LIGO- G030546-00-D Gravitational Wave Observations with Interferometers: Results and Prospects Stan Whitcomb for the LIGO Scientific Collaboration 2 nd.

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Presentation transcript:

LIGO- G D Gravitational Wave Observations with Interferometers: Results and Prospects Stan Whitcomb for the LIGO Scientific Collaboration 2 nd Gravitational Wave Phenomenology Workshop Penn State University 6 November 2003

LIGO- G D GWPW03 2 GW interferometers TAMA »First observations Sept 1999 »>80% duty cycle over DT8/S2 run (Feb-Apr 2002) GEO600 »Advanced features—fused silica suspensions, signal recycling, etc. »Stable lock in signal recycled mode – preparing for first observations in this mode Virgo »First arm locked Oct 2003 LIGO »First full interferometer lock Oct 2000 »Total of three interferometers at two sites--L1, H1, H2 (2km) –Essentially identical orientation

LIGO- G D GWPW03 3 S1 S2 Detector Sensitivity Progression Steady improvement in LIGO interferometers - Example: Livingston interferometer (L1) TAMA interferometer - Installation of improved seismic isolation, planned for next year, should aid at low frequencies

LIGO- G D GWPW03 4 First LIGO Science Run (S1) August 23 - September 9 (~400 hours duration) 1st coincidence interferometer observations since 1989 (“100 hour run”) »Three LIGO interferometers, plus GEO (Europe) and TAMA (Japan) Hardware reliability good for this stage in the commissioning »Longest locked segment for LIGO interferometer: 21 hrs LLO-4KLHO-4KLHO-2K3x Coinc.GEO600 Duty cycle42%58%73%24%97%

LIGO- G D GWPW03 5 Astrophysical Searches with Interferometer Data Compact binary inspiral: “chirps” »NS-NS waveforms are well described »BH-BH need better waveforms »search technique: matched templates Supernovae / GRBs: “bursts” »burst signals in coincidence with signals in electromagnetic radiation »prompt alarm (~ one hour) with neutrino detectors Pulsars in our galaxy: “periodic” »search for observed neutron stars (frequency, doppler shift) »all sky search (computing challenge) »r-modes, LMXBs Cosmological Signals “stochastic background”

LIGO- G D GWPW03 6 Compact Binary Coalescence Search technique: matched templates »Neutron Star – Neutron Star –waveforms known with confidence »Black Hole – Black Hole –need better waveforms TAMA DT6 search »m 1 +m 2 < ~10 M  LIGO S1 Search »Discrete set of templates labeled by (m1, m2) –1.0 M  < m1, m2 < 3.0 M  –2110 templates –At most 3% loss in SNR

LIGO- G D GWPW03 7 TAMA Range for Binary Inspirals (total)

LIGO- G D GWPW03 8 Results of S1 Inspiral Search LIGO S1 Upper Limit R < 170 / yr / MWEG (Milky Way Equivalent Galaxy) Theoretical prediction : R ~ / yr / MWEG (??) Potential for improvement : » x increase in range (~20 Mpc) »100 x observation time  Monte Carlo simulation to determine efficiency for detecting galactic events  Simulated Galactic Population includes Milky Way, LMC and SMC  LMC and SMC contribute ~12% TAMA TAMA DT6 Upper Limit R < 120 / yr

LIGO- G D GWPW03 9 Short GW Burst Sources Known sources -- Supernovas & GRBs Coincidence with observed electromagnetic observations. No close events occurred during S1 Second science run – We are analyzing data near the very bright and close GRB (both Hanford detectors and TAMA operating) Unknown phenomena » Emission of short transients of gravitational radiation of unknown waveform (e.g. black hole mergers). S1

LIGO- G D GWPW03 10 ‘Unmodelled’ Burst Search search for waveforms from sources for which we cannot currently make an accurate prediction of the waveform shape. GOAL METHODS ‘Raw Data’ Time-domain high pass filter Time-Frequency Plane ‘TFCLUSTERS’ time frequency tt ff Temporal coincidence Cross correlation Amplitude test Final event list

LIGO- G D GWPW03 11 Determination of Efficiency Detection efficiency vs. amplitude, averaged over source direction and polarization 010 time (ms) amplitude 0 h To determine sensitivity, inject “representative” waveforms into actual data and run through the analysis pipeline 1ms Gaussian burst

LIGO- G D GWPW03 12 LIGO S1 Upper Limit ex: 1ms gaussian bursts Not as good as the best bar results to date, due to their » Longer observation time » Higher sensitivity near 1 kHz Broaden parameter space of waveforms searched » Longer duration bursts » Astrophysically motivated Prospects for improvement : » x detector sensitivity » 300x in observation time » 3x analysis improvements (?) » ?x improved gaussianity 90% confidence Excluded regions in rate-amplitude plane

LIGO- G D GWPW03 13 CW Sources and Search Methods Neutron stars in our galaxy: »Search for observed neutron stars (known location and frequency) »Low mass X-ray binaries (known location, rough frequency range) »Unobserved NS’s (unknown location, unknown frequency) Search Challenges »Frequency modulation of signal due to Earth’s motion »Amplitude modulation due to the detector’s antenna pattern »All sky search represents significant computational challenge Search methods »Time Domain –Computationally easy but best suited to known sources »Frequency Domain –Best suited for large parameter space searches

LIGO- G D GWPW03 14 TAMA Search for SN1987A Evidence of modulated emission at Hz »GW emission expected at 935 Hz »Highest sensitivity region of TAMA300 DT6: ~1000 hours of observation in 2001 Search over ~ 0.1 Hz bandwidth Upper limit »h < 5 x »99% confidence level

LIGO- G D GWPW03 15 Directed Search in LIGO S1 NO DETECTION EXPECTED at S1 sensitivities PSR J Hz Compare searches using time and frequency domain algorithms Confront challenge of coherent analysis of detectors with different orientations on different continents

LIGO- G D GWPW03 16 S1 Result: PSR J Upper limit for targeted pulsar »Comparison of frequency domain and time domain searches 95% upper limits on h: Spindown estimate: h < 1.8 x Prospects for improvement:  x from detector sensitivity (depending on frequency)  10x from observation time IFO Frequentist FDS Bayesian TDS GEO 1.9 x x LLO 2.7 x x LHO-2K 4.0 x x LHO-4K 5.4 x x

LIGO- G D GWPW03 17 Stochastic Background Strength specified by ratio of GW energy density to closure density: Detect by cross-correlating output of two interferometer detectors »Use widely separated detectors to minimize correlated environmental noise Prospects for improvement in  : »10 6 x from detector sensitivity improvements (  h 2 ) »10 x from observation time Hanford - Livingston LHO 2km-LLO 4km 61 Hours of S1 data  GW (40Hz Hz) < 23

LIGO- G D GWPW03 18 Stochastic Background: measurements and predictions S2 LIGO Adv LIGO results projected S1

LIGO- G D GWPW03 19 Second LIGO Science Run (S2) TAMA Data-taking 8 (DT8) February 14 – April 14, 2002 (~ 1400 hours) Three LIGO interferometers and TAMA (Japan) ~10x sensitivity improvement over S1 Duty cycle similar to S1 »Increased sensitivity did not degrade operation »Longest locked stretch ~ 66 hours (LHO-4K) LLO-4KLHO-4KLHO-2K3x Coinc. Duty cycle (cf. S1)37% (42%)74% (58%)58% (73%)22% (24%)

LIGO- G D GWPW03 20 S2 Sensitivity and Stability Inspiral Range for SNR=8 with M  Inspiral Preliminary Calibration Andromeda Galaxy (M31) Large Magellanic Cloud Virgo Cluster “Typical” 12 hours

LIGO- G D GWPW03 21 Third LIGO Science Run (S3) October 31, 2003 – January 5, 2004 Three LIGO interferometers, with some participation by TAMA and GEO Improvements relative to S2 »Sensitivity better by 3-4x for LHO interferometers »Duty cycle improved for LHO interferometers (>80% for H1 so far) »Reduction of acoustic nose coupling (possible source of correlated noise at LHO) »Sensitivity and duty cycle for LLO interferometer ~ S2 level

LIGO- G D GWPW03 22 “Schedule” for Full Sensitivity Operation TAMA »Installation of new seismic isolation system in 2004 »Should lead to improved duty cycle and low f sensitivity GEO600 »Harder to predict schedule because of new technologies »Observations may take a backseat to technology development Virgo »First full interferometer lock within a few months »One year commissioning to bring to full sensitivity (my guess!) LIGO »Installation of external preisolator at LLO in early 2004 »Full sensitivity operation by the end of 2004

LIGO- G D GWPW03 23 Potential for Current Generation of Interferometers »My personal assessment Binary inspirals »NS-NS range ~20 Mpc »BH-BH range ~100 Mpc Continuous waves from neutron stars »Minimum h ~ few x Stochastic background »Minimum  ~ Generic bursts »Minimum E GW < 1 M  for source at 100 Mpc »Less certain than other projections