LIGO ADVANCED SYSTEMS TEST INTERFEROMETER (LASTI)

Size: px
Start display at page:

Download "LIGO ADVANCED SYSTEMS TEST INTERFEROMETER (LASTI)"

Transcription

1 LIGO ADVANCED SYSTEMS TEST INTERFEROMETER (LASTI) Program Update: LSC Meeting, Hannover Dave Ottaway August 2003 LSC Meeting August 03 1

2 Talk Overview 1. LASTI goals and timelines 2. Overview of progress to date 3. Previously proposed solution, new problems 4. Proposed solutions 5. Conclusions LSC Meeting August 03 2

3 LASTI Mission Test LIGO components & systems at full mechanical scale Practice installation & commissioning Minimize delays & downtime for advanced LIGO upgrades Qualify design mods & retrofits for initial LIGO Specific Advanced LIGO Program Tasks ( ): Qualify advanced isolation & suspension systems and associated controls at full scale Develop detailed SEI/SUS installation & commissioning handbook Look for unforeseen interactions & excess displacement noise Test PSL and Input Mode Cleaner together at full power LSC Meeting August 03 3

4 LASTI People Resident MIT Staff Students - Jamie Rollins, Stefan Ballmer, Dan Mason, Waseem Bakr Engineering -Myron MacInnis, Ken Mason, Jonathan Allen, Bill Rankin Scientists - Gregg Harry, Rich Mittleman, Dave Ottaway, David Shoemaker, Pradeep Sarin, Mike Zucker (Advice) Computers Keith Bayer Laboratory and LSC Visitors (to date) Initial SEI & SUS- Corey Gray, Hugh Radkins, Gary Traylor, Harry Overmier, Betsy Bland, Jonathan Kern, Marcel Hammond, Dennis Coyne Advanced SEI - Joe Giaime, Brian Lantz, Wensheng Hua, Corwin Hardham Advanced SUS - Norna Robertson, Calum Torrie, Janeen Romie, Phil Willems, Justin Greenhalgh, Ken Strain, Caroline Cantley, Mark Barton CDS/DAQ - Jay Heefner, Rus Wooley, Paul Russel LSC Meeting August 03 4

5 LASTI Advanced LIGO R&D Program Commission infrastructure (vacuum, cleanrooms, cranes ) Commission PSL & controls Commission initial seismic stack, suspensions & 1m test cavity in HAM chamber Develop & test EPI for LLO seismic remediation Qualification test of early pre-prototype triple pendulum (Delayed) Integrate/test active HAM SEI pathfinder (Delayed) Integrate/test active BSC SEI pathfinder (Delayed) Integrate/test Quad and Triple suspensions Integrate/test sapphire & fused silica core optics Qualify for low displacement noise with sensitive interferometer system Integrate and test full scale adaptive thermal compensation Integrate/test AdLIGO 180 Watt PSL & Mode Cleaner LSC Meeting August 03 5

6 High Bay Schematic X-end HAM BSC Y-mid HAM PSL Y-end HAM Currently planned to use the Y-arm More space around the X-arm BSC orientated such that layout mimics: ETM Chamber X arm, ITM Chamber Y arm Y mid with seismic isolation installed is not compatible for additional experiments if Y-end HAM is used for LASTI LSC Meeting August 03 6

7 LASTI Infrastructure and PSL LASTI PSL Mid Y HAM with MEPI BSC chamber including cartridge clean room LSC Meeting August 03 7

8 Pre-stabilized Laser (PSL) J. Rollins aligning PMC cavity D. Ottaway and J. Rollins commissioning controls LSC Meeting August 03 8

9 Intensity Stabilization Experiment Our approach: => Very low noise AC-coupled PD => Low voltage low noise parts in the signal path => Beam geometry stabilized by PMC LSC Meeting August 03 9

10 High Bandwidth FSS Servo Design Alternative high bandwidth frequency topology tried Achieved an upper unity gain frequency of 1 MHz Based on design by J. Hall LSC Meeting August 03 10

11 External Pre-Isolators (EPI) Magnitude Ground to Optical Table (Jun15) Ground to Optical Table (Jul23) Ground to Optical Table (loops off) K. Mason, MIT 10-4 Frequency (Hz) Coherence Ground to Optical Table (Jun15) Ground to Optical Table (Jul23) Ground to Optical Table (loops off) LSC Meeting August 03 11

12 External Pre-Isolators (EPI) J. Giaime, LLO/LSU Active vibration suppression interposed between ground and existing internal seismic isolation Main gravitational load is supported by angled coil springs (2 per leg) 2 forcers per leg, one vertical and one tangential Payload-mounted L-4C geophone + DC position sensor for local feedback STS-2 seismometer on floor permits feedforward at low frequencies (µseism) LSC Meeting August 03 12

13 Initially proposed Interferometric Noise Test Configuration 16 m ITM ETM RM RM MC3 MC2 MCx, MMTx, SM: Adv LIGO SOS ETM, ITM: Adv LIGO LOS MC1 PSL LSC Meeting August 03 13

14 LASTI Interferometer Sensitivity Model For sapphire TM s (baseline plan) Q TM = 2e8, Φ coating = 4e-4 6W laser power (LIGO I laser) Cavity finesse m cavity length 3mm beam radius (max. practical) Limited by thermoelastic noise over most of band due to small beam G. Harry, 6/25/02 LSC Meeting August 03 14

15 (Silica Test Mass Option) For silica TM s (backup plan) Q TM = 3e7, Φ coating = 4e-4 6W laser power (LIGO I laser) Cavity finesse m cavity length 2.25mm beam radius Limited by internal Brownian noise over most of band due to lower Q G. Harry, 6/25/02 LSC Meeting August 03 15

16 Summary of Initial Solution Two cavities proposed to provide common mode rejection of mode cleaner frequency noise and technical radiation pressure noise Problem : Proposed payload exceeds seismic limits Seismic mass limit = 800 kg Current payload mass ~ 1000 kg ITM Suspension mass = kg ETM Suspension mass = kg MC Suspension mass = 81.3 kg +spacer Possible solutions : Modify seismic for LASTI or modify/remove one of the reference cavities or anchor mirror catchers elsewhere LSC Meeting August 03 16

17 Active Seismic Isolation Internal active isolator External active isolator Existing LIGO I structure & vacuum chamber Quad-pendulum suspension (GEO/LIGO) LSC Meeting August 03 17

18 Advanced LIGO Suspensions Based on successful GEO600 triple pendulum design Quad pendula for TM, BS; Triples for input optics Blade springs for vertical isolation Indirect damping through upper stage recoil Electrostatic or photon drive for fast control at final stage; reaction mass for ES recoil R. Jones, LSC Glasgow Meeting U. August 03 18

19 More details of possible solutions Designing higher payload LASTI Seismic => Specifically testing Seismic then re-engineering to hold larger suspension weight Cons -Expensive, time consuming -Almost certainly better ways Anchoring catcher to vacuum chamber Cons -Not likely to be used in AdvLIGO, and hence not testing what is in Advanced LIGO Pros -Saves a lot of weight -No modifications necessary to LASTI Seismic LSC Meeting August 03 19

20 More details of possible solutions Using a single test cavity Mass closest to designed AdvLIGO seismic load Simplest design Potentially good performance if OSEM noise in MC can be overcome Also possible if global control can be used to damp the MC Alternatively turn damping off for short periods Using a second lighter cavity test cavity Possible solution if OSEM noise in MC cavity cannot be fixed Disable local damping rely on global control for damping Control problems and noise analysis to still needs to be done! LSC Meeting August 03 20

21 Parameter File for Calculations Test Cavity Parameters Length =16m Finesse = 2026 Modulation frequency = 9.8 MHz Mode Cleaner Parameters Length = 16 m Finesse = 2026 PD quantum efficiency = 0.9 Modulation frequency = 25 MHz Laser Power = 0.3 W (Low Power) Laser power = 0.3 W (Low Power) = 1.5 W (High Power) Spot size = 3mm (Conservative) = 1.5 W (High Power) = 16 mm (Aggressive) MC1,MC3 ROC = Flat Coating phi =5.0e-5 MC2 ROC = 26.9 m Input mirror substrate: Fused Silica Substrate phi = 1.0e-7 Spotsize = 2.7 mm Substrate mass =15 kg Coating phi = 5.0e-5 Input mirror ROC = Flat (Aggressive) Substrate phi = 0.3e-7 = 40 m (Conservative) End mirror substrate: Sapphire Substrate mass =3 kg Substrate phi = 1.0e-8 General Parameters Substrate mass = 40 kg Intensity noise =Advanced LIGO Requirements Output mirror ROC = 40 km Beam Jitter = LIGO 1 Measured PSL filtered by MC LSC Meeting August 03 21

22 Predicted MC Operation Frequency Noise (Hz/Hz 1/2 ) Advanced LIGO requirement Radiation pressure noise Shot noise VCO noise Best suspension Beam Jitter Noise Thermal noise Total noise (0.3 W att input) Total Noise (10 Watt input) Initial LIGO MC Beam jitter only known 100 Hz Calculated using AdvLIGO Parameters High power curve ignores VCO, beam jitter noise Relies on alternative OSEM strategy Frequency (Hz) LSC Meeting August 03 22

23 Predicted Single Arm LASTI Performance (Low Power) Length Noise (Hz/Hz 1/2 ) Frequency (Hz) Thermal Noise Thermoelastic Noise Radiation Pressure Noise Shot Noise MC Requirement Advanced LIGO MC Total Noise Aggressive Thermal Aggressive Thermoelastic Aggressive Beam Jitter Noise Power incident on mode cleaner =0.3 W Conservative LASTI not limited by MC noise Requires significant improvement over OSEM damping Should be possible with eddy current damping LSC Meeting August 03 23

24 Predicted Single Arm LASTI Performance (Higher Power) Frequency Noise (Hz/Hz 1/2 ) Thermal Noise Thermoelastic Noise Radiation Pressure Noise Shot Noise MC Requirement Advanced LIGO MC Total Noise Aggressive Thermal Aggressive Thermoelastic Power incident on mode cleaner =1.5 W Can reach AdvLIGO sensitivity at 1kHz if technical intensity noise is improved from 2e-6 to 5e-7 at 1kHz Frequency (Hz) LSC Meeting August 03 24

25 Comments on Aggressive LASTI Beam Jitter Noise Susceptability Parameters used:» Cavity length = 16 m» Input mirror roc =flat, Output mirror roc =40 km» Spot size = 16 mm» Alignment sensitivity 3e-7 radians for 1% power loss» Beam jitter not likely to be a problem based on static mis-alignment of 3e-7 radians and dynamic beam jitter limited by current PSL. Agressive LASTI Conservative LASTI πc( ε sε + βsβ ) ν ( f ) = 2( ε sβ + βsε ) f LF 2sin( α) 1 cos( α) 2sin( α + θm) 1 cos( α + θ ) m 2sin( α θ m) 1 cos( α θ ) m Ref E. Calloni et al. Optics Communications 142 (1997) Modulation Frequency/FSR LSC Meeting August 03 25

26 Updated milestones: LLO seismic remediation interleaved with Advanced LIGO development 4Q99 (4Q99 act): LASTI vacuum envelope commissioned 1Q00sch (3Q01 act): LASTI SEI external structures installed 2Q00sch (4Q00 act): LASTI infrastructure design review 3Q01sch (1Q02 act): LASTI infrastructure complete (DAQ, SEI, PSL, test cavity) NEW 4Q01: Fit LIGO I BSC stack (from spare parts) to support EPI qualification NEW 1Q02: External pre-isolator tests for LLO seismic retrofit underway NEW 4Q02: PSL intensity stabilization experiment underway NEW 4Q02: MC triple suspension prototype installed for controls pre-test 4Q02: HAM SEI pathfinder installed for standalone testing (slips to 3Q04) 3Q02: BSC SEI pathfinder installed for standalone testing (slips to 3Q04) 2Q04: LASTI noise test begins; SUS prototypes installed (slips to 2Q05) NEW: 2Q05: Thermal compensation integration and test 4Q05: Interferometric displacement tests 1Q06: LASTI SUS/SEI test review 2Q06: Adv LIGO PSL/MC tests start (180 Watts) LSC Meeting August 03 26

27 Short term plans (ie 6months) Finalize the design of the LASTI experiment for Advanced LIGO EPI» Test HEPI on a HAM» Finish conversion of controls from Dspace to VME Install a controls prototype in the Xend HAM LSC Meeting August 03 27

28 Conclusions LASTI s mission to pre-qualify Advanced LIGO technology has an unexpected dress rehearsal in the LLO seismic retrofit with the successful trial of HEPI/MEPI Need to find more information about MC suspensions before final decision can be made on the Advanced LIGO experimental program If mode cleaner suspension noise is significantly better than the radiation pressure limited Advanced LIGO specification can probably only require a single test cavity It may be technically feasible to significantly increase the spot size in the test cavity and measure noise at the Advanced LIGO displacement sensitivity (Not 10 X below) at 10 Hz and 1kHz LSC Meeting August 03 28

Active Isolation and Alignment in 6 DOF for LIGO 2

Active Isolation and Alignment in 6 DOF for LIGO 2 Active Isolation and Alignment in 6 DOF for LIGO 2 JILA, LSU, MIT, Stanford LIGO Science Collaboration Rana Adhikari, Graham Allen, Daniel Debra, Joe Giaime, Giles Hammond, Corwin Hardham, Jonathan How,

More information

Advanced LIGO Status Report

Advanced LIGO Status Report Advanced LIGO Status Report Gregory Harry LIGO/MIT On behalf of the LIGO Science Collaboration 22 September 2005 ESF PESC Exploratory Workshop Perugia Italy LIGO-G050477 G050477-00-R Advanced LIGO Overview

More information

Status of LIGO. David Shoemaker LISA Symposium 13 July 2004 LIGO-G M

Status of LIGO. David Shoemaker LISA Symposium 13 July 2004 LIGO-G M Status of LIGO David Shoemaker LISA Symposium 13 July 2004 Ground-based interferometric gravitational-wave detectors Search for GWs above lower frequency limit imposed by gravity gradients» Might go as

More information

Hydraulic Actuators for the LIGO Seismic Retrofit

Hydraulic Actuators for the LIGO Seismic Retrofit Hydraulic Actuators for the LIGO Seismic Retrofit Stanford, Caltech, LSU, MIT, LLO Rich Abbott, Graham Allen, Daniel DeBra, Dennis Coyne, Jeremy Faludi, Amit Ganguli, Joe Giaime, Marcel Hammond, Corwin

More information

LIGO s Thermal Noise Interferometer: Progress and Status

LIGO s Thermal Noise Interferometer: Progress and Status LIGO s Thermal Noise Interferometer: Progress and Status Eric Black LSC Meeting Review November 12, 2003 Ivan Grudinin, Akira Villar, Kenneth G. Libbrecht Thanks also to: Kyle Barbary, Adam Bushmaker,

More information

Next Generation Interferometers

Next Generation Interferometers Next Generation Interferometers TeV 06 Madison Rana Adhikari Caltech 1 Advanced LIGO LIGO mission: detect gravitational waves and initiate GW astronomy Next detector» Should have assured detectability

More information

BASELINE SUSPENSION DESIGN FOR LIGO II - UPDATE

BASELINE SUSPENSION DESIGN FOR LIGO II - UPDATE BASELINE SUSPENSION DESIGN FOR LIGO II - UPDATE Norna A Robertson University of Glasgow for the GEO suspension team LSC, Hanford 15th August 2000 LIGO-G000295-00-D GEO suspension team for LIGO II G Cagnoli,

More information

Seismic isolation and suspension systems for Advanced LIGO

Seismic isolation and suspension systems for Advanced LIGO Seismic isolation and suspension systems for Advanced LIGO N. A. Robertson*,a,b,, B Abbott c, R. Abbott d, R. Adhikari e, G. Allen a, H. Armandula c, S. Aston f, A. Baglino a, M. Barton c, B. Bland g,

More information

After ~ 40 years of effort, no one has detected a GW! Why? Noise levels in detectors exceed expected

After ~ 40 years of effort, no one has detected a GW! Why? Noise levels in detectors exceed expected NOISE in GW detectors After ~ 40 years of effort, no one has detected a GW! Why? Noise levels in detectors exceed expected signal; insufficient sensitivity Want to detect GW strain h; can express detector

More information

6WDWXVRI/,*2. Laser Interferometer Gravitational-wave Observatory. Nergis Mavalvala MIT IAU214, August 2002 LIGO-G D

6WDWXVRI/,*2. Laser Interferometer Gravitational-wave Observatory. Nergis Mavalvala MIT IAU214, August 2002 LIGO-G D 6WDWXVRI/,*2 Laser Interferometer Gravitational-wave Observatory Hanford, WA Livingston, LA Nergis Mavalvala MIT IAU214, August 2002 *UDYLWDWLRQDOZDYH,QWHUIHURPHWHUVWKHSULQ LSOH General Relativity (Einstein

More information

LASER INTERFEROMETER GRAVITATIONAL WAVE OBSERVATORY. LIGO Scientific Collaboration. Enhanced LIGO. R Adhikari. Distribution of this draft:

LASER INTERFEROMETER GRAVITATIONAL WAVE OBSERVATORY. LIGO Scientific Collaboration. Enhanced LIGO. R Adhikari. Distribution of this draft: LASER INTERFEROMETER GRAVITATIONAL WAVE OBSERVATORY LIGO LIGO Scientific Collaboration LIGO T06009-00-I May 006 Enhanced LIGO R Adhikari Distribution of this draft: LIGO Scientific Collaboration This is

More information

Advanced LIGO Research and Development

Advanced LIGO Research and Development Advanced LIGO Research and Development David Shoemaker NSF Annual Review of LIGO 17 November 2003 LIGO Laboratory 1 LIGO mission: detect gravitational waves and initiate GW astronomy Commissioning talk

More information

Development of ground based laser interferometers for the detection of gravitational waves

Development of ground based laser interferometers for the detection of gravitational waves Development of ground based laser interferometers for the detection of gravitational waves Rahul Kumar ICRR, The University of Tokyo, 7 th March 2014 1 Outline 1. Gravitational waves, nature & their sources

More information

Advanced LIGO, Advanced VIRGO and KAGRA: Precision Measurement for Astronomy. Stefan Ballmer For the LVC Miami 2012 Dec 18, 2012 LIGO-G

Advanced LIGO, Advanced VIRGO and KAGRA: Precision Measurement for Astronomy. Stefan Ballmer For the LVC Miami 2012 Dec 18, 2012 LIGO-G Advanced LIGO, Advanced VIRGO and KAGRA: Precision Measurement for Astronomy Stefan Ballmer For the LVC Miami 2012 Dec 18, 2012 LIGO-G1201293 Outline Introduction: What are Gravitational Waves? The brief

More information

Advanced LIGO Optical Configuration and Prototyping Effort

Advanced LIGO Optical Configuration and Prototyping Effort Advanced LIGO Optical Configuration and Prototyping Effort Alan Weinstein *, representing the LIGO Scientific Collaboration Advanced Interferometer Configurations Working Group, and the LIGO 40 Meter Group

More information

LIGO Status Report 1. LIGO I. 2. E7 run (Dec.28,2001 ~ Jan.14,2002) 3. Advanced LIGO. Hiro Yamamoto

LIGO Status Report 1. LIGO I. 2. E7 run (Dec.28,2001 ~ Jan.14,2002) 3. Advanced LIGO. Hiro Yamamoto LIGO Status Report Hiro Yamamoto LIGO Laboratory / California Institute of Technology 1. LIGO I 2. E7 run (Dec.28,2001 ~ Jan.14,2002) 3. Advanced LIGO References : M.Coles (G020009), D.Coyne and D.Shoemaker

More information

Advanced LIGO Research and Development

Advanced LIGO Research and Development Advanced LIGO Research and Development David Shoemaker NSF Annual Review of LIGO 17 October 2003 LIGO Laboratory 1 LIGO mission: detect gravitational waves and initiate GW astronomy Commissioning talk

More information

Prospects for joint transient searches with LOFAR and the LSC/Virgo gravitational wave interferometers

Prospects for joint transient searches with LOFAR and the LSC/Virgo gravitational wave interferometers Prospects for joint transient searches with LOFAR and the LSC/Virgo gravitational wave interferometers Ed Daw - University of Sheffield On behalf of the LIGO Scientific Collaboration and the Virgo collaboration

More information

Long-term strategy on gravitational wave detection from European groups

Long-term strategy on gravitational wave detection from European groups Longterm strategy on gravitational wave detection from European groups Barry Barish APPEC Meeting London, UK 29Jan04 International Interferometer Network Simultaneously detect signal (within msec) LIGO

More information

Gary Sanders LIGO/Caltech LSC Meeting, LLO March 16, 2004 LIGO-G M

Gary Sanders LIGO/Caltech LSC Meeting, LLO March 16, 2004 LIGO-G M State of State the LIGO of LIGO Laboratory Gary Sanders LIGO/Caltech LSC Meeting, LLO March 16, 2004 A 10 Year Anniversary LIGO s near death experience of early 1994» LIGO s second chance What was our

More information

LIGO workshop What Comes Next for LIGO May 7-8, 2015, Silver Spring, MD KAGRA KAGRA. Takaaki Kajita, ICRR, Univ. of Tokyo for the KAGRA collaboration

LIGO workshop What Comes Next for LIGO May 7-8, 2015, Silver Spring, MD KAGRA KAGRA. Takaaki Kajita, ICRR, Univ. of Tokyo for the KAGRA collaboration LIGO workshop What Comes Next for LIGO May 7-8, 2015, Silver Spring, MD KAGRA KAGRA Takaaki Kajita, ICRR, Univ. of Tokyo for the KAGRA collaboration Outline Introduction: Overview of KAGRA Status of the

More information

Advanced LIGO Reference Design

Advanced LIGO Reference Design LIGO Laboratory / LIGO Scientific Collaboration LIGO-060056-07-M Advanced LIGO 29 August 2006 Advanced LIGO Reference Design Advanced LIGO Team This is an internal working note of the LIGO Laboratory.

More information

Gravitational Waves and LIGO

Gravitational Waves and LIGO Gravitational Waves and LIGO Ray Frey, University of Oregon 1. GW Physics and Astrophysics 2. How to detect GWs The experimental challenge 3. Prospects June 16, 2004 R. Frey QNet 1 General Relativity Some

More information

Review of LIGO Upgrade Plans

Review of LIGO Upgrade Plans Ando Lab Seminar April 13, 2017 Review of LIGO Upgrade Plans Yuta Michimura Department of Physics, University of Tokyo Contents Introduction A+ Voyager Cosmic Explorer Other issues on ISC Summary KAGRA+

More information

Interferometry beyond the Standard Quantum Limit using a Sagnac Speedmeter Stefan Hild

Interferometry beyond the Standard Quantum Limit using a Sagnac Speedmeter Stefan Hild Interferometry beyond the Standard Quantum Limit using a Sagnac Speedmeter Stefan Hild ET general meeting Hannover, December 2012 Overview Ü What is a speedmeter and how does it work? Ü Could a Sagnac

More information

Displacement Noises in Laser Interferometric Gravitational Wave Detectors

Displacement Noises in Laser Interferometric Gravitational Wave Detectors Gravitational Wave Physics @ University of Tokyo Dec 12, 2017 Displacement Noises in Laser Interferometric Gravitational Wave Detectors Yuta Michimura Department of Physics, University of Tokyo Slides

More information

An Overview of Advanced LIGO Interferometry

An Overview of Advanced LIGO Interferometry An Overview of Advanced LIGO Interferometry Luca Matone Columbia Experimental Gravity group (GECo) Jul 16-20, 2012 LIGO-G1200743 Day Topic References 1 2 3 4 5 Gravitational Waves, Michelson IFO, Fabry-Perot

More information

Gravitational Waves and LIGO: A Technical History

Gravitational Waves and LIGO: A Technical History Gravitational Waves and LIGO: A Technical History Stan Whitcomb IEEE SV Tech History Committee Event 11 October 2018 LIGO-G180195-v3 Goal of Talk Review a few of the technical developments that enabled

More information

Ground-based GW detectors: status of experiments and collaborations

Ground-based GW detectors: status of experiments and collaborations Ground-based GW detectors: status of experiments and collaborations C.N.Man Univ. Nice-Sophia-Antipolis, CNRS, Observatoire de Cote d Azur A short history GW & how to detect them with interferometry What

More information

Innovative Technologies for the Gravitational-Wave Detectors LIGO and Virgo

Innovative Technologies for the Gravitational-Wave Detectors LIGO and Virgo Innovative Technologies for the Gravitational-Wave Detectors LIGO and Virgo Jan Harms INFN, Sezione di Firenze On behalf of LIGO and Virgo 1 Global Network of Detectors LIGO GEO VIRGO KAGRA LIGO 2 Commissioning

More information

Squeezed Light for Gravitational Wave Interferometers

Squeezed Light for Gravitational Wave Interferometers Squeezed Light for Gravitational Wave Interferometers R. Schnabel, S. Chelkowski, H. Vahlbruch, B. Hage, A. Franzen, and K. Danzmann. Institut für Atom- und Molekülphysik, Universität Hannover Max-Planck-Institut

More information

Advanced LIGO Optical Configuration, Prototyping, and Modeling

Advanced LIGO Optical Configuration, Prototyping, and Modeling Advanced LIGO Optical Configuration, Prototyping, and Modeling Alan Weinstein *, representing the LIGO Scientific Collaboration Advanced Interferometer Configurations Working Group, and the LIGO 40 Meter

More information

LIGO I status and advanced LIGO proposal

LIGO I status and advanced LIGO proposal LIGO I status and advanced LIGO proposal Hiro Yamamoto LIGO Lab / Caltech LIGO I» basic design» current status advanced LIGO» outline of the proposal» technical issues GW signals and data analysis ICRR

More information

Advanced Virgo and LIGO: today and tomorrow

Advanced Virgo and LIGO: today and tomorrow Advanced Virgo and LIGO: today and tomorrow Michał Was for the LIGO and Virgo collaborations Michał Was (SFP Gravitation) 2017 Nov 22 1 / 21 d Basics of interferometric gravitational wave detections Need

More information

Squeezed Light Techniques for Gravitational Wave Detection

Squeezed Light Techniques for Gravitational Wave Detection Squeezed Light Techniques for Gravitational Wave Detection July 6, 2012 Daniel Sigg LIGO Hanford Observatory Seminar at TIFR, Mumbai, India G1200688-v1 Squeezed Light Interferometry 1 Abstract Several

More information

Interferometric. Gravitational Wav. Detectors. \p World Scientific. Fundamentals of. Peter R. Sawlson. Syracuse University, USA.

Interferometric. Gravitational Wav. Detectors. \p World Scientific. Fundamentals of. Peter R. Sawlson. Syracuse University, USA. SINGAPORE HONGKONG Fundamentals of Interferometric Gravitational Wav Detectors Second Edition Peter R. Sawlson Martin A. Pomerantz '37 Professor of Physics Syracuse University, USA \p World Scientific

More information

The Advanced LIGO detectors at the beginning of the new gravitational wave era

The Advanced LIGO detectors at the beginning of the new gravitational wave era The Advanced LIGO detectors at the beginning of the new gravitational wave era Lisa Barsotti MIT Kavli Institute LIGO Laboratory on behalf of the LIGO Scientific Collaboration LIGO Document G1600324 LIGO

More information

Advanced Virgo: Status and Perspectives. A.Chiummo on behalf of the VIRGO collaboration

Advanced Virgo: Status and Perspectives. A.Chiummo on behalf of the VIRGO collaboration Advanced Virgo: Status and Perspectives A.Chiummo on behalf of the VIRGO collaboration Advanced Virgo 2 Advanced Virgo What s that? 3 Advanced Virgo Advanced Virgo (AdV): upgrade of the Virgo interferometric

More information

Status and Plans for Future Generations of Ground-based Interferometric Gravitational-Wave Antennas

Status and Plans for Future Generations of Ground-based Interferometric Gravitational-Wave Antennas Status and Plans for Future Generations of Ground-based Interferometric Gravitational-Wave Antennas 4 th international LISA Symposium July 22, 2002 @ Penn State University Seiji Kawamura National Astronomical

More information

Gravitational Waves & Precision Measurements

Gravitational Waves & Precision Measurements Gravitational Waves & Precision Measurements Mike Smith 1 -20 2 HOW SMALL IS THAT? Einstein 1 meter 1/1,000,000 3 1,000,000 smaller Wavelength of light 10-6 meters 1/10,000 4 10,000 smaller Atom 10-10

More information

Status of the LIGO Project

Status of the LIGO Project Status of the LIGO Project Gary Sanders California Institute of Technology LSC Meeting University of Florida - March 4, 1999 1 LIGO-G990012-00-M LIGO-G990022-02-M LIGO Schedule at Very Top Level 1996 Construction

More information

April 21-23, Barry Barish LIGO-G M

April 21-23, Barry Barish LIGO-G M LIGO NSF Review April 21-23, 1999 Overview Barry Barish LIGO Plans main activity 1996 Construction Underway -mostly civil 1997 Facility Construction -vacuum system 1998 Interferometer Construction -complete

More information

Gravitational Wave Astronomy

Gravitational Wave Astronomy Gravitational Wave Astronomy Giles Hammond SUPA, University of Glasgow, UK on behalf of the LIGO Scientific Collaboration and the Virgo Collaboration 14 th Lomonosov conference on Elementary Particle Physics

More information

GEO 600: Advanced Techniques in Operation

GEO 600: Advanced Techniques in Operation GEO 600: Advanced Techniques in Operation Katherine Dooley for the GEO team DCC# G1400554-v1 LISA Symposium X Gainesville, FL May 21, 2014 GEO600 Electronics shop Corner building Operator's station Offices

More information

Towards Sagnac speed meter interferometers for gravitational wave detection

Towards Sagnac speed meter interferometers for gravitational wave detection Towards Sagnac speed meter interferometers for gravitational wave detection Christian Gräf for the Glasgow Sagnac Speed Meter Team ICONO/LAT Conference, September 2016 Minsk, Belarus LIGO-G1601997 Outline

More information

Probing for Gravitational Waves

Probing for Gravitational Waves Probing for Gravitational Waves LIGO Reach with LIGO AdLIGO Initial LIGO Barry C. Barish Caltech YKIS2005 Kyoto University 1-July-05 Einstein s Theory of Gravitation a necessary consequence of Special

More information

The LIGO Experiment Present and Future

The LIGO Experiment Present and Future The LIGO Experiment Present and Future Keith Riles University of Michigan For the LIGO Scientific Collaboration APS Meeting Denver May 1 4, 2004 LIGO-G040239-00-Z What are Gravitational Waves? Gravitational

More information

Overview Ground-based Interferometers. Barry Barish Caltech Amaldi-6 20-June-05

Overview Ground-based Interferometers. Barry Barish Caltech Amaldi-6 20-June-05 Overview Ground-based Interferometers Barry Barish Caltech Amaldi-6 20-June-05 TAMA Japan 300m Interferometer Detectors LIGO Louisiana 4000m Virgo Italy 3000m AIGO Australia future GEO Germany 600m LIGO

More information

Gauss Modes. Paul Fulda

Gauss Modes. Paul Fulda Interferometry Interferometry with with LaguerreLaguerreGauss Gauss Modes Modes Paul Paul Fulda Fulda University University of of Birmingham Birmingham E.T. E.T. WP3 WP3 Meeting Meeting -- -- 09/06/2009

More information

Seismic isolation of Advanced LIGO: Review of strategy, instrumentation and performance

Seismic isolation of Advanced LIGO: Review of strategy, instrumentation and performance Classical and Quantum Gravity PAPER Seismic isolation of Advanced LIGO: Review of strategy, instrumentation and performance To cite this article: F Matichard et al 0 Class. Quantum Grav. 00 Manuscript

More information

Gravitational Wave Detection from the Ground Up

Gravitational Wave Detection from the Ground Up Gravitational Wave Detection from the Ground Up Peter Shawhan (University of Maryland) for the LIGO Scientific Collaboration LIGO-G080393-00-Z From Simple Beginnings Joe Weber circa 1969 AIP Emilio Segre

More information

LIGO On-line Documents July 1997

LIGO On-line Documents July 1997 LASER INTERFEROMETER GRAVITATIONAL WAVE OBSERVATORY - LIGO - CALIFORNIA INSTITUTE OF TECHNOLOGY MASSACHUSETTS INSTITUTE OF TECHNOLOGY Document Type LIGO-T970089-05- P 7/22/97 LIGO On-line Documents July

More information

Advanced LIGO the Laser Interferometer Gravitational-wave Observatory The Next Gravitational-Wave Observatory

Advanced LIGO the Laser Interferometer Gravitational-wave Observatory The Next Gravitational-Wave Observatory Advanced LIGO the Laser Interferometer Gravitational-wave Observatory The Next Gravitational-Wave Observatory Brian Lantz, for the LSC (40+ institutions, hundreds of people) SLAC Instrumentation Series,

More information

LIGO: On the Threshold of Gravitational-wave Astronomy

LIGO: On the Threshold of Gravitational-wave Astronomy LIGO: On the Threshold of Gravitational-wave Astronomy Stan Whitcomb LIGO/Caltech IIT, Kanpur 18 December 2011 Outline of Talk Quick Review of GW Physics and Astrophysics LIGO Overview» Initial Detectors»

More information

The Status of Enhanced LIGO.

The Status of Enhanced LIGO. The Status of Enhanced LIGO. Aidan Brooks. December 2008 AIP Congress 2008, Adelaide, Australia 1 Outline Gravitational Waves» Potential sources» Initial LIGO interferometer Enhanced LIGO upgrades» Increased

More information

The Quantum Limit and Beyond in Gravitational Wave Detectors

The Quantum Limit and Beyond in Gravitational Wave Detectors The Quantum Limit and Beyond in Gravitational Wave Detectors Gravitational wave detectors Quantum nature of light Quantum states of mirrors Nergis Mavalvala GW2010, UMinn, October 2010 Outline Quantum

More information

Enhancing sensitivity of gravitational wave antennas, such as LIGO, via light-atom interaction

Enhancing sensitivity of gravitational wave antennas, such as LIGO, via light-atom interaction Enhancing sensitivity of gravitational wave antennas, such as LIGO, via light-atom interaction Eugeniy E. Mikhailov The College of William & Mary, USA New Laser Scientists, 4 October 04 Eugeniy E. Mikhailov

More information

CLIO. Presenter : : Shinji Miyoki. S.Telada (AIST) A.Yamamoto, T.Shintomi (KEK) and CLIO collaborators

CLIO. Presenter : : Shinji Miyoki. S.Telada (AIST) A.Yamamoto, T.Shintomi (KEK) and CLIO collaborators CLIO Presenter : : Shinji Miyoki T.Uchiyama, K.Yamamoto, T.Akutsu M.Ohashi, K.Kuroda,,,(ICRR) S.Telada (AIST) T.Tomaru, T.Suzuki, T.Haruyama. N.Sato, A.Yamamoto, T.Shintomi (KEK) and CLIO collaborators

More information

LIGO: The Laser Interferometer Gravitational Wave Observatory

LIGO: The Laser Interferometer Gravitational Wave Observatory LIGO: The Laser Interferometer Gravitational Wave Observatory Credit: Werner Benger/ZIB/AEI/CCT-LSU Michael Landry LIGO Hanford Observatory/Caltech for the LIGO Scientific Collaboration (LSC) http://www.ligo.org

More information

LIGO Present and Future. Barry Barish Directory of the LIGO Laboratory

LIGO Present and Future. Barry Barish Directory of the LIGO Laboratory LIGO Present and Future Barry Barish Directory of the LIGO Laboratory LIGO I Schedule and Plan LIGO I has been built by LIGO Lab (Caltech & MIT) 1996 Construction Underway (mostly civil) 1997 Facility

More information

Searching for Stochastic Gravitational Wave Background with LIGO

Searching for Stochastic Gravitational Wave Background with LIGO Searching for Stochastic Gravitational Wave Background with LIGO Vuk Mandic University of Minnesota 09/21/07 Outline LIGO Experiment:» Overview» Status» Future upgrades Stochastic background of gravitational

More information

The Status of KAGRA Underground Cryogenic Gravitational Wave Telescope

The Status of KAGRA Underground Cryogenic Gravitational Wave Telescope TAUP2017 @ Laurentian University Jul 26, 2017 The Status of KAGRA Underground Cryogenic Gravitational Wave Telescope Yuta Michimura Department of Physics, University of Tokyo on behalf of the KAGRA Collaboration

More information

ISC In-vacuum Gouy phase telescopes

ISC In-vacuum Gouy phase telescopes LASER INTERFEROMETER GRAVITATIONAL WAVE OBSERVATORY - LIGO - CALIFORNIA INSTITUTE OF TECHNOLOGY MASSACHUSETTS INSTITUTE OF TECHNOLOGY Technical Note LIGO-T1247-v3 211/3/5 ISC In-vacuum Gouy phase telescopes

More information

How to measure a distance of one thousandth of the proton diameter? The detection of gravitational waves

How to measure a distance of one thousandth of the proton diameter? The detection of gravitational waves How to measure a distance of one thousandth of the proton diameter? The detection of gravitational waves M. Tacca Laboratoire AstroParticule et Cosmologie (APC) - Paris Journée GPhys - 2016 July 6th General

More information

Squeezing manipulation with atoms

Squeezing manipulation with atoms Squeezing manipulation with atoms Eugeniy E. Mikhailov The College of William & Mary March 21, 2012 Eugeniy E. Mikhailov (W&M) Squeezing manipulation LSC-Virgo (March 21, 2012) 1 / 17 About the college

More information

Experimental measurements of coating mechanical loss factors

Experimental measurements of coating mechanical loss factors INSTITUTE OF PHYSICS PUBLISHING Class. Quantum Grav. 21 (2004) S1059 S1065 CLASSICAL AND QUANTUM GRAVITY PII: S0264-9381(04)69009-5 Experimental measurements of coating mechanical loss factors D R M Crooks

More information

The gravitational wave detector VIRGO

The gravitational wave detector VIRGO The gravitational wave detector VIRGO for the VIRGO collaboration Raffaele Flaminio Laboratoire d Annecy-le-Vieux de Physique des Particules (LAPP) IN2P3 - CNRS Summary I. A bit of gravitational wave physics

More information

3 LIGO: The Basic Idea

3 LIGO: The Basic Idea 3 LIGO: The Basic Idea LIGO uses interference of light waves to detect gravitational waves. This is accomplished using a device called an interferometer. LIGO actually uses several interferometers for

More information

Advanced LIGO: Context and Overview

Advanced LIGO: Context and Overview Advanced LIGO Advanced LIGO: Context and Overview Gravitational waves offer a remarkable opportunity to see the universe from a new perspective, providing access to astrophysical insights that are available

More information

Physics of LIGO Lecture 2

Physics of LIGO Lecture 2 Last week: LIGO project GW physics, astrophysical sources Principles of GW IFO s This week: Engineering and Science runs Noise in GW IFOs Focus on thermal noise Next week: Optics Control systems Advanced

More information

Present and Future. Nergis Mavalvala October 09, 2002

Present and Future. Nergis Mavalvala October 09, 2002 Gravitational-wave Detection with Interferometers Present and Future Nergis Mavalvala October 09, 2002 1 Interferometric Detectors Worldwide LIGO TAMA LISA LIGO VIRGO GEO 2 Global network of detectors

More information

The Search for Gravitational Waves

The Search for Gravitational Waves The Search for Gravitational Waves Fred Raab, LIGO Hanford Observatory, on behalf of the LIGO Scientific Collaboration 21 October 2008 Outline What are gravitational waves? What do generic detectors look

More information

Large-scale Cryogenic Gravitational wave Telescope (LCGT) TAMA/CLIO/LCGT Collaboration Kazuaki KURODA

Large-scale Cryogenic Gravitational wave Telescope (LCGT) TAMA/CLIO/LCGT Collaboration Kazuaki KURODA 29-March, 2009 JPS Meeting@Rikkyo Univ Large-scale Cryogenic Gravitational wave Telescope (LCGT) TAMA/CLIO/LCGT Collaboration Kazuaki KURODA Overview of This talk Science goal of LCGT First detection of

More information

AdvLIGO Static Interferometer Simulation

AdvLIGO Static Interferometer Simulation AdvLIGO Static Interferometer Simulation Hiro Yamamoto, Caltech/LIGO AdvLIGO simulation tools» Stationary, frequency domain and time domain Stationary Interferometer Simulation, SIS, basic» Motivation»

More information

Fused silica suspension for the Virgo optics: status and perspectives

Fused silica suspension for the Virgo optics: status and perspectives Fused silica suspension for the Virgo optics: status and perspectives Helios Vocca for the Virgo Perugia Group The expected Virgo Sensitivity 10-15 Total sensitivity h(f) [1/sqrt(Hz)] 10-16 10-17 10-18

More information

Advanced Virgo: status and gravitational waves detection. Flavio Travasso on behalf of Virgo Collaboration INFN Perugia - University of Perugia - EGO

Advanced Virgo: status and gravitational waves detection. Flavio Travasso on behalf of Virgo Collaboration INFN Perugia - University of Perugia - EGO Advanced Virgo: status and gravitational waves detection Flavio Travasso on behalf of Virgo Collaboration INFN Perugia - University of Perugia - EGO Minkowski vs general metric dx dx ds 2 1 1 1 1 Flat

More information

Progress in Gravitational Wave Detection: Interferometers

Progress in Gravitational Wave Detection: Interferometers 1 Progress in Gravitational Wave Detection: Interferometers Kazuaki Kuroda a and LCGT Collaboration b a Institute for Cosmic Ray Research, The University of Tokyo, 5-1-5, Kashiwanoha, Kashiwa, Chiba 277-8582,

More information

Gearing up for Gravitational Waves: the Status of Building LIGO

Gearing up for Gravitational Waves: the Status of Building LIGO Gearing up for Gravitational Waves: the Status of Building LIGO Frederick J. Raab, LIGO Hanford Observatory LIGO s Mission is to Open a New Portal on the Universe In 1609 Galileo viewed the sky through

More information

Advanced LIGO, LIGO-Australia and the International Network

Advanced LIGO, LIGO-Australia and the International Network Advanced LIGO, LIGO-Australia and the International Network Stan Whitcomb LIGO/Caltech IndIGO - ACIGA meeting on LIGO-Australia 8 February 2011 Gravitational Waves Einstein in 1916 and 1918 recognized

More information

Advanced LIGO Project Book

Advanced LIGO Project Book Advanced LIGO Project Book 1. Overview To be done 20 jan03 Project Summary (1-2 pages) Insert costs and schedule Following the initial LIGO scientific observation period, planned for 2003 through 2006,

More information

The Advanced LIGO Gravitational Wave Detector arxiv: v1 [gr-qc] 14 Mar Introduction

The Advanced LIGO Gravitational Wave Detector arxiv: v1 [gr-qc] 14 Mar Introduction The Advanced LIGO Gravitational Wave Detector arxiv:1103.2728v1 [gr-qc] 14 Mar 2011 S. J. Waldman, for the LIGO Scientific Collaboration LIGO Laboratory, Kavli Institute for Astrophysics and Space Research,

More information

Adaptive Thermal Compensation Advanced Photodetectors Photon Drive

Adaptive Thermal Compensation Advanced Photodetectors Photon Drive Adaptive Thermal Compensation Advanced Photodetectors Photon Drive M. E. Zucker LIGO Project, MIT Center for Space Research National Science Foundation Review Caltech, 29 January - 1 February 2001 LIGO-G010015-00-D

More information

Plans for Advanced Virgo

Plans for Advanced Virgo Plans for Advanced Virgo Raffaele Flaminio Laboratoire des Materiaux Avances CNRS/IN2P3 On behalf of the Virgo-IN2P3 groups (APC, LAL, LAPP, LMA) SUMMARY - Scientific case - Detector design - The IN2P3

More information

The Quest to Detect Gravitational Waves

The Quest to Detect Gravitational Waves The Quest to Detect Gravitational Waves Peter Shawhan California Institute of Technology / LIGO Laboratory What Physicists Do lecture Sonoma State University March 8, 2004 LIGO-G040055-00-E Outline Different

More information

Design of a Tuned Mass Damper for High Quality Factor Suspension Modes in Advanced LIGO I. INTRODUCTION

Design of a Tuned Mass Damper for High Quality Factor Suspension Modes in Advanced LIGO I. INTRODUCTION Design of a Tuned Mass Damper for High Quality Factor Suspension Modes in Advanced LIGO N A Robertson 1, a), b), P. Fritschel 2, B. Shapiro 3, C. I. Torrie 1, M. Evans 2 1 LIGO, California Institute of

More information

Physics of LIGO Lecture 3

Physics of LIGO Lecture 3 Physics of LIGO Lecture 3 Last week: LIGO project GW physics, astrophysical sources Principles of GW IFO s Engineering and Science runs Noise in GW IFOs Focus on thermal noise This week: Cavity Optics

More information

The Investigation of Geometric Anti-springs Applied to Euler Spring Vibration Isolators

The Investigation of Geometric Anti-springs Applied to Euler Spring Vibration Isolators The Investigation of Geometric Anti-springs Applied to Euler Spring Vibration Isolators Eu-Jeen Chin Honours 2002 School of Physics Supervisors: Prof. David Blair Dr. Li Ju Dr. John Winterflood The University

More information

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

The gravitational waves detection: 20 years of research to deliver the LIGO/VIRGO mirrors. Christophe MICHEL on behalf of LMA Team Christophe MICHEL on behalf of LMA Team 1 The event February 11th 2016 LIGO and VIRGO announced the first direct detection of gravitational waves https://www.youtube.com/watch?v=vd1pak5f6gq http://journals.aps.org/prl/abstract/10.1103/physrevlett.1

More information

Advanced VIRGO EXPERIMENT

Advanced VIRGO EXPERIMENT Advanced VIRGO EXPERIMENT Advanced VIRGO Interferometer: a second generation detector for Gravitational Waves observation F. Frasconi for the VIRGO Collaboration 16 th Lomonosov Conference Moscow State

More information

Effects of Ultraviolet Irradiation on LIGO Mirror Coating

Effects of Ultraviolet Irradiation on LIGO Mirror Coating Effects of Ultraviolet Irradiation on LIGO Mirror Coating Ke-Xun Sun, Nick Leindecker, Ashot Markosyan, Sasha Buchman, Roger Route, Marty Fejer, Robert Byer, Helena Armandula, Dennis Ugolini, Gregg Harry

More information

v P Q LASER Phase Modulator MHz v I +90 Q

v P Q LASER Phase Modulator MHz v I +90 Q Plans for the 40m Upgrade ffl The 40m Program ffl Purpose of the upgrade ffl Timescale why now? ffl Restrictions on the scope of the upgrade ffl Obvious anticipated upgrades ffl Paths towards advanced

More information

No signal yet: The elusive birefringence of the vacuum, and whether gravitational wave detectors may help

No signal yet: The elusive birefringence of the vacuum, and whether gravitational wave detectors may help Nosignalyet: Theelusivebirefringenceofthe vacuum,andwhether gravitationalwavedetectors mayhelp HartmutGrote AEIHannover CaJAGWR, Caltech 24.Feb.2015 Horror Vacui? Otto Von Guerrike 1654/1656 Vacuum The

More information

System Failure Diagnosis for the Advanced LIGO HAM Chamber Seismic Isolation System

System Failure Diagnosis for the Advanced LIGO HAM Chamber Seismic Isolation System System Failure Diagnosis for the Advanced LIGO HAM Chamber Seismic Isolation System A THESIS SUBMITTED TO THE DEPARTMENT OF AERONAUTIC AND ASTRONAUTIC ENGINEERING AND THE COMMITTEE ON GRADUATE STUDIES

More information

Recent LIGO I simulation results

Recent LIGO I simulation results Recent LIGO I simulation results Hiro Yamamoto / Caltech - LIGO Lab As-built LIGO I performance and the path to it FFT run with as-built HR phase map» Contrast defect» Shot noise limited sensitivity» R.Dodda(SLU),

More information

Advanced LIGO Two-Stage Twelve-Axis Vibration. Part 2: Experimental Investigation and Tests Results

Advanced LIGO Two-Stage Twelve-Axis Vibration. Part 2: Experimental Investigation and Tests Results Advanced LIGO Two-Stage Twelve-Axis Vibration Isolation and Positioning Platform Part 2: Experimental Investigation and Tests Results F. Matichard 1,2,*, B. Lantz 3, K. Mason 1, R. Mittleman 1, B. Abbott

More information

Laser Safety for LIGO

Laser Safety for LIGO Laser Safety for LIGO Peter King 8 th Annual DOE Laser Safety Officer Workshop September 12 th, 2012 LIGO G1200825 v1 An Overview of LIGO LIGO is the Laser Interferometer Gravitational Wave Observatory

More information

The technology behind LIGO: how to measure displacements of meters

The technology behind LIGO: how to measure displacements of meters The technology behind LIGO: how to measure displacements of 10-19 meters The LIGO interferometers Interferometry: displacement sensing Noise limits Advanced LIGO 4pm today, 1 West: Results from science

More information

Nonequilibrium issues in macroscopic experiments

Nonequilibrium issues in macroscopic experiments Nonequilibrium issues in macroscopic experiments L. Conti, M. Bonaldi, L. Rondoni www.rarenoise.lnl.infn.it European Research Council Gravitational Wave detector Motivation: GWs will provide new and unique

More information

LIGO s Detection of Gravitational Waves from Two Black Holes

LIGO s Detection of Gravitational Waves from Two Black Holes LIGO s Detection of Gravitational Waves from Two Black Holes Gregory Harry Department of Physics, American University February 17,2016 LIGO-G1600274 GW150914 Early History of Gravity Aristotle Kepler Laplace

More information

LISA Pathfinder measuring pico-meters and femto-newtons in space

LISA Pathfinder measuring pico-meters and femto-newtons in space LISA Pathfinder measuring pico-meters and femto-newtons in space M Hewitson for the LPF team Barcelona, February 15th 2012 Observing from Space 2 Observing from Space 2 Observing from Space Push down to

More information