Broadband Search for Continuous-Wave Gravitation Radiation with LIGO Vladimir Dergachev (University of Michigan) for the LIGO/Virgo scientific collaboration.

Slides:



Advertisements
Similar presentations
A walk through some statistic details of LSC results.
Advertisements

GWDAW 11 - Potsdam, 19/12/ Coincidence analysis between periodic source candidates in C6 and C7 Virgo data C.Palomba (INFN Roma) for the Virgo Collaboration.
LIGO-G Z Beating the spin-down limit on gravitational wave emission from the Crab pulsar Michael Landry LIGO Hanford Observatory for the LIGO.
Broadband Search for Continuous-Wave Gravitation Radiation with LIGO Vladimir Dergachev (University of Michigan) LIGO Scientific Collaboration APS meeting,
Searches for continuous gravitational waves with LIGO and GEO600 M. Landry for the LIGO Scientific Collaboration LIGO Hanford Observatory, Richland WA.
1 Hough transform Some Fourier basics: –Nyquist frequency: 1/2 , with  the difference between time samples. If signal is bandwidth limited below Nyquist.
1 Status of Unbiased Search for Continuous-Wave Sources Dave Chin, Vladimir Dergachev, Keith Riles (University of Michigan) LIGO Scientific Collaboration.
LIGO-G W Gregory Mendell, LIGO Hanford Observatory on behalf of the LIGO Scientific Collaboration StackSlide Summary LSC Meeting, August 2005.
Searching for pulsars using the Hough transform Badri Krishnan AEI, Golm (for the pulsar group) LSC meeting, Hanford November 2003 LIGO-G Z.
1 Status of Power-Flux * Search for Continuous-Wave Sources Dave Chin, Vladimir Dergachev, Keith Riles (University of Michigan) LIGO Scientific Collaboration.
Systematic effects in gravitational-wave data analysis
LIGO-G W Gregory Mendell, LIGO Hanford Observatory on behalf of the LIGO Scientific Collaboration Stackslide search for continuous gravitational.
1/25 Current results and future scenarios for gravitational wave’s stochastic background G. Cella – INFN sez. Pisa.
Searching for gravitational radiation from Scorpius X-1: Limits from the second LIGO science run Alberto Vecchio on behalf of the LIGO Scientific Collaboration.
LIGO-G Z Peter Shawhan, for the LIGO Scientific Collaboration APS Meeting April 25, 2006 Search for Gravitational Wave Bursts in Data from the.
Searching for Gravitational Waves with LIGO Andrés C. Rodríguez Louisiana State University on behalf of the LIGO Scientific Collaboration SACNAS
LIGO-G Z April 2006 APS meeting Igor Yakushin (LLO, Caltech) Search for Gravitational Wave Bursts in LIGO’s S5 run Igor Yakushin (LLO, Caltech)
LIGO-G D Status of Stochastic Search with LIGO Vuk Mandic on behalf of LIGO Scientific Collaboration Caltech GWDAW-10, 12/15/05.
Searching for Gravitational Waves from Binary Inspirals with LIGO Duncan Brown University of Wisconsin-Milwaukee for the LIGO Scientific Collaboration.
1 Status of Search for Compact Binary Coalescences During LIGO’s Fifth Science Run Drew Keppel 1 for the LIGO Scientific Collaboration 1 California Institute.
LIGO-G Z The Q Pipeline search for gravitational-wave bursts with LIGO Shourov K. Chatterji for the LIGO Scientific Collaboration APS Meeting.
S.Frasca on behalf of LSC-Virgo collaboration New York, June 23 rd, 2009.
LIGO-G v2 The Search For Continuous Gravitational Waves Gregory Mendell, LIGO Hanford Observatory on behalf of the LIGO Science Collaboration The.
GWDAW10, UTB, Dec , Search for inspiraling neutron star binaries using TAMA300 data Hideyuki Tagoshi on behalf of the TAMA collaboration.
1 Unbiased All-Sky Search (Michigan) [as of August 17, 2003] [ D. Chin, V. Dergachev, K. Riles ] Analysis Strategy: (Quick review) Measure power in selected.
APS meeting, Dallas 22/04/06 1 A search for gravitational wave signals from known pulsars using early data from the LIGO S5 run Matthew Pitkin on behalf.
15-18 December 2004 GWDAW-9 Annecy 1 All-Sky broad band search for continuous waves using LIGO S2 data Yousuke Itoh 1 for the LIGO Scientific Collaboration.
LIGO-G All-Sky Burst Search in the First Year of the LSC S5 Run Laura Cadonati, UMass Amherst For the LIGO Scientific Collaboration GWDAW Meeting,
Peter Shawhan The University of Maryland & The LIGO Scientific Collaboration Penn State CGWP Seminar March 27, 2007 LIGO-G Z Reaching for Gravitational.
LIGO-G Z Peter Shawhan (University of Maryland) for the LIGO Scientific Collaboration Special thanks to Michael Landry and Bruce Allen Eastern.
LIGO-G v1 Searching for Gravitational Waves from the Coalescence of High Mass Black Hole Binaries 2014 LIGO SURF Summer Seminar August 21 st, 2014.
SEARCH FOR INSPIRALING BINARIES S. V. Dhurandhar IUCAA Pune, India.
All-sky LIGO Search for Periodic Gravitational Waves in the Fourth Science Run (S4) Keith Riles University of Michigan For the LIGO Scientific Collaboration.
LIGO-G07XXXX-00-Z Beating the Crab pulsar spin-down and other upper limits: new results from the LIGO S5 known pulsar search Matthew Pitkin for the LIGO.
LIGO Document G v4 A search for gravitational waves from Cassiopeia A using LIGO S5 data Karl Wette Centre for Gravitational Physics The Australian.
LIGO-G Z The Q Pipeline search for gravitational-wave bursts with LIGO Shourov K. Chatterji for the LIGO Scientific Collaboration APS Meeting.
Broadband Search for Continuous-Wave Gravitational Radiation with LIGO Vladimir Dergachev (University of Michigan) for the LIGO scientific collaboration.
LIGO Insert Name of the Meeting KAWABE K., 2006/Apr/25 APS Meeting Dallas, W DCC: LIGO-G Z Coherent searches for periodic gravitational.
Search for gravitational waves from binary inspirals in S3 and S4 LIGO data. Thomas Cokelaer on behalf of the LIGO Scientific Collaboration.
Search for compact binary systems in LIGO data Craig Robinson On behalf of the LIGO Scientific Collaboration Cardiff University, U.K. LIGO-G
Thomas Cokelaer for the LIGO Scientific Collaboration Cardiff University, U.K. APS April Meeting, Jacksonville, FL 16 April 2007, LIGO-G Z Search.
SC03 failed results delayed FDS: parameter space searches
Xavier Siemens for the LSC University of Wisconsin -- Milwaukee
S2 Fstat paper presentation isolated
A 2 veto for Continuous Wave Searches
All-Sky broad band search for continuous waves using LIGO S2 data
S4 Pulsar Search Results from PowerFlux
Bounding the strength of gravitational radiation from Sco-X1
Searching for pulsars using the Hough transform
on behalf of the LIGO Scientific Collaboration
Sco-X1search : S2 results
Searching for gravitational-wave transients with Advanced detectors
S4 Pulsar Search Results from PowerFlux
The Q Pipeline search for gravitational-wave bursts with LIGO
Analysis of LIGO S2 data for GWs from isolated pulsars
Coherent wide parameter space searches for gravitational waves from neutron stars using LIGO S2 data Xavier Siemens, for the LIGO Scientific Collaboration.
Searching for Gravitational-Wave Bursts (GWBs) associated with Gamma-Ray Bursts (GRBs) during the LIGO S5 run Isabel Leonor University of Oregon (for the.
A.M. Sintes for the pulgroup
Matthew Pitkin on behalf of the LIGO Scientific Collaboration
Broad-band CW searches in LIGO and GEO S2 and S3 data
Stochastic background search using LIGO Livingston and ALLEGRO
Background estimation in searches for binary inspiral
Broad-band CW searches in LIGO and GEO S2 and S3 data
LIGO Scientific Collaboration, UW - Milwaukee
Hough search for continuous gravitational waves using LIGO S4 data
Broad-band CW searches in LIGO and GEO S2 and S3 data
Coherent Coincident Analysis of LIGO Burst Candidates
A Waveform Consistency Test for Binary Inspirals using LIGO data
CW Search Group Efforts – overview Michael Landry LIGO Hanford Observatory on behalf of the CW Search Group LSC Meeting June 6, 2004 Tufts University,
Gravitational radiation from known radio pulsars using LIGO data
Presentation transcript:

Broadband Search for Continuous-Wave Gravitation Radiation with LIGO Vladimir Dergachev (University of Michigan) for the LIGO/Virgo scientific collaboration April APS meeting May DCC: LIGO-G v2

Continuous gravitational waves Rotating neutron star Bump (not to scale) Circularly polarized gravitational waves Linearly polarized gravitational waves ● We know of many rotating neutron stars with frequencies from below 1 Hz to more than 700 Hz ● Gravitational radiation is expected to be emitted at twice the frequency ● Not all rotating neutron stars have to emit radio waves or X rays ● Are any convenient sources nearby ?

Challenges of search for CW gravitational waves ● Gravitational waves from spinning neutron stars are expected to be weak – need to average over long time periods ● Several parameters to search for: frequency, spindown, sky position, polarization ● Coherent methods are very sensitive, but result in enormous search space size – broadband, all sky search is impractical for large time base ● PowerFlux – place sky-dependent upper limits and detect signals by averaging power. Practical for all-sky broadband searches.

PowerFlux analysis pipeline

Choice of 1/1800 Hz SFT bins ● Small enough so that signal does not change appreciably from Doppler shifts. ● Large enough to have stationary noise over most of the spectrum. ● For a system of a neutron star of 1.5 solar masses and a companion of 1e-3 solar masses at 1 AU we would see ~90 degree phase shift at 1500 Hz over 30 minutes – not a problem with power based statistic.

Monte-Carlo run ● 8000 injections between 200Hz and 300Hz using background data collected by H1 interferometer during S3 run ● 20 injections into each 0.25 Hz band ● Uniformly distributed locations on the sky and orientation of the linearly polarized injected signal ● Power-only injection – phase was assumed to be independent and uniformly distributed for each SFT ● log 10 of injected strain values was uniformly distributed between -24 and -22.4

Upper limit versus injected strain 96.3% frequentist success rate Red points – Monte Carlo run Blue line – injected value

PowerFlux results ● PowerFlux produces a 95% CL upper limit for a particular frequency, sky position, spindown and polarization. One of three methods used in S4 all-sky search ( arXiv: = Phys. Rev. D 77 (2008) ) ● Too much data to store, let alone present – the number of sky positions alone is ~10^5 at low frequencies and grows quadratically with frequency ● The upper limit plots show maximum over spindown range, sky and all polarizations ● Performed all-sky, multiple spindown (from 0 through -5e-9 Hz/s) searches ● Data from first 8 months of S5 science run: 7 Nov 2005 through 20 July 2006

Hanford 4km, ~270 Hz, non-zero spindown (equatorial coordinates) Poor antenna pattern Good antenna pattern RA DEC 5.3e e Strain SNR

Histograms (one entry per sky point) Good antenna pattern / noise Poor antenna pattern Quoted limit

Early S5 excluded sky area %

S5 science run sensitivity

Upper limits, PRL 102, (2009) ● Red – equatorial region ● Green – intermediate regions ● Blue – polar regions All-sky Hz Worst case Best case arXiv:

Upper limits ● Our best sensitivity is at 153 Hz where we obtain upper limit of 4.2e-25 for circularly polarized sources in polar region. ● At a signal frequency of 1100 Hz we achieve sensitivity to neutron stars of equatorial ellipticity ∼ 1e−6 at distances up to 500 pc.

Hardware injected pulsar signal Simulated data RA DEC

Outlier followup ● Determine local SNR maxima, pick N highest (1000 from each of 10 sky slices) ● Apply a variation of gradient search to optimize SNR ● Look for outliers common to two interferometers: SNR>6.25 for each interferometer Difference in frequency less than 1/180 Hz Difference in spindown of less than 4e-10 Hz/s Closer than 0.14 radians (~8 degrees) on the sky ● Surviving coincidence candidates subjected to intensive followup

Multiple outliers SNR map Candidate domain map, red marks higher SNR candidates Each local maximum used as seed – then apply gradient search Clean band – maximum SNR 6 Color indicates rank RA DEC

Sample outlier - caused by violin modes (5) RA DEC SNR skymap H1 power sum L1 power sum Ecliptic poles Hz Hz Hz Hz

Signal injections guide followup MinSNR=min(SNR.H1, SNR.L1) Combined H1L1-MinSNR ● Hz ● Separate runs for H1, L1 and combined H1-L1 data ● Search in 0.3 radian disk around the injection point ● Spindown mismatch can be as large as 5e-10 Hz/s

Issues in followup ● Number of sky positions comparable with quantity of input data (especially at high frequencies) – SNR of the loudest outlier in pure noise can easily reach 6.0 ● Relatively loose initial coincidence requirements are necessary not to miss real signals ● Sky partitioning that was done to reduce memory footprint introduces spurious initial coincidences – as partition boundaries are likely to be marked as local SNR maxima. ● Parameters that are narrow for a semi-coherent search are too wide for a comfortable coherent followup

Detection search results ● No credible signal found ● We encountered 6 outliers with low SNR for which we could not identify hardware source – not unexpected in this search.

Full S5 ● Full S5 search is in preparation. ● The timebase spans 2 years – this provides improved sky localization, but requires much smaller spindown steps. ● New version of PowerFlux with 10x speedup when iterating over closely spaced spindown values and better statistics output. ● Run in progress iterating over 201 spindown values in steps of 3e-11 Hz/s.

Simulation with gaussian noise ● Slightly longer timebase than full S5 ● Software injections from 50 through 1500Hz with different spindown values ● PowerFlux scanned 0.3 radian area around the injection point assuming 0 spindown ● Vertical axis shows difference between upper limit and injected strain

Restricting to small spindowns ● Same data but only showing injections with spindown less than 1e-11 ● Upper limit is the maximum in 0.3 radian area

Parameter reconstruction Strain ● Find highest SNR coincidences using method close to one that will be used in full S5 analysis (still fine tuning the constants) ● Plots show difference between coincidence and injection Ang. separation (radians) Frequency difference (Hz)

Parameter reconstruction Strain ● Find highest SNR coincidences using method close to one that will be used in full S5 analysis (still fine tuning the constants) ● Plots show difference between coincidence and injection Frequency difference (Hz)

Conclusion ● All-sky multiple-spindown run over first 8 months of data complete, results available in arXiv: , published in PRL 102, (2009) ● No credible signal found ● Full S5 data is available, more results to follow

End of talk (supporting slides for questions follow)

Size of frequency shift in 1/1800 Hz bins due to different causes Circularly polarized Linearly polarized

PowerFlux validation ● Internal diagnostics ● Numerous software injection runs ● Analysis of hardware injected signals ● Passed code review

Noise decomposition algorithm 1. Compute log10 of each matrix entry. 2. Compute medians of each row, subtract from the matrix and add to Tmedians accumulation array. 3. Compute medians of each column, subtract from the matrix and add to Fmedians accumulation array. 4.Continue steps 2 and 3 until all medians are 0 or very small. 5.If matrix dimensions are odd always finishes in finite time with exact precision.

Residuals histograms Blue curve – analysis of hardware injected pulsar signal Red curve – analysis of fake pure noise SFTs

Are averaged powers gaussian ? (Kolmogorov-Smirnov test) Simulated data Hardware injected pulsar signal DEC RA

Sky partitioning ● PowerFlux can group templates based on a “sky marks” configuration file. ● Grouping can be done by sky location and by how strongly a given template will be affected by present line artifacts or by a signal injected into another template. ● A special group number indicates that template should not be processed. ● For example, one can mark regions around Sag A* and globular clusters and designate everything else as “do not process”. This search runs in the fraction of time of full sky analysis, yet shows most of the artifacts and issues of full run. ● During S5 analysis the sky was partitioned into equatorial band, two polar bands, two intermediate bands and a region strongly affected by instrumental artifacts.

Targeted search example (for ~270 Hz, non-zero spindown) RA DEC Area decreases with frequency Sgr A* M31 M55 NGC1 04 Need to search different sky locations due to difference between possible source spindown and spindown sampled

Interactive interface Sample loud injection

Frequency distribution

Power accumulation

Graphs

L1 S5 0-spindown run ● Blue – non Gaussian noise ● RedDiamonds – wandering line ● Magenta – 60 hz harmonics ● Green – upper limit All-sky Hz Preliminary results

S5 science run sensitivity

Partial sky (targeted) run ● Searched sky around  globular clusters M55, NGC104  galactic center Sgr A*  Andromeda M31 (control) ● Hz ● -1.01e-8 Hz/s through 1.01e-8 Hz/s in 2e-10 Hz/s steps

Search area (for ~270 Hz, non-zero spindown) RA DEC Area decreases with frequency Sgr A* M31 M55 NGC1 04 Need to search different sky locations due to difference between possible source spindown and spindown sampled

H1 Sgr A* upper limits ● Blue – non Gaussian noise ● RedDiamonds – wandering line ● Magenta – 60 hz harmonics ● Green – upper limit Preliminary results f0=132 Hz

S5 spindown-0 run ● S4 L1 upper limit ● S5 L1 upper limit (data through March) ● S5 L1 upper limit (data through July) July L1 SFTs= 3x March SFTs 3x 1.6x ● 60 Hz lines excluded ● Blue points – non-gaussian noise in July run

“S parameter” Spindown (Hz/s) Frequency Unit sky position vector Average detector velocity Average detector acceleration When S is closer to 0 susceptibility to stationary artifacts increases Earth orbit angular velocity

Doppler Skybands Skyband 0 (good – only exceptionally strong detector artifacts) Skyband 10 (worst – many detector artifacts) RA DEC

S4 run results Hanford 4km ● Blue – non Gaussian noise ● Red - wandering line suspected ● Magenta – 60 hz harmonics ● Green – 95% CL upper limit Summary curve Hanford 4km upper limits are slightly higher than the summary curve, but much cleaner in low frequency range

S4 run results Livingston 4km ● Blue – non Gaussian noise ● Red - wandering line suspected ● Magenta – 60 hz harmonics ● Green – 95% CL upper limit Summary curve Livingston 4km upper limits are slightly lower than the summary curve, but not as clean in low frequency range

S5 summary curve deviation log10(h0/summary) Excludes 60 Hz lines and non-Gaussian bands Preliminary results