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Günter Sigl, Astroparticules et Cosmologie, Paris ILIAS/N5-N6 meeting, Paris, January 23-24, 2006 Supernovae as neutrino and gravitational wave sources Cosmological Backgrounds of Neutrinos, Photons, And Gravitational Waves nter Sigl eCO, Institut d’Astrophysique de Paris, CNRS et dération de Recherche Astroparticule et Cosmologie, Université Paris tp://www2.iap.fr/users/sigl/homepage.html

Supernovae as neutrino and gravitational wave sources

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Cosmological Backgrounds of Neutrinos, Photons, And Gravitational Waves. Supernovae as neutrino and gravitational wave sources. G ü nter Sigl GReCO, Institut d’Astrophysique de Paris, CNRS et Fédération de Recherche Astroparticule et Cosmologie, Université Paris 7 - PowerPoint PPT Presentation

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Page 1: Supernovae as neutrino and gravitational wave sources

Günter Sigl, Astroparticules et Cosmologie, ParisILIAS/N5-N6 meeting, Paris, January 23-24, 2006

Supernovae as neutrino and gravitational wave sources

Cosmological Backgrounds ofNeutrinos, Photons,

And Gravitational Waves

Günter SiglGReCO, Institut d’Astrophysique de Paris, CNRS etFédération de Recherche Astroparticule et Cosmologie, Université Paris 7http://www2.iap.fr/users/sigl/homepage.html

Page 2: Supernovae as neutrino and gravitational wave sources

Günter Sigl, Astroparticules et Cosmologie, ParisILIAS/N5-N6 meeting, Paris, January 23-24, 2006

Onion structure of a supernova

Convection, turbulence

Janka, Mueller

Page 3: Supernovae as neutrino and gravitational wave sources

Günter Sigl, Astroparticules et Cosmologie, ParisILIAS/N5-N6 meeting, Paris, January 23-24, 2006

Supernovae as Neutrino and Gravitational Wave Sources

Anisotropic mass motion and neutrino emission in massive star collapse leadsto gravitational wave emission. At low frequencies neutrino emission withluminosity Lν(t) and anisotropy q(t) dominates and leads todimensionless strain at distance D:

2

)()(

)()( 2

)(

0

N

thffh

tqtLtdD

Gth

f

Dt

L(t)memory h(t)

q(t)

A rotating core collapse model by Müller & Janka

Page 4: Supernovae as neutrino and gravitational wave sources

Günter Sigl, Astroparticules et Cosmologie, ParisILIAS/N5-N6 meeting, Paris, January 23-24, 2006

neutrino spectra gravitational wave spectra

Simulated individual signals

ordinary SN

≥100Msun PopIII

Individual supernovae (SN) in our Galaxy can give prominent signalsin neutrinos in Super-Kamiokande, Amanda, ICECUBE, Uno… and ingravitational waves in Virgo/EGO, LIGO…, but are RARE events.

2x10-3 Msun in gw, <q>~3%

10-8 Msun in gw, <q>~0.5%

Page 5: Supernovae as neutrino and gravitational wave sources

Günter Sigl, Astroparticules et Cosmologie, ParisILIAS/N5-N6 meeting, Paris, January 23-24, 2006

The background is then given by integration over all events

The Gaussianity of the signal is given by the “duty factor” which is proportionalto the event rate:

Where τ(f) is the time scale over which frequency f is emitted “coherently”In a given event. For us: τ(f)~1/f

Page 6: Supernovae as neutrino and gravitational wave sources

Günter Sigl, Astroparticules et Cosmologie, ParisILIAS/N5-N6 meeting, Paris, January 23-24, 2006

Ordinary SN ~ 1/sec

+ very massive PopIII starsat z ≥ 15 with rate

~ 0.2 (fIII/10-3)/sec,

where fIII = baryon fractioncycled thru PopIII stars.

future input from SWIFT…

However, backgrounds from cosmological SN may soon be detectableby gadolinium upgrade of Super-K in neutrinos and by gravitational wavedetectors such as the Big Bang Observatory (BBO).

SN rate

Page 7: Supernovae as neutrino and gravitational wave sources

Günter Sigl, Astroparticules et Cosmologie, ParisILIAS/N5-N6 meeting, Paris, January 23-24, 2006

=>diffuse neutrino spectra from ordinarySN close to current sensitivities stochastic gravitational wave backgroundAndo and Sato, astro-ph/0410061 Buonanno, Sigl, Raffelt, Janka, Mueller,

Phys.Rev.D 72 (2005) 084001

Page 8: Supernovae as neutrino and gravitational wave sources

Günter Sigl, Astroparticules et Cosmologie, ParisILIAS/N5-N6 meeting, Paris, January 23-24, 2006

Diffuse infrared background can not be explained bygalaxies alone -> may need a Pop III contribution

Dwek et al., astro-ph/0508262

Pop III fraction of baryons fIII and infraredbackground resulting from Lyα emission

Madau, Silk., astro-ph/0502304

Page 9: Supernovae as neutrino and gravitational wave sources

Günter Sigl, Astroparticules et Cosmologie, ParisILIAS/N5-N6 meeting, Paris, January 23-24, 2006

Fate of a massive star as function of progenitor mass and metallicity

low metallicity: less cooling, larger progenitor masses,less mass loss, more powerful explosions.

Heger et al., astro-ph/0211062

Page 10: Supernovae as neutrino and gravitational wave sources

Günter Sigl, Astroparticules et Cosmologie, ParisILIAS/N5-N6 meeting, Paris, January 23-24, 2006

Fate of a massive star as function of progenitor mass and metallicity

Heger et al., astro-ph/0211062

Page 11: Supernovae as neutrino and gravitational wave sources

Günter Sigl, Astroparticules et Cosmologie, ParisILIAS/N5-N6 meeting, Paris, January 23-24, 2006

Compare this with upper limits, sensitivities, and cosmological predictions

Giovannini

BBO

BBO correlated

SN and PopIII

Page 12: Supernovae as neutrino and gravitational wave sources

Günter Sigl, Astroparticules et Cosmologie, ParisILIAS/N5-N6 meeting, Paris, January 23-24, 2006

Consequence:Gravitational Wave Background from type II supernovae and PopIII stars

could mask inflationary background

Page 13: Supernovae as neutrino and gravitational wave sources

Günter Sigl, Astroparticules et Cosmologie, ParisILIAS/N5-N6 meeting, Paris, January 23-24, 2006

Conclusions

There is a deep connection between neutrino and gravitational wave emission by collapsing massive stars. Both signals have good chances to be seen by future experiments.