Precision Tilt and Radius of Curvature Sensor Using Double-Pass AOM 2013. 6. 10. Kyuman Cho Department of Physics Sogang University.

Slides:



Advertisements
Similar presentations
Géraldine Guerri Post-doc CSL
Advertisements

1 Extreme Ultraviolet Polarimetry Utilizing Laser-Generated High- Order Harmonics N. Brimhall, M. Turner, N. Herrick, D. Allred, R. S. Turley, M. Ware,
Current Status of Collaboration Research Kyuman Cho and Shinji Miyoki Sogang University, Institute for Cosmic Ray Research and LCGT Collaboration 3 rd.
Measurements using Atom Free Fall
3. Image motion due to optical element motion
Development of a mover having one nanometer precision and 4mm moving range Y. Morita, S. Yamashita ICEPP, University of Tokyo Y. Higashi, M. Masuzawa,
X-Ray Survey of The ATLAS SCT. The ATLAS Semi-Conductor Tracker.
The Linear Collider Alignment and Survey (LiCAS) Project Richard Bingham*, Edward Botcherby*, Paul Coe*, Grzegorz Grzelak*, Ankush Mitra*, Johannes Prenting.
Initial Calibration and Stability Results from the LiCAS RTRS FSI System John Dale for the LiCAS Collaboration IWAA February 2008.
G D Calibration of the LIGO Interferometer Using the Recoil of Photons Justice Bruursema Mentor: Daniel Sigg.
Higher order laser modes in gravitational wave detectors
1 Sébastien Boutet 1 Coherent X-ray Imaging Instrument FAC Meeting, June Coherent X-ray Imaging Instrument Sébastien Boutet.
Integration and Alignment of Optical Subsystem Roy W. Esplin Dave McLain.
Proposal for Being a KAGRA Member July 30, 2012 Kyuman Cho Department of Physics, Sogang Universit y.
The wave nature of light Interference Diffraction Polarization
SAM PDR1 SAM LGS Mechanical Design A. Montane, A. Tokovinin, H. Ochoa SAM LGS Preliminary Design Review September 2007, La Serena.
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.
Effective lens aperture Deff
Status of the advanced LIGO laser O. Puncken, L. Winkelmann, C. Veltkamp, B. Schulz, S. Wagner, P. Weßels, M. Frede, D. Kracht.
Particle Image Velocimetry (PIV) Introduction
19 February 2009 Cophasing sensor for synthetic aperture optics applications First steps of the development of a cophasing sensor for synthetic aperture.
Einstein gravitational wave Telescope Next steps: from technology reviews to detector design Andreas Freise for the ET WG3 working group , 2nd.
Test mass dynamics with optical springs proposed experiments at Gingin Chunnong Zhao (University of Western Australia) Thanks to ACIGA members Stefan Danilishin.
PACS IIDR 01/02 Mar 2001 FPFPU Alignment1 D. Kampf KAYSER-THREDE.
Experimental Characterization of Frequency Dependent Squeezed Light R. Schnabel, S. Chelkowski, H. Vahlbruch, B. Hage, A. Franzen, N. Lastzka, and K. Danzmann.
Feedback R&D for Optical Cavity Ryuta TANAKA (Hiroshima univ.) 19 th Feb 2013 SAPPHiRE DAY.
IP-BSM Improvement Work N. Terunuma 2012/6/26 ATF2 Project Meeting.
High Throughput Microscopy
Optical Gyroscopes for Ground Tilt Sensing in Advanced LIGO The need for low frequency tilt sensing The optics in Advanced LIGO’s suspensions must be very.
S. ChelkowskiSlide 1ET Meeting, Hannover 01/2009.
LIGO-G D LIGO II1 AUX OPTICS SUPPORT Michael Smith, 6/11/03 STRAY LIGHT CONTROL ACTIVE OPTICS COMPENSATION OUTPUT MODE CLEANER PO MIRROR AND PO.
1/10 Tatsuya KUME Mechanical Engineering Center, High Energy Accelerator Research Organization (KEK) ATF2-IN2P3-KEK kick-off meeting (Oct. 10, 2006) Phase.
MICROSCOPE DESIGN. beam expander and objective Why do we need a beam expander? What facts about the laser do we need to know? How much expansion do we.
Oct 17, 2001SALT PFIS Preliminary Design Review1 Southern African Large Telescope Prime Focus Imaging Spectrograph Mechanical Mechanism Design Michael.
I.Introduction II. System Design B.E. Unks, N. A. Proite, D. D. Yavuz University of Wisconsin – Madison The above figure shows a block diagram of the apparatus.
The stabilisation of the final focus (StaFF) system Sun 12 th March 2006 MDI – LCWS06 at I I Sc Bangalore David Urner, Paul Coe, Armin Reichold.
Christoph Gabor, ASTeC HIPPI—Meeting (WP 5) 26 th – 28 th September 2007 Non—destructive transverse emittance measurement device The Front End Test Stand.
LASER FRAME: Straightness monitor (Tentative results of resolution test) Third Mini-Workshop on Nano Project at ATF May 30-31,2005 KEK Nano BPM Group Y.Higashi,
New emittance monitor beamline
Current Status of LASER FRAME for KEK-Nano BPM (Tentative results of resolution test) Second Mini-Workshop on Nano Project at ATF December 11-12, 2004.
IPBSM Operation 11th ATF2 Project Meeting Jan. 14, 2011 SLAC National Accelerator Laboratory Menlo Park, California Y. Yamaguchi, M.Oroku, Jacqueline Yan.
Taikan SUEHARA, ATF2 meeting, KEK, 2006/11/22 Status of fringe stabilization of Shintake-monitor Taikan SUEHARA The University of Tokyo.
Planar Chiral Metamaterials & their application to optoelectronics devices W. Zhang, A. Papakostas, A. Potts, D. M. Bagnall, N. I. Zheludev Microelectronic.
Taikan SUEHARA et al., LCWS2007 & DESY, 2007/06/01 R&D Status of ATF2 IP Beam Size Monitor (Shintake Monitor) Taikan SUEHARA, H.Yoda, M.Oroku,
Advanced LIGO UK 1 LIGO-G K OSEM Development UK Advanced LIGO project Stuart Aston University of Birmingham for the UK Advanced LIGO Team LSC.
SL/BI 16/05/1999DIPAC’99 -- JJ Gras -- CERN SL/BI -- Adaptive Optics for the LEP 2 SR Monitors G. Burtin, R.J. Colchester, G. Ferioli, J.J. Gras, R. Jung,
1 In situ wavefront distortion measurements Efim Khazanov, Anatoly Poteomkin, Anatoly Mal’shakov, Nikolay Andreev, Alexander Sergeev Institute of Applied.
Space Gravitational Wave Antenna DECIGO Project 3rd TAMA Symposium February 7, Institute for Cosmic Ray Research, Japan Seiji Kawamura National.
25/05/2007POSIPOL FOUR MIRRORS Fabry Perot resonator at LAL-Orsay Y. Fedala With help of F. Zomer, R.Cizeron.
ME-250 Precision Machine Design Semiconductor Lithography Tool Alok Bhatt Sarang Deshpande Instructor: Dr. B. J. Furman Mechanical and Aerospace Engineering.
Date of download: 6/3/2016 Copyright © 2016 SPIE. All rights reserved. Schematic layout of the interferometer setup. (a) T: test beam; R: reference beam;
Design for a New Optical Table of the Shintake Monitor Takashi Yamanaka The University of Tokyo ATF2 weekly meeting 2007/9/26.
Progress of Shintake Monitor (ATF2 IP-BSM) ATF2 weekly meeting 2008/9/3 Takashi Yamanaka The University of Tokyo.
Optical Instruments II Instruments for Imaging the Retina.
Date of download: 7/2/2016 Copyright © 2016 SPIE. All rights reserved. The schematic of experimental setup used for generation of collimated hollow beam.
Thermal compensation issues: sensing and actuation V. Fafone University of Rome Tor Vergata and INFN ASPERA Technological Forum – EGO October, 2011.
Non-Contact Inspection of Internal Threads of Machined Parts
Local control sensors for iKAGRA payloads and perspective (Optical lever) Kazuhiro Agatsuma 2013/Dec./5 ELiTES meeting at Tokyo1.
Date of download: 7/8/2016 Copyright © 2016 SPIE. All rights reserved. Through-the-objective TIRF creates the evanescent field on the aqueous side of the.
Pasquale Arpaia, University of Naples Federico II
Recap- Optical extensometer
Interferometer configurations for Gravitational Wave Detectors
From: Microtube Laser Forming for Precision Component Alignment
Lithium Niobate Waveguide Phase Modulator for Roll Angular
Manuel Marchiò, Raffaele Flaminio, Shunshi Kuroki
Interferometric measurements on mirrors
الفصل 1: الحركة الدورانية Rotational Motion
Paper Synopsis: Lens Centering using the Point Source Microscope Robert E. Parks by Wenrui Cai Opti521.
Volume 74, Issue 2, Pages (February 1998)
MAMBO PRE-LAUNCH CALIBRATION CONSIDERATIONS
Presentation transcript:

Precision Tilt and Radius of Curvature Sensor Using Double-Pass AOM Kyuman Cho Department of Physics Sogang University

Overview I.Introduction II.Tilt Sensor Using AOM III.Experimental Results IV.Local Slope Profiler V.Summery

Introduction

Introduction: Previous Works

11 bounces Optical lever inside a Sagnac Interferometer (J.M. Hogan et al., Opt. Lett., 36, 1698 ) Introduction: Previous Works

Double-Pass AOM Intterferometer Youngkyu Park, Kyuman Cho, OPTICS LETTERS / Vol. 36, No. 3 / February 1, 2011

ff Incident Beam PBS QWP Lens AOM M M Tilt Sensor Arrangement

Beam Separation at focal plane: d = 0.945mm CCD Beam profiler image 0.945mm Experimental Results

Experimental Results: Directional Tilt pivot line1 pivot line2 Pivot line1 Pivot line2 Pivot line1 = 45Hz Pivot line2 = 85Hz ~ 33dB Driven angle variance ~0.27 rad ~ 85dB

Motorized Rotation stage Experimental Results: Linearity

Applied Tilt Experimental Results

Opt. Lett., 36, 1479 Work of M. D. Turner et al.

Work of J. M. Hogan et al. Opt. Lett., 36, 1968

DC stability is measured by using a fixed mirror Stability Fixed Mirror To Detector Laser Excellent DC Stability! AOM Experimental Results

Measurement of lateral motion rejection using a displace mirror Measurement result Displaced Mirror To Detector Laser AOM 8mm rad (~58nm) Experimental Results

Scanning Local Slope Profiler

R x  Point by point scanning scheme for mapping local slope of the mirror

Summary A double-pass AOM interferometer scheme has been used for precision tilt measurements Can provide very high sensitivity, Highly immune to environmental perturbations Application of our new scheme has been discussed Initial tilt alignment of mirrors for KAGRA, Local slope profiler for mirrors Potentially, a tilt sensor for TOBA