1/26 Science case for AdV 1 st project review November 1 st, 2008 A.Viceré for the AdV Team‏

Slides:



Advertisements
Similar presentations
Michele Punturo INFN Perugia and EGO On behalf of the Einstein Telescope Design Study Team 1GWDAW-Rome 2010.
Advertisements

A walk through some statistic details of LSC results.
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.
Inspiraling Compact Objects: Detection Expectations
LIGO-G Z Beating the spin-down limit on gravitational wave emission from the Crab pulsar Michael Landry LIGO Hanford Observatory for the LIGO.
ICECUBE & Limits on neutrino emission from gamma-ray bursts IceCube collaboration Journal Club talk Alex Fry.
VIRGO: WHERE WE COME FROM WHERE WE ARE GOING GIOVANNI LOSURDO - INFN Firenze Advanced Virgo Project Leader for the Virgo Collaboration (and the LIGO Scientific.
A SEARCH FOR GRAVITATIONAL WAVES FROM INSPIRALING NEUTRON STARS AND BLACK HOLES Using data taken between July 2009 and October 2010, researchers from the.
1 Science Opportunities for Australia Advanced LIGO Barry Barish Director, LIGO Canberra, Australia 16-Sept-03 LIGO-G M.
LIGO Status and Advanced LIGO Plans Barry C Barish OSTP 1-Dec-04.
Gamma Ray Bursts and LIGO Emelie Harstad University of Oregon HEP Group Meeting Aug 6, 2007.
R. Frey Student Visit 1 Gravitational Waves, LIGO, and UO GW Physics LIGO
Gravitational Wave Detectors: new eyes for physics and astronomy Gabriela González Department of Physics and Astronomy Louisiana State University.
G Z April 2007 APS Meeting - DAP GGR Gravitational Wave AstronomyKeith Thorne Coincidence-based LIGO GW Burst Searches and Astrophysical Interpretation.
Dawn of GW Astrophysics: Multi-messenger Astronomy May 7, 2015Silver Spring, MD1 Jonah Kanner LIGO Lab - Caltech LIGO-G v6.
The Astrophysics of Gravitational Wave Sources Conference Summary: Ground-Based Detectors ( Hz) Kimberly New, LANL.
1/25 Current results and future scenarios for gravitational wave’s stochastic background G. Cella – INFN sez. Pisa.
LIGO-G Opening the Gravitational Wave Window Gabriela González Louisiana State University LSC spokesperson For the LIGO Scientific Collaboration.
Status of LIGO Data Analysis Gabriela González Department of Physics and Astronomy Louisiana State University for the LIGO Scientific Collaboration Dec.
Double NS: Detection Rate and Stochastic Background Tania Regimbau VIRGO/NICE.
Le Fond Gravitationnel Stochastique Tania Regimbau ARTEMIS - OCA.
Adapting matched filtering searches for compact binary inspirals in LSC detector data. Chad Hanna – For the LIGO Scientific Collaboration.
LIGO- G D Status of LIGO Stan Whitcomb ACIGA Workshop 21 April 2004.
RAS National Astronomy Meeting, Queens University, Belfast Gravitational wave astrophysics: Are we there yet? Matthew Pitkin for the LIGO Scientific Collaboration.
TAMA binary inspiral event search Hideyuki Tagoshi (Osaka Univ., Japan) 3rd TAMA symposium, ICRR, 2/6/2003.
Merger of binary neutron stars in general relativity M. Shibata (U. Tokyo) Jan 19, 2007 at U. Tokyo.
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.
Searching for Gravitational Waves with LIGO Andrés C. Rodríguez Louisiana State University on behalf of the LIGO Scientific Collaboration SACNAS
Expected Coalescence Rate of NS/NS Binaries for Ground Based Interferometers Tania Regimbau OCA/ARTEMIS on the behalf of J.A. de Freitas Pacheco, T. Regimbau,
G Z 1 Searching for gravitational waves with LIGO Gabriela González Louisiana State University On behalf of the LIGO Scientific Collaboration.
Gamma ray burst triggered searches in the S2, S3, S4 runs of LIGO Soumya D. Mohanty On behalf of the LIGO Science Collaboration.
Searches for Compact Binary Coalescences in LIGO and Virgo data Gabriela González For the LIGO Scientific Collaboration and the Virgo Collaboration APS.
LIGO-G Z LIGO Observational Results I Patrick Brady University of Wisconsin-Milwaukee on behalf of LIGO Scientific Collaboration.
Searching for gravitational waves with LIGO detectors
LIGO- G D Gravitational Wave Observations with Interferometers: Results and Prospects Stan Whitcomb for the LIGO Scientific Collaboration 2 nd.
LIGO- G D Experimental Upper Limit from LIGO on the Gravitational Waves from GRB Stan Whitcomb For the LIGO Scientific Collaboration Informal.
Rates from binaries: current status Tomasz Bulik Warsaw University.
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.
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.
G Z The LIGO gravitational wave detector consists of two observatories »LIGO Hanford Observatory – 2 interferometers (4 km long arms and 2 km.
Binary Compact Object Inspiral: Rate Expectations Vicky Kalogera with Chunglee Kim Richard O’Shaughnessy Tassos Fragkos Physics & Astronomy Dept.
GWDAW11 – Potsdam Results by the IGEC2 collaboration on 2005 data Gabriele Vedovato for the IGEC2 collaboration.
LIGO- G D Results from the LIGO Science Runs Stan Whitcomb for the LIGO Scientific Collaboration Aspen Winter Conference on Gravitational Waves.
GW – the first GW detection ! Is it a start of GW astronomy ? If “yes” then which ? «Счастлив, кто посетил сей мир в его минуты роковые !...» Ф.Тютчев.
Steering Astronomy Toward Gravitational Wave-Supernova Science Kiranjyot (Jasmine) Gill, 1 Dr. Michele Zanolin 1 With support from Marek Szczepanczyk 1.
APS Meeting April 2003 LIGO-G Z 1 Sources and Science with LIGO Data Jolien Creighton University of Wisconsin–Milwaukee On Behalf of the LIGO.
LIGO-G Z Peter Shawhan for the LSC-Virgo Burst Analysis Working Group LSC-Virgo Meeting July 23, 2007 Eyes Wide Open: Searching for Gravitational.
Gravitational Waves What are they? How can they be detected?
LIGO-G Z Results from LIGO Observations Stephen Fairhurst University of Wisconsin - Milwaukee on behalf of the LIGO Scientific Collaboration.
GRB triggered Inspiral Searches in the fifth Science Run of LIGO Alexander Dietz Cardiff University for the LIGO Scientific Collaboration LIGO-G Z.
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 Thomas Cokelaer On behalf of the LIGO Scientific Collaboration Cardiff University, U.K. LIGO-G Z.
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.
Gravitational Wave Astronomy
The Quest for Gravitational Waves: a global strategy
Brennan Hughey MIT Kavli Institute Postdoc Symposium
Detecting a Galactic Supernova with H2 or GEO
Electromagnetic Follow-ups of LIGO/Virgo Triggers
Detecting a Galactic Supernova with H2 or GEO
Searching for gravitational-wave transients with Advanced detectors
The science potential of gravitational wave observation
GW signal associated with GRBs & prospects for coincident detection
GW150914: The first direct detection of gravitational waves
Detection of gravitational waves from binary black hole mergers
Brennan Hughey for the LSC May 12th, 2008
Stochastic Background
Update on Status of LIGO
Center for Gravitational Wave Physics Penn State University
Presentation transcript:

1/26 Science case for AdV 1 st project review November 1 st, 2008 A.Viceré for the AdV Team‏

2/26 Sensitivities AdV sensitivity, BNS tuned, about 10x better at all frequencies Compared to Virgo design and Virgo+ alternatives

3/26 A partial list of sources... Binary coalescences  “Bread and butter” of the field Supernovae  Can GW be a third way to look at them? Rotating neutron stars  Possibly the cleanest signal of all Stochastic background  Key to first instants of the universe

4/26 AdV as part of a network Joint Advanced LIGO – AdV observations – Full exchange of data, joint analysis – Joint science 4 detectors to operate as a single observatory 3 having similar sensitivities Great scientific value added

5/26 Triangulation allowing to pinpoint the source A network allows to deconvolve detector response and regress signal waveform --> measure signal parameters Benefits of a network False alarm rejection thanks to coincidence Joint operation yields a longer observation time, and a better sky coverage LIGO VIRGO

6/26 Binary NS sight distance AdV: ~150 Mpc Advanced LIGO: ~170 Mpc each detector

7/26 BNS events: how frequent? Empirical models  Use observed (4) galactic binary systems coalescing on timescales comparable to Universe age  Infer # of events/Milky Way Equivalent Galaxy  Assume galactic density 0.01 Mpc -3 Population synthesis models  Use galactic luminosity to deduce star formation rate  Alternatively, use supernova events to calibrate the number of massive stars  Model binary formation and evolution to deduce # of systems coalescing in less than Hubble time

8/26 BNS: AdV predictions Empirical model rather uncertain  Small number of systems observed, little statistic Population synthesis still unclonclusive  Strong dependence on models  AdV alone sees from O(1) to O(10) events/year AdV will operate together with LIGO!  Combined sight distance may exceed 300 Mpc, if coherent analysis works as well as hoped  Network will see from O(10) to O(100) events/year

9/26 BBH sight distance AdV: ~ 700 Mpc

10/26 BBH: pop. synth. predictions Notes  Sight distance is effective: takes into account the distribution of masses in the population synthesis  Only masses < 10 M are simulated BBH population synthesis very uncertain  Merger rates vary by factors of hundreds  If model A is true, prospects of detection are dim!  However...

11/26 BBH: empirical prediction IC10 X-1  Binary system in local group (~ 700 kpc)‏  Includes a BH, m~24 M o, and a massive Wolf-Rayet star, m~ 35 M o Allows to predict a rate (Bulik et al.)‏  The WR will evolve in BH, without disrupting the binary system  The resulting system should have M chirp ~14M o  Such systems are detectable by AdV up to 1.1 Gpc...  Rate for AdV should be ~ 250 /year Rate for combined Advanced LIGO – AdV ~ 2500/year

12/26 Binaries: network advantages Detection probability increase  Advanced LIGO will have 300 Mpc coherent sight distance for BNS; corresponds to three detectors having d~170Mpc in coherent mode  AdV will boost sight distance by 10% -> rate by 30% More importantly, detection confidence  Allow checks based on coincidencing and on requiring amplitude consistency (NULL streams techniques)‏ Event reconstruction  Location of the source in the sky  Reconstruction of the polarization components  Reconstruction of the source, hence  Determination of the source distance

13/26 Core-collapse supernovae... A possible mechanism for short bursts of GW energy  Not the only one! But uncontroversial about its existence  Clear correlation between and GW emission Events relatively rare in our Galaxy  Less than 1 event/20 yrs in the local group  Sanduleak, or 1987a, was the latest in the Milky Way GW emitted

14/26.. and the advanced network  Waveforms poorly known, and signal weaker than BNS  AdV + AdLIGO will guarantee the galactic coverage  As for BNS, source parameters will be accessible  A very good timing, in conjunction with detection, could constrain mass strongly

15/26 Known pulsars: limits on h Dots: spin down limits. Beaten by AdV for about 40 known objects

16/26 Known pulsars: limits on  Dots; minimal  in the hypothesis of reaching h min More interesting at higher frequencies (smaller  values)

17/26 What about unknown NS? Distance at which the blind search would select a candidate AdV covering a fraction of the Milky Way  ~1e-7  ~1e-6  ~1e-8  ~1e-5

18/26 AdV – AdLIGO network & pulsars Coherent analysis sensitivity grows as #detectors 1/2.  Gain a factor 2  Well motivated for known sources. Blind search sensitivity grows as #detectors 1/4  Coherent analysis boost at best by a factor 40%  Use coincidences of candidates to cut the false alarm rate. Further benefits of AdV in the network  Good sensitivity at low frequencies  Stronger limits on objects like Vela and Crab

19/26 Cosmological stochastic background Frequency distribution of SNR The upper limit for a power law model can be written as here ¯ : statistical factor related to false dismissal and false alarm probability °(f) : overlap reduction function S i (f): spectrum of detector noise Correlation signal is differently distributed in frequency for LIGO pair and for LIGO-Virgo H1 - L1 V1 - H1

20/26 Limits for power law models H1 - L1H1 - V1 One year of operation of AdV – AdLIGO  Will improve over nucleosynthesis bounds by several orders  For comparison, LIGO S5 results should be just below BBN limit  AdV contribution depends on the exponent n of the stochastic background model, and is more relevant for larger n

21/26 Astrophysical backgrounds A network can locate point sources of random GW signals  Such could be objects of astrophysical interests, for instance very large black holes in active galaxies  LIGO – Virgo network, with multiple baselines, improves sensitivity by 25% at equator and by 42% at poles, over LIGO only  Source localization is improved by a factor O(10)‏

22/26 Targeting SNe; low energy 's... Boost detection confidence  Neutrino and GW expected within a few ms delay  Very tight coincidence can be required Constrain mass strongly  1ms accuracy: m < 1eV constrain

23/26 High energy 's KM3Net and IceCube will see with E up to 100's GeV  Coverage of Southern and Northern sky  Reconstruction capabilities in the 1° range  Common targets: GRB's, SGR giant flares, etc...

24/26 Targeting GRB events Swift now, Fermi (GLAST) keep looking at  rays from GRB GRB powered by accretion disks on newly formed objects Neutrino and GW expected within a few ms delay Short GRB (< 2s) potentially related to BNS, BH-NS Long GRB (>2s, average 30s) related to (classes of) SNe  Again, boost detection confidence  Provide insight in the fireball mechanism

25/26 Other messengers... Radiotelescopes  Crucial, f.i. to “lock” on pulsar signals (Automated) Optical telescopes  To alert us of interesting events  To be alerted by us of triple coincidences X-ray telescopes  Privileged eyes on the hot material falling into compact objects  For instance, in LMXB  Another eye at GRB events ..

26/26 Conclusions AdV and Advanced LIGO will do great Science!  The models anticipate several sources to be seen or strongly constrained  The AdV contribution is crucial for characterizing any event and fully extract available physics information  Source physics will be accessible: not only to check GR predictions, but to contribute to the understanding of SNe, GRB's, LMXB, NS structure... Lots of multimessenger opportunities  Collaborating with E.M. and detectors will increase the search sensitivity, or equivalently detection confidence.  Joint studies will shed light on emission mechanisms.