LIGO G010258-0-Z Perspectives on detector networks, and noise Lee Samuel Finn Center for Gravitational Physics and Geometry, Penn State University.

Slides:



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

LIGO-G Z Beating the spin-down limit on gravitational wave emission from the Crab pulsar Michael Landry LIGO Hanford Observatory for the LIGO.
Adaptive Hough transform for the search of periodic sources P. Astone, S. Frasca, C. Palomba Universita` di Roma “La Sapienza” and INFN Roma Talk outline.
LIGO- G Z August 19, 2004August 2004 LSC Meeting 1 Towards an Astrophysics-Based Burst ETG Tuning Keith Thorne Penn State University Relativity.
GWDAW-8 (December 17-20, 2003, Milwaukee, Wisconsin, USA) Search for burst gravitational waves with TAMA data Masaki Ando Department of Physics, University.
Modeling of Mel Frequency Features for Non Stationary Noise I.AndrianakisP.R.White Signal Processing and Control Group Institute of Sound and Vibration.
1 GWIC Gravitational Wave International Committee Report to PaNAGIC 9-Sept-03.
Overview Ground-based Interferometers Barry Barish Caltech Amaldi-6 20-June-05.
Wireless Communication Channels: Small-Scale Fading
July 13, 2007 Robert Ward, Caltech LIGO-G Z 1 Robert Ward for the LIGO Scientific Collaboration Amaldi 7 Sydney, Australia July 2007 A Radiometer.
Systematic effects in gravitational-wave data analysis
G Z April 2007 APS Meeting - DAP GGR Gravitational Wave AstronomyKeith Thorne Coincidence-based LIGO GW Burst Searches and Astrophysical Interpretation.
1/25 Current results and future scenarios for gravitational wave’s stochastic background G. Cella – INFN sez. Pisa.
S.Klimenko, G Z, December 21, 2006, GWDAW11 Coherent detection and reconstruction of burst events in S5 data S.Klimenko, University of Florida.
Chapter 21 R(x) Algorithm a) Anomaly Detection b) Matched Filter.
Silvia Poggi - GW burst detection strategy in non-homogeneus networks Detection strategies for bursts in networks of non-homogeneus gravitational waves.
A coherent null stream consistency test for gravitational wave bursts Antony Searle (ANU) in collaboration with Shourov Chatterji, Albert Lazzarini, Leo.
Coincidences in gravitational wave experiments Pia Astone 4 th Amaldi conference Perth July 8-13, 2001.
The RIDGE pipeline as a method to search for gravitational waves associated with magnetar bursts LIGO-G Z Jason Lee, Tiffany Summerscales (Andrews.
LIGO-G Z The AURIGA-LIGO Joint Burst Search L. Cadonati, G. Prodi, L. Baggio, S. Heng, W. Johnson, A. Mion, S. Poggi, A. Ortolan, F. Salemi, P.
Advanced interferometers for astronomical observations Lee Samuel Finn Center for Gravitational Wave Physics, Penn State.
Detection and estimation of abrupt changes in Gaussian random processes with unknown parameters By Sai Si Thu Min Oleg V. Chernoyarov National Research.
1SBPI 16/06/2009 Heterodyne detection with LISA for gravitational waves parameters estimation Nicolas Douillet.
LIGO-G Z Coherent Analysis of Signals from Misaligned Interferometers M. Rakhmanov, S. Klimenko Department of Physics, University of Florida,
The Analysis of Binary Inspiral Signals in LIGO Data Jun-Qi Guo Sept.25, 2007 Department of Physics and Astronomy The University of Mississippi LIGO Scientific.
Solution of the Inverse Problem for Gravitational Wave Bursts Massimo Tinto JPL/CIT LIGO Seminar, October 12, 2004 Y. Gursel & M. Tinto, Phys. Rev. D,
Physical Layer Continued. Review Discussed how to design the communication scheme depending on the physical mediums – pulling voltage up and down for.
S.Klimenko, August 2005, LSC, G Z Constraint likelihood analysis with a network of GW detectors S.Klimenko University of Florida, in collaboration.
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.
Amaldi-7 meeting, Sydney, Australia, July 8-14, 2007 LIGO-G Z All-Sky Search for Gravitational Wave Bursts during the fifth LSC Science Run Igor.
LIGO- G Z Analyzing Event Data Lee Samuel Finn Penn State University Reference: T030017, T
Space Time Codes. 2 Attenuation in Wireless Channels Path loss: Signals attenuate due to distance Shadowing loss : absorption of radio waves by scattering.
LIGO-G Z Center for Gravitational Wave Physics, Penn State 1 RayleighMonitor: A Time-Frequency Gaussianity Monitor for the DMT Lee Samuel Finn,
S.Klimenko, G Z, December 2006, GWDAW11 Coherent detection and reconstruction of burst events in S5 data S.Klimenko, University of Florida for.
S.Frasca on behalf of LSC-Virgo collaboration New York, June 23 rd, 2009.
LIGO- G Z August 17, 2005August LSC Meeting – ASIS Session 1 Recovering Hardware Injection Waveforms with Maximum Entropy Tiffany Summerscales.
S.Klimenko, G Z, December 21, 2006, GWDAW11 Coherent detection and reconstruction of burst events in S5 data S.Klimenko, University of Florida.
GWDAW10, UTB, Dec , Search for inspiraling neutron star binaries using TAMA300 data Hideyuki Tagoshi on behalf of the TAMA collaboration.
LIGO-G Z Confidence Test for Waveform Consistency of LIGO Burst Candidate Events Laura Cadonati LIGO Laboratory Massachusetts Institute of Technology.
Data Analysis Algorithm for GRB triggered Burst Search Soumya D. Mohanty Center for Gravitational Wave Astronomy University of Texas at Brownsville On.
S.Klimenko, December 2003, GWDAW Burst detection method in wavelet domain (WaveBurst) S.Klimenko, G.Mitselmakher University of Florida l Wavelets l Time-Frequency.
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.
LIGO- G Z August 17, 2005August 2005 LSC Meeting 1 Bayesian Statistics for Burst Search Results LIGO-T Keith Thorne and Sam Finn Penn State.
Comparison of filters for burst detection M.-A. Bizouard on behalf of the LAL-Orsay group GWDAW 7 th IIAS-Kyoto 2002/12/19.
LIGO- G Z March 23, 2005March LSC Meeting – ASIS Session 1 Extracting Supernova Information from a LIGO Detection Tiffany Summerscales Penn State.
G Z The LIGO gravitational wave detector consists of two observatories »LIGO Hanford Observatory – 2 interferometers (4 km long arms and 2 km.
LIGO-G ZSearle LSC Mtg Aug A Coherent Network Burst Analysis Antony Searle (ANU) in collaboration with Shourov Chatterji, Albert Lazzarini,
LIGO-G Z 23 October 2002LIGO Laboratory NSF Review1 Searching for Gravitational Wave Bursts: An Overview Sam Finn, Erik Katsavounidis and Peter.
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.
LIGO-G Z Searching for gravitational wave bursts with the new global detector network Shourov K. Chatterji INFN Sezioni di Roma / Caltech LIGO.
High Resolution Array Detector Design of Infrasound Detection and Parameter Estimation Systems Hein Haak & Läslo Evers June-September 2003.
Fletcher’s band-widening experiment (1940) Present a pure tone in the presence of a broadband noise. Present a pure tone in the presence of a broadband.
Development of a Readout Scheme for High Frequency Gravitational Waves Jared Markowitz Mentors: Rick Savage Paul Schwinberg.
24 th Pacific Coast Gravity Meeting, Santa Barbara LIGO DCC Number: G Z 1 Search for gravitational waves from inspiraling high-mass (non-spinning)
Fletcher’s band-widening experiment (1940)
ELEC4600 Radar and Navigation Engineering
A 2 veto for Continuous Wave Searches
Coherent wide parameter space searches for gravitational waves from neutron stars using LIGO S2 data Xavier Siemens, for the LIGO Scientific Collaboration.
Igor Yakushin, LIGO Livingston Observatory
L(h) = || X – A*h ||2 + hT *Ω*h
Maria Principe University of Sannio, Benevento, Italy
Targeted Searches using Q Pipeline
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:
J. Ellis, F. Jenet, & M. McLaughlin
Presentation transcript:

LIGO G Z Perspectives on detector networks, and noise Lee Samuel Finn Center for Gravitational Physics and Geometry, Penn State University

LIGO G Z 10 July 2001Fourth Amaldi Meeting, Perth Overview Coincidence, Correlation and the Effective Detector –Is the whole less or greater than the sum of the parts? In the presence of non-Gaussian noise –The effectiveness of the Normal distribution, and going beyond Cf. Finn, “Aperture synthesis for grav. wave data analysis…”, PRD 63, (2001)

LIGO G Z 10 July 2001Fourth Amaldi Meeting, Perth Coincidence … Coincidence –Detection if each detector registers wave’s passage Sensitivity limited by weakest link … –No detection, no coincidence … or gain nothing by including weaker detectors –Too high false rate leaves statistics unimproved Incident plane wave interacts with an array of detectors

LIGO G Z 10 July 2001Fourth Amaldi Meeting, Perth Coincidence … Incident plane wave interacts with an array of detectors Coincidence Sensitivity limited by weakest link … … or gain nothing by including weaker detectors But what if we shouldn’t have seen anything in a given detector? –Polarization, amplitude, signal bandwidth, etc.

LIGO G Z 10 July 2001Fourth Amaldi Meeting, Perth … and Correlation Incident plane wave interacts with array of detectors Detector array responds coherently –I.e., relative timing, polarizations, amplitudes Treat network response via likelihood techniques –I.e., optimal filter when signal known Sensitivity?

LIGO G Z 10 July 2001Fourth Amaldi Meeting, Perth Correlation For multiple detectors and no inter-detector noise correlations: f S(f) The effective detector noise spectrum: Recall optimal filter for single detector:

LIGO G Z 10 July 2001Fourth Amaldi Meeting, Perth Correlation Additional detectors always reduce effective detector noise –No more “weakest link” vis a vis sensitivity f S(f) Effective detector best envelope of component detectors –Get Virgo’s low frequency response, LIGO’s mid- frequency, GEO’s RSE high- frequency, etc. Polarization, amplitude, signal bandwidth all accommodated –Effective detector noise direction, orientation dependent

LIGO G Z 10 July 2001Fourth Amaldi Meeting, Perth What if noise non-Gaussian? What if noise non-Gaussian! –As long as stationary… Suppose know only mean, variance (i.e., psd S(f)) –What probability distribution P(x) makes least assumptions about noise character? The maximum entropy distribution: Extensible to higher- order moments –As long as highest order even

LIGO G Z 10 July 2001Fourth Amaldi Meeting, Perth Summary Coincidence –Effective only when working with detectors of comparable sensitivity in comparable bands with comparable polarization … Correlation –The whole is greater than the sum of the parts –Failure to “see” in a given detector is positive information! In the presence of non-Gaussian noise –The Normal distribution, and “optimal” filtering, is the most robust choice if only noise mean, PSD are known –Can do better (with cost!) if additional information available. Critical information is higher-order moments of distribution