Bursts without memory Ryan Shannon (and Emily Petroff)

Slides:



Advertisements
Similar presentations
Higher order waveforms in the search for gravitational waves from compact binary coalescences David McKechan In collaboration with: C. Robinson, B. Sathyaprakash,
Advertisements

Statistic for Combination of Results from Multiple Gravitational-Wave Searches Chris Pankow and Sergey Klimenko GWPAW 2011 Milwaukee, Wisconsin LIGO G v5G v5.
Aspects of Conditional Simulation and estimation of hydraulic conductivity in coastal aquifers" Luit Jan Slooten.
Burst detection efficiency  In order to interpret our observed detection rate (upper limit) we need to know our efficiency for detection by the IFO and.
Searching for pulsars using the Hough transform Badri Krishnan AEI, Golm (for the pulsar group) LSC meeting, Hanford November 2003 LIGO-G Z.
Search for the Gravitational Wave Memory effect with the Parkes Pulsar Timing Array Jingbo Wang 1,2,3, Hobbs George 3, Dick Manchester 3, Na Wang 1,4 1.
Prof. SankarReview of Random Process1 Probability Sample Space (S) –Collection of all possible outcomes of a random experiment Sample Point –Each outcome.
Brennan Ireland Rochester Institute of Technology Astrophysical Sciences and Technology December 5, 2013 LIGO: Laser Interferometer Gravitational-wave.
Capabilities of a Gravitational Wave Network Bernard F Schutz Albert Einstein Institute (Potsdam, Germany) and School of Physics and Astronomy, Cardiff.
1/25 Current results and future scenarios for gravitational wave’s stochastic background G. Cella – INFN sez. Pisa.
Gravitational lensing effects on parameters estimation in gravitational wave detection with advanced detectors Zhoujian Cao Institute of Applied Mathematics,
Searching for gravitational radiation from Scorpius X-1: Limits from the second LIGO science run Alberto Vecchio on behalf of the LIGO Scientific Collaboration.
Silvia Poggi - GW burst detection strategy in non-homogeneus networks Detection strategies for bursts in networks of non-homogeneus gravitational waves.
Precession during merger R. O’Shaughnessy (UWM) J. Healy, L. London, D. Shoemaker (Georgia Tech) Midwest Relativity Meeting, Chicago arXiv:
The Effect of Higher Harmonic Corrections on Non-Spinning Massive BH Binaries for LISA. Ed Porter (AEI) & Neil Cornish (MSU)
BY Siyandiswa Juanitta Bangani Supervisor: Dr R.Van Zyl
The ANTARES neutrino telescope is located on the bottom of the Mediterranean Sea, 40 km off the French coast. The detector is installed at a depth of 2.5.
Searching for Gravitational Waves with LIGO Andrés C. Rodríguez Louisiana State University on behalf of the LIGO Scientific Collaboration SACNAS
S.Klimenko, July 14, 2007, Amaldi7,Sydney, G Z Detection and reconstruction of burst signals with networks of gravitational wave detectors S.Klimenko,
18/01/01GEO data analysis meeting, Golm Issues in GW bursts Detection Soumya D. Mohanty AEI Outline of the talk Transient Tests (Transient=Burst) Establishing.
Sarah Burke Spolaor Jet Propulsion Laboratory, California Institute of Technology Gravitational Wave Detection with Pulsar Timing Arrays: Status and Prospects.
LIGO-G Z LIGO Observational Results I Patrick Brady University of Wisconsin-Milwaukee on behalf of LIGO Scientific Collaboration.
LIGO-G Data Analysis Techniques for LIGO Laura Cadonati, M.I.T. Trento, March 1-2, 2007.
S.Klimenko, G Z, December 2006, GWDAW11 Coherent detection and reconstruction of burst events in S5 data S.Klimenko, University of Florida for.
EE354 : Communications System I
PTA and GW detection --- Lecture K. J. Lee ( 李柯伽 ) Max-Planck Institute for Radio astronomy Aug
Joint LIGO-Virgo data analysis Inspiral and Burst Summary of the first project results Overview of the future activities M.-A. Bizouard (LAL-Orsay) on.
Science with DECIGO Naoki Seto (Kyoto U) The 1st International LISA-DECIGO.
Peter Shawhan The University of Maryland & The LIGO Scientific Collaboration Penn State CGWP Seminar March 27, 2007 LIGO-G Z Reaching for Gravitational.
Stochastic Background Data Analysis Giancarlo Cella I.N.F.N. Pisa first ENTApP - GWA joint meeting Paris, January 23rd and 24th, 2006 Institute d'Astrophysique.
Soichiro Isoyama Collaborators : Norichika Sago, Ryuichi Fujita, and Takahiro Tanaka The gravitational wave from an EMRI binary Influence of the beyond.
BREAKDOWN OF PN TEMPLATES FOR MASSIVE INSPIRALING BINARIES OBSERVED BY LIGO-I: The Necessity to Expand the Template Family Kip S. Thorne CaRT, California.
Nonlinear time series analysis Delay embedding technique –reconstructs dynamics from single variable Correlation sum –provides an estimator of fractal.
LIGO-G Z Results from LIGO Observations Stephen Fairhurst University of Wisconsin - Milwaukee 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.
PERFORMANCE OF A WAVELET-BASED RECEIVER FOR BPSK AND QPSK SIGNALS IN ADDITIVE WHITE GAUSSIAN NOISE CHANNELS Dr. Robert Barsanti, Timothy Smith, Robert.
A 2 veto for Continuous Wave Searches
P.Astone, S.D’Antonio, S.Frasca, C.Palomba
Detecting gravitational waves with the SKA: Recent results and open questions Present how we have limits on GW levels to constrain the massive black hole.
Searching for pulsars using the Hough transform
on behalf of the LIGO Scientific Collaboration
Searching for gravitational-wave transients with Advanced detectors
Methods of Detecting the Gravitational Wave Background
The Q Pipeline search for gravitational-wave bursts with LIGO
Outline Introduction Signal, random variable, random process and spectra Analog modulation Analog to digital conversion Digital transmission through baseband.
Igor Yakushin, LIGO Livingston Observatory
GW150914: The first direct detection of gravitational waves
S3 time domain known pulsar search
Gravitational Waves and Pulsar Timing
Stochastic Background
April 24th, 2006 AC Circuits PHYS 102
M.-A. Bizouard, F. Cavalier
Pulsar and Transient Science with the 12m Antenna
Targeted Searches using Q Pipeline
Weak microlensing effect and stability of pulsar time scale
Stochastic background search using LIGO Livingston and ALLEGRO
Stochastic gravitational wave and its spectral property
LISA Data Analysis & Sources
Search for gravitational waves from binary black hole mergers:
Searching for GRB-GWB coincidence during LIGO science runs
EE513 Audio Signals and Systems
Center for Gravitational Wave Physics Penn State University
J. Ellis, F. Jenet, & M. McLaughlin
Templates for M* BHs spiraling into a MSM BH
Minimum Weighted Norm Extrapolation Using Frequency Domain Blocking for Digital Audio By J. Alex Souppa April 16, 1999.
Time-Dependent Searches for Neutrino Point Sources with IceCube
Alexei Pozanenko, Pavel Minaev,
Joint bar-IFO observations
Maximum Likelihood Estimation (MLE)
Presentation transcript:

Bursts without memory Ryan Shannon (and Emily Petroff) 2011: EP, GH, RMS worked on bursts. 2012: JW and XZ (WC, GH, RMS): harnessing power of A+ Ax 2013: RMS resumed work in earnest in late March Today’s presentation: project outline (not any real results yet).

Do we expect bursts? Sources: Very nearby very massive, eccentric BH binary Exotic string-things Black holes are getting bigger by the day Exploration of the unknown

Project goals Develop algorithm to search A+,Ax time series for quadrupolar signatures of duration << observing span Place limits on amplitude and rates of short-duration GW events. Astrophysics? Better understand PPTA response to polarised GWs Gain better understanding of datasets (wide-sense stationary noise that could mimic burst)

Project Manifesto For what are we searching? “Data side” algorithm Not memory bursts Not continuous wave sources Complements other search algorithms “Data side” algorithm Measurements in units of Antenna power (vs. source side). Not a template-based approach Appeal to searches for radio transients for algorithms(Thornton Bursts)

Analogy to RF Detecting Radio Pulses A+, Ax are like voltage time series Null case: zero mean signal -> deviations from mean Want to make power measurement (phase likely a nuisance) Discriminating versus non-modelled noise Angular correlation of signal Sky localisation Time localisation

Differences with detecting radio bursts Issues: Time series are highly correlated Noise in time series is different Conclusion need to weight by inverse parameter covariance matrix C-1 This should mitigate effects of cross coupling, as long as C is a good estimate of covariance. Example: single measurement of +, x [+ x] C-1 [+ x]T

Progress so far Started developed tempo2 plugin Monte-carlo capabilities re-fitting global variables Identified tiny memory leak in doFit.C Definition of A+ and Ax Current definition based on KJ Lee Ryan redefined + and x on Celestial sphere and got consistent results Covariance of A+ and Ax Under what condtions are they covariant

A+,Ax corellation

Questions to answer Developing detection criterion Search in single polarisation? PTA polarisations Use of null stream? Ryan 2008-2013: Scramble pulsar positions and recalculate DS