report Alexandre Camsonne Hall A Collaboration Meeting January 4.
Hall A Collaboration Meeting S. Nanda, June 23, 2005 Hall A Compton Polarimeter For Hall A Collaboration Meeting June 23 rd 2005 Sirish Nanda Thomas Jefferson.
Thomas Jefferson National Accelerator Facility S. Nanda, December 5, Hall A Compton Polarimeter Sirish Nanda Jefferson Laboratory Hall A Collboration.
Thomas Jefferson National Accelerator Facility S. Nanda, June 22, The Hall A Compton Polarimeter Sirish Nanda Jefferson Laboratory Hall A Collaboration.
Wavelength532 nm Power1500 Watts Gain15,000 Q-factor1.8 x Length0.85 m ModeCW, TEM 00 Free Spectral Range176 MHz Cavity Band Width3.12 kHz Mirror.
J.T. Hodges, D.A. Long, G.W. Truong, K.O. Douglass,
FINESSE FINESSE Frequency Domain Interferometer Simulation Versatile simulation software for user-defined interferometer topologies. Fast, easy to use.
Dual Recycling for GEO 600 Andreas Freise, Hartmut Grote Institut für Atom- und Molekülphysik Universität Hannover Max-Planck-Institut für Gravitationsphysik.
III. Feedback control The laser dynamics can be modelled by a system of linked rate equations introduced by Roy et al. (1993) Based on the model it was.
T1 task- update Mike Plissi. 2 Collaboration Groups actively involved INFN-VIRGO MAT IGR-Glasgow Groups that have expressed interest INFN-AURIGA CNRS-LKB.
Compton Laser and Systematics for PREx Abdurahim Rakhman Syracuse University PREx Collaboration Meeting, JLab January 30, 2011.
Laser Physics EAL 501 Lecture 6 Power & Frequency.
Marcus Ng Mentor: Alan Weinstein Co-mentor: Robert Ward
A_RD_01 Applications of a high finesse Fabry Perot Cavity for the ILC ► Introduction ► Status of the cavity R&D – at ATF – at LAL/Orsay French Labs. :
COMPUTER MODELING OF LASER SYSTEMS
Status of g ray generation at KEK-ATF ► Introduction ► Status of the cavity R&D ► Out Look French Labs. : LAL (Orsay) in Collaboration with CELIA (Laser.
SLAC XFEL Short Bunch Measurement and Timing Workshop 1 Current status of the FERMI project (slides provided by Rene Bakker) Photoinjector laser system.
Overview of enhancement cavity work at LAL/Orsay  INTRO:  Optical cavity developments at LAL  Results on optical cavity in picosecond regime  Polarised.
GWADW, May 2012, Hawaii D. Friedrich ICRR, The University of Tokyo K. Agatsuma, S. Sakata, T. Mori, S. Kawamura QRPN Experiment with Suspended 20mg Mirrors.
October 16-18, 2012Working Group on Space-based Lidar Winds 1 AEOLUS STATUS Part 1: Design Overview.
Introduction to Optical Electronics
Status of R&D of Optical Cvities at KEK-ATF ►Introduction ►Status of the cavity R&D ►Out Look KEK, Hiroshima University LAL (Orsay) in Collaboration withCELIA.
Thomas Jefferson National Accelerator Facility S. Nanda, July 22, The Hall A Compton Polarimeter Upgrade Sirish Nanda Jefferson Laboratory Parity.
GEO‘s experience with Signal Recycling Harald Lück Perugia,
Feedback R&D for Optical Cavity Ryuta TANAKA (Hiroshima univ.) 19 th Feb 2013 SAPPHiRE DAY.
Mikael Siltanen,1 Markus Metsälä,1
LPOL-cavity Introduction Tests at Orsay Optics (laser polarisation) Calorimeter DAQ Mechanics & installation at DESY  Norbert’s talk.
Nonplanar Cavity Construction and Locking Technique for High Finesse Cavity Soskov V., Chiche R., Cizeron R., Jehanno D., Zomer F. Laboratoire de l’Accélérateur.
PMD Measurement Methods  Fixed Analyzer Method IEC / ITU-T G.650.2/ EIA/TIA Standard FOTP-113  Jones Eigenanalysis Matrix Method IEC /
European Gravitational Observatory12/12/2005 WG1 Hannover 1 Mode Matching of the Fabry-Perrot cavities Julien Marque.
Status and Plan of Compton  -ray Generation at KEK-ATF Japanese Labs. : KEK, ATF group, Hiroshima University Tsunehiko OMORI (KEK) for 13 February 2014.
Lecture 6. Polarization splitter based Filters Acoustooptic Tunable Filters.
Compton polarimetry for EIC Jefferson Lab Compton Polarimeters.
Compton Experiment at ATF Tohru Takahashi Hiroshima University for Collaborators (particularly Omori san for slides)
Haifeng Huang and Kevin K. Lehmann
S. ChelkowskiSlide 1WG1 Meeting, Birmingham 07/2008.
Abstract The Hannover Thermal Noise Experiment V. Leonhardt, L. Ribichini, H. Lück and K. Danzmann Max-Planck- Institut für Gravitationsphysik We measure.
PULSE LASER WIRE Laser pulse storage in an optical cavity as a beam monitor & an X-ray source Kaori Takezawa Kyoto Univ. 2nd Mini-Workshop on Nano Project.
T.Takahashi Hiroshima Optical Cavity R&D around KEK-ATF T.Takahashi Hiroshima Univ. Nov LCWS08 at Chicago.
Dual Recycling in GEO 600 H. Grote, A. Freise, M. Malec for the GEO600 team Institut für Atom- und Molekülphysik University of Hannover Max-Planck-Institut.
Compton Experiment at ATF Compton Meeting at LAL Orsey 2-Dec-2008 Tsunehiko OMORI (KEK) with many thanks to Compton collaborators.
The Hall A Compton Polarimeter Upgrade
Nonlinear generation of radiation by periodically poled LiTaO 3 crystals Single pass UV generation Intracavity Second Harmonic Generation HWP: half wave.
Compton polarimetry for EIC. Outline Polarized electron beam Compton process Compton polarimeters at Jefferson Laboratory – Parity experiments at Jlab.
Workshop for advanced THz and Compton X-ray generation
Laser-Undulator Compact X-ray source (LUCX) POSIPOL2006 Workshop at CERN 1/23 Experimental Plan of X-ray Generation using Optical Resonator using Optical.
FINESSE FINESSE Frequency Domain Interferometer Simulation Andreas Freise European Gravitational Observatory 17. March 2004.
0 Frequency Gain 1/R 1 R 2 R 3 0 Frequency Intensity Longitudinal modes of the cavity c/L G 0 ( ) Case of homogeneous broadening R2R2 R3R3 R1R1 G 0 ( )
Compton Gamma-ray Generation Experiment by Using an Optical Cavity in ATF POSIPOL 2007 Workshop at LAL Hirotaka Shimizu Hiroshima University.
Update of R&D Optical Cvities at KEK-ATF ►Introduction ►Status of the cavity R&D ►Recent activities ►Out Look KEK, Hiroshima University LAL (Orsay) in.
Date of download: 9/17/2016 Copyright © 2016 SPIE. All rights reserved. A schematic of a tunable external cavity diode laser in a Littman-Metcalf configuration.
Interferometer configurations for Gravitational Wave Detectors
Quantum noise reduction using squeezed states in LIGO
Recent developments of optical cavity systems for advanced photon sources based on Compton backscattering A. Martens, F. Zomer, P. Favier, K. Cassou,
Status report of Polarization RSE
Optical frequency divider with division uncertainty at the 10−21 level
Chapter III Optical Resonators
Light Sources for Optical Communications
Development of Optical Resonant Cavities for laser-Compton Scattering
Variable reflectivity signal-recycling mirror and control
Optical Fiber Communications
PHYS 408 Applied Optics (Lecture 18)
Fabry-Perot Resonator
High finesse cavity for Polarised Positron Source on ILC.
Presentation transcript:

The High-finesse Fabry-Perot Cavity Abdurahim Rakhman Advisors: Prof. Paul Souder, Dr. Sirish Nanda PREx Collaboration Meeting 12/07/2007

Outline Compton Upgrade at Jefferson Lab Principles of the Fabry-Perot Cavity Cavity Parameters & Prometheus Laser Mode Matching Cavity Locking Conclusions and Future Plans

Compton Polarimeter: e-  e-  Z

Compton Upgrade: Gain: 7000 15000 λ=1064nm λ=532nm 0.85 8GeV 4GeV 1GeV

Fabry-Perot Cavity: L r1 r2 Circulation Incident Transmission Reflected r1 r2 Previously locking was successful with a G~2,000 Current Cavity Mirror: Los Gatos Research, Inc. (LGR) Type: Plano-Concave Radius of Curvature: 1 m Reflectivity: 99.987±0.001% G=6,000 F=18,000

Prometheus Laser: 2 W 0.1W Innolight GmbH, Germany ▪809 nm Pump Diodes ▪1064 nm Nd:YAG ▪532 nm SHG via PPKTP 2 W 0.1W

Prometheus Laser Profile: Beam is highly elliptic, circularization is needed Before After

Mode-Matching: laser mode (beam) should match the cavity resonator mode beam waist at the center should match the natural waist of the cavity L3 L2 cavity waist L1 0.5787 TEM00 mode incident reflected mode matched

OptoCad: FORTRAN90 program for tracing Gaussian beams computes the parameters of the optical system Green cavity optical layout by OptoCad

Complete ray tracing by OptoCad (in development):

Pound-Drever-Hall (PDH) Locking Scheme: Detect phase of the resonance from reflected light Feedback to tunable element to stay “locked” to resonance Photo detector Beam Splitter Cavity Oscillator Phase Shifter Mixer Low Pass Filter Tunable Laser PID-Regulator Error signal

Digital CavLock Electronics (Homemade): 4” previous current

Search / scan / lock logic: Transmission Reflection Fast Scan Slow Search Successful locking with low gain cavity Reflection Error Signal Transmission Signals of LGR cavity

Cavity Locking: Feedback loop tuning in progress Reflection Transmission 2 sec level lock, only with fast PZT feedback, but unacceptable due to large fluctuations Reflection Error Signal Transmission reworked electronics, 40 msec level short lock with fast PZT feedback only Feedback loop tuning in progress

Thank you ! Conclusions: Prometheus Laser has been reprofiled Mode matching of LGR mirror has been accomplished Complete ray tracing of the system by OptoCad is in development Cavity feedback loop tuning in progress Short duration lock has been achieved Thank you !

Cavity Parameters: Free Spectral Range : Gain: Finesse: Band Width: