Status of the LIGO Detectors

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Presentation transcript:

Status of the LIGO Detectors 6th EDOARDO AMALDI CONFERENCE, Okinawa, June 21, 2005 Daniel Sigg, LIGO Hanford Observatory

Arial View of the LIGO Sites LIGO Livingston Observatory LIGO Hanford Observatory LIGO I

Time Line 1999 2000 2001 2002 2003 2004 2005 2006 Inauguration First Lock Full Lock all IFO Now 10-21 10-22 4K strain noise at 150 Hz [Hz-1/2] 10-17 10-18 10-20 E2 E3 E5 E7 E8 E9 E10 E11 Engineering First Science Data S1 S4 Science S2 Runs S3 S5 LIGO I

Major Achievements Since Last Amaldi An order of magnitude improvement in sensitivity (at 150Hz) All 3 interferometers within a factor of 2 of design Hydraulic external pre-isolator at Livingston Success! Allows 24 hour operation Thermal compensation system Output Mode Cleaner Test Some good features but “large” acoustic sensitivity S1/S2 analysis published, S3 analysis in progress, S4 run completed LIGO I

The 4th Science Run Dates (2005): Duty cycle: Start: 22 Feb Stop: 23 Mar Duty cycle: H1: 80% L1: 74% H2: 81% Triple coincidence: 57% LIGO I

S4 Sensitivity LIGO I

Results from the 1st/2nd Science Run Binary inspirals (S2): Neutron star binary coalescence: range up to 1.5 Mpc, rate ≤ 47/y/MW (90% CL) Black hole coalescence (0.2-1M) in Galactic halo: rate ≤ 63/y/MW (90% CL) Pulsars (S2): Limits on 28 pulsars Upper limits on h as low as 2×10-24 (95% CL) and as low as 5×10-6 on the eccentricity Stochastic background (S1): Energy limit as fraction of closure density: h2100W0 ≤ 23 ± 4.6 (90% CL) PRELIMINARY S2: h2100W0 ≤ 0.018 +0.007-0.003 (90% CL) Burst (S2): Sensitivity: hrss ~ 10-20 - 10-19 /√Hz, rate ≤ 0.26/day (90% CL) GRB030329: hrss ≤ 6×10-21 /√Hz LIGO I

2001 2003 LIGO I

Hydraulic External Pre-Isolator The payload is supported by large coil springs, and actuated by quiet, high force hydraulic bridges. Vibration reduction is obtained by actively following inertial sensor signals from payload-mounted seismometers and by canceling floor vibrations. LIGO I

X-arm length disturbance, noisy afternoon With HEPI in use, we expect the LLO detector to work on a typical noisy day, with at least a factor of 2 headroom. LIGO I

Thermal Compensation System Over-heat Correction Inhomogeneous Correction Under-heat Correction CO2 Laser ? ZnSe Viewport Over-heat pattern Inner radius = 4cm Outer radius =11cm ITM Cold power recycling cavity is unstable: poor buildup and mode shape for the RF sidebands Require 10’s of mW absorbed by 1μm beam LIGO I

Sideband Images as Function of Thermal Heating No Heating 30 mW 60 mW 90 mW 120 mW 150 mW 180 mW Input beam Best match LIGO I

Sideband Imbalance Schnupp carrier anti-symmetric port + sideband carrier/sideband mode mismatch phase LIGO I

Other Commissioning Highlights Bull’s eye wave front sensor to servo the thermal compensation system Auto-alignment system at full bandwidth Low noise oscillator for main modulation Low noise digital-to-analog converters Acoustic mitigation and isolation improved Reworked common mode feedback path Better control on auxiliary degrees-of-freedom EMI improvements at LLO LIGO I

Summary All LIGO interferometers are within a factor of 2 of design sensitivity over a broad range of frequencies Thermal compensation essential to reach this sensitivity Active pre-isolator essential at LLO to lock during work days For sources like binary neutron star coalescence we can see beyond our own galaxy! Join Einstein@home (einstein.phys.uwm.edu) LIGO I