LIGO- G000333-00-D LSC ASIS Marcel Grossman 2000.07.02LIGO Scientific Collaboration - University of Wisconsin - Milwaukee 1 Astrophysical Source Identification.

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Presentation transcript:

LIGO- G D LSC ASIS Marcel Grossman LIGO Scientific Collaboration - University of Wisconsin - Milwaukee 1 Astrophysical Source Identification and Signature (ASIS) Group: Implementation for LIGO-I Bruce Allen Chair, LSC ASIS working group University of Wisconsin - Milwaukee

LIGO- G D LSC ASIS Marcel Grossman LIGO Scientific Collaboration - University of Wisconsin - Milwaukee 2 What Is ASIS? Subgroup of the LIGO Scientific Collaboration (LSC) Formed: March One of three LSC “data” groups. Meets about once/month (typically 30 people). Mailing list:110 members of whom >25 actively doing ASIS coordinated-work Chair: Bruce Allen Webmaster: Patrick Brady Meeting Organizer: Alan Wiseman Secretary: Alberto Vecchio LIGO Laboratory Liaison: Barry Barish

LIGO- G D LSC ASIS Marcel Grossman LIGO Scientific Collaboration - University of Wisconsin - Milwaukee 3 Purpose of ASIS Development of techniques to search for proposed sources: templates, algorithms and filters for »Inspiral of compact objects »Periodic sources »Stochastic backgrounds »Impulsive sources Blind search methods (unknown sources)

LIGO- G D LSC ASIS Marcel Grossman LIGO Scientific Collaboration - University of Wisconsin - Milwaukee 4 ASIS Web Site: Documents, software, & links Meetings announcements, agendas & minutes Mailing list & archives

LIGO- G D LSC ASIS Marcel Grossman LIGO Scientific Collaboration - University of Wisconsin - Milwaukee 5 Organization of ASIS Work Priorities set in “LSC Data Analysis White Paper” Identified lead groups for different software development/coding tasks Analysis codes collected in public LAL Library »current release 0.4 (last week) »code and documentation available for public examination »easy interface to the LIGO Data Analysis System The ASIS group could use additional help: if you or your research group has something to contribute, please consider joining the LSC.

LIGO- G D LSC ASIS Marcel Grossman LIGO Scientific Collaboration - University of Wisconsin - Milwaukee 6 Science Goals & Assumptions LIGO,GEO & VIRGO bring GW detection into region where it’s plausible to detect astrophysical sources. Compared to previous detectors, they will extend: »amplitude sensitivity by factor (space volume ) »bandwidth by factor of 100 However: no known sources with rates/amplitudes large enough to guarantee detection with LIGO-I, “Well understood” sources are probably too weak for LIGO-I Large uncertainties in rate/amplitude estimates, and no body of prior knowledge/best practice (as in HEP).

LIGO- G D LSC ASIS Marcel Grossman LIGO Scientific Collaboration - University of Wisconsin - Milwaukee 7 Hence: “Opportunistic” Data Analysis Strategy for LIGO-I Initial emphasis is breadth (not depth) »Instrument “broadband”, not tuned for particular source type »Computing resources shared between different GW source types, not targeted at a particular type Maintain ability to recognize unanticipated sources Search for (and set upper limits on) »NS/NS, NS/BH, BH/BH binary coalescence (rate) »Correlated GW emission by Gamma Ray Bursts (energy) »GW emission by known pulsars (amplitude) »GW stochastic background (energy-density) »Nearby strongly GW-emitting pulsars (spatial density) »Generic “burst” sources (rate & amplitude)

LIGO- G D LSC ASIS Marcel Grossman LIGO Scientific Collaboration - University of Wisconsin - Milwaukee 8 Essential GW Searches... Binary Inspiral (pair of compact stars): either observe, or place upper limit on the rate in the Universe »NS/NS well understood (a premiere LIGO design goal) –Waveform can be calculated very accurately –Hulse-Taylor binary (wrong freq for LIGO) is canonical example –Hundreds of NS pulsars are cataloged »NS/BH might offer much stronger signals for 20 solar-mass BH, but –Rate “more” uncertain –Waveform not calculable analytically (or numerically, currently) –Signal processing strategy less certain »BH/BH even more speculative Approach: parallel MPI-based hierarchical search: Gflops drives LIGO computing requirements

LIGO- G D LSC ASIS Marcel Grossman LIGO Scientific Collaboration - University of Wisconsin - Milwaukee 9 …essential GW Searches... Continuous wave sources (e.g., rapidly rotating neutron stars with bumps on them) »Known neutron stars probably too weak to observe with LIGO-I »Data analysis “easy” for observed pulsars with known periods, spin- downs »Data analysis “difficult” for full-sky or partial-sky survey –source waveform not single frequency (spindown) –waveform modulated by earth’s spin, motion around sun, and Jupiter- induced perturbations »Detector-limited search: Petaflops »Practical search (factor of 2 less sensitive in amplitude): Teraflops Approach: hierarchical search, using off-site supercomputers and large beowulf clusters

LIGO- G D LSC ASIS Marcel Grossman LIGO Scientific Collaboration - University of Wisconsin - Milwaukee 10 …essential GW Searches... Stochastic background signals »Produced by early-universe processes (speculative) or unresolved “contemporary” phenomena »A factor of 100 (or more!) smaller in amplitude than detector noise »Analysis method: correlate signals from separated detectors »Approach: “Easy” low bandwidth data analysis problem Gamma-Ray Bursts (poorly understood) »At cosmological distances. Release huge amounts of energy »Approach: correlate GRB catalog with GW burst catalog & h data Black hole formation »Search for characteristic “ringdown” signal emitted by the perturbed horizon when BH is formed or enlarged by merger »Tests Einstein’s theory of GR »Approach: trivial flops - use inspiral search code

LIGO- G D LSC ASIS Marcel Grossman LIGO Scientific Collaboration - University of Wisconsin - Milwaukee 11 …essential GW Searches. Close SN (Feeling lucky today? One/ years.) »Approach: plan duty cycle so one IFO is always in operation » Join the neutrino SN watch Optically observed supernovae »Place limits on in-band signal Neutron stars formed in SN »Rapidly rotating stars may have GW driven instability that spins them up and carries away large angular momentum in first year Unknown signals - for example previously undetected supernovae (unmodeled waveforms) »Use time/frequency methods to add “events” to database »Eventual early-warning for electromagnetic & neutrino observatories »Approach: search for correlation between 2 or more sites

LIGO- G D LSC ASIS Marcel Grossman LIGO Scientific Collaboration - University of Wisconsin - Milwaukee 12 Organization of ASIS Work Current Lead groups for coding/development work: »Albert Einstein Institute (MPG - Potsdam): hierarchical pulsar search »Caltech: directed pulsar search »Cardiff: (1) binary inspiral search - template generation & placement (2) “blind” line-tracking time-frequency search »Cornell: (1) transient source search with power statistic (2) robust stochastic background search »U. Michigan: amplitude-modulation discriminator (antenna pattern) »U. Texas - Brownsville: stochastic background search »U. Wisconsin - Milwaukee: (1) binary inspiral search - hierarchical filtering code (2) hierarchical stack-slide pulsar search Other groups actively participating in ASIS include: CFA, CIT-TAPIR, LLO, Stanford, TAMA, UFG

LIGO- G D LSC ASIS Marcel Grossman LIGO Scientific Collaboration - University of Wisconsin - Milwaukee 13 Pulsar Search: Albert Einstein Institute (Potsdam) Entire AEI gravitational-wave group General-purpose code for targeted or area searches Expected sensitivity: »Infinite CPU: detector-limited sensitivity h~ cos(  t)) »100 Gflops: 4-month equally-sensitive search of Galaxy with no spindown (pulsars > 10 7 years old) in frequency range Hz Area search method: three-step hierarchical 1.Start with database of short (~1 hour-long) FFTs. Combine (with demodulation) 24 of these to make ~1-day long demodulated FFT for large sky- position/spindown “patch”. Identify frequency-space “peaks”. 2.Use Hough transform to look for pattern of peaks consistent with small sky- position/spindown “patch”. 3.If threshold exceeded, follow up with coherent demodulation.

LIGO- G D LSC ASIS Marcel Grossman LIGO Scientific Collaboration - University of Wisconsin - Milwaukee 14 Pulsar Search: Albert Einstein Institute (Potsdam) Current status: »Source database code completed for several source types, from NASA ADC, Princeton Pulsar Group, and Parkes multi-beam survey catalogs. »Earth GPS time to solar-system barycenter time conversion code completed. »Demodulation code completed and tested (used in stages 1 & 3). »Coarse parameter space gridding code now undergoing testing. Fine gridding code now underway »Hough transform code (used in stage 2) coding underway, currently several implementations. Working with VIRGO-Rome group. Open problems: »How to take full advantage of correlations in source-parameter space »Finding a very efficient implementation of the Hough transform

Spectrum from one of the SFTs, with time baseline Tc ~ 1 hour. The signal has f0 = 400Hz, the peak appears at a different freq. because of the Doppler modulation. Spectrum of one of the demodulated FFTs with time baseline Tc ~ 21 hours. Since in this case there is perfect signal- template match there is no power loss and perfect shift of the peak to f0 = 400Hz. - AEI continuous signals search -

LIGO- G D LSC ASIS Marcel Grossman LIGO Scientific Collaboration - University of Wisconsin - Milwaukee 16 Pulsar Search: Caltech Stuart Anderson Search for GW emission from known (radio) pulsars. Will obtain detector-limited sensitivity h~ cos(  t)) using insignificant computational resources. Method: for each known pulsar, fold (add together) time- series GW data using correct period pre-determined from radio data.

LIGO- G D LSC ASIS Marcel Grossman LIGO Scientific Collaboration - University of Wisconsin - Milwaukee 17 Binary Inspiral Search: Cardiff D. Churches and B.S. Sathyaprakash Inspiral waveform template generation and parameter-space gridding. “Half” of binary inspiral search code (filtering “half” from UWM) Produce accurate or “best” waveforms: »2.5 post-Newtonian order »systems from 0.1 to 30 solar masses »Taylor and Pade approximation methods »time-domain & stationary-phase in frequency-domain.

LIGO- G D LSC ASIS Marcel Grossman LIGO Scientific Collaboration - University of Wisconsin - Milwaukee 18 Binary Inspiral Search: Cardiff Current status »time and frequency domain Taylor & Pade approximant code complete for spinless zero-eccentricity systems. »Coding for template placement now underway - should be completed by September.

LIGO- G D LSC ASIS Marcel Grossman LIGO Scientific Collaboration - University of Wisconsin - Milwaukee 19 Line-Tracking Time-Frequency Search: Cardiff R. Balasubramanian, W. Anderson, E. Chassande-Mottin Method looks for “curves” in time-frequency diagram Useful technique for unmodeled sources, such as high- mass binary systems Current status: time-frequency transform code complete: »Wigner-Ville »Windowed FFT »Reassigned Spectrogram Steger’s line-tracking algorithm complete Currently being tested on LIGO engineering data

LIGO- G D LSC ASIS Marcel Grossman LIGO Scientific Collaboration - University of Wisconsin - Milwaukee 20 Power Statistic: Cornell E. Flanagan, P. Brady, J. Creighton Method looks for “rectangles” in time-frequency diagram with excess energy Useful technique for unmodeled sources Code complete Paper documenting method “in preparation”

LIGO- G D LSC ASIS Marcel Grossman LIGO Scientific Collaboration - University of Wisconsin - Milwaukee 21 Robust Stochastic Background Detection: Cornell E. Flanagan, S. Drasco Method to search for stochastic background by correlating two or more detectors Generalization of the “traditional” two-detector correlation method, which gives optimal treatment of some types of non-Gaussian detector noise, in weak signal limit Code being written in collaboration with UTB group and others

LIGO- G D LSC ASIS Marcel Grossman LIGO Scientific Collaboration - University of Wisconsin - Milwaukee 22 Amplitude Modulation Discriminator: U. of Michigan D. Chin, K. Riles Tools to see if the amplitude of a posited source (for example a pulsar) exhibits an amplitude modulation consistent with it’s inferred position. First version is completed, and in LAL library. Testing revealed errors in literature. Next version will: »examine change in antenna pattern when period of wave comparable to storage time in interferometer »take account of variable earth rotation, precession, nutation, oblateness, etc.

LIGO- G D LSC ASIS Marcel Grossman LIGO Scientific Collaboration - University of Wisconsin - Milwaukee 23 Amplitude Modulation Discriminator: U. of Michigan Here is a typical antenna pattern (average sensitivity to both source polarizations):

LIGO- G D LSC ASIS Marcel Grossman LIGO Scientific Collaboration - University of Wisconsin - Milwaukee 24 Stochastic Background Detection: U. Texas - Brownsville J. Romano, M. Diaz, E. Flanagan, A. Vecchio, C. Ungarelli Method to search for stochastic background by correlating two or more detectors Tool-kit for two-detector correlation Filter bank will search for  (f) of “broken power law” form Should enable detector-limited sensitivity of  (f~100 Hz)~10 -6 in four months of integration with the two LIGO detectors.

LIGO- G D LSC ASIS Marcel Grossman LIGO Scientific Collaboration - University of Wisconsin - Milwaukee 25 Hierarchical Binary Inspiral Search: U. Wisconsin - Milwaukee B. Allen, P. Brady, D. Brown, J. Creighton, A. Wiseman The “filtering half” of the binary inspiral search code (Cardiff doing templates, template placement) Implements general N-level hierarchical search through arbitrary set of templates »Family of post-Newtonian binary inspiral waveforms »Black hole horizon-formation ringdown Code now complete. »Being used as example for building/testing LIGO Data Analysis System “Wrapper API” interface »Undergoing first stage of testing (simulated Gaussian noise)

LIGO- G D LSC ASIS Marcel Grossman LIGO Scientific Collaboration - University of Wisconsin - Milwaukee 26 Hierarchical Stack-Slide Pulsar Search: U. Wisconsin - Milwaukee P. Brady, T. Creighton General-purpose code for area or targeted searches. Uses a two-step hierarchy: »On coarse grid: –Demodulate short time-series for given source parameters (sky position & spindown) –Combine resulting FFTs by sliding (depending on source parameters) and adding power. »For grid points exceeding threshold, repeat on (selected) fine grid Expected sensitivity: similar to Hough-transform search (details in papers by Brady & T. Creighton).

LIGO- G D LSC ASIS Marcel Grossman LIGO Scientific Collaboration - University of Wisconsin - Milwaukee 27 Hierarchical Stack-Slide Pulsar Search: U. Wisconsin - Milwaukee Current status: »low-pass filtering code completed »time series resampling completed »power spectrum sliding completed »power spectrum summing completed »Currently at work on fine template bank