Black holes as particle detectors Vtor Cardoso (CENTRA/ Tcn ico - - PowerPoint PPT Presentation

black holes as particle detectors
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Black holes as particle detectors Vtor Cardoso (CENTRA/ Tcn ico - - PowerPoint PPT Presentation

Black holes as particle detectors Vtor Cardoso (CENTRA/ Tcn ico & Perim eter) ... Quy Nhon, Vietnam supports this project b la ckh oles.ist .u t l.p t Cardoso, Gualtieri, Herdeiro & Sperhake Exploring New Physics


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Black holes as particle detectors

supports this project

 Vítor Cardoso 

(CENTRA/ Técn ico & Perim eter) ...

Quy Nhon, Vietnam

b la ckh oles.ist .u t l.p t

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Cardoso, Gualtieri, Herdeiro & Sperhake Exploring New Physics Frontiers Through Num erical Relativity,

  • Liv. Rev. Relativity; arXiv:1409.0014

Brito, Cardoso & Pani, Superradiance, Springer-Verlag (2015); arXiv:1501.06570 Berti et al, Testing General Relativity w ith Present and Future Observations, arXiV:1501.07274

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Black holes exist

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Black holes exist

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Black holes have no hair

One star made of matter and other of antimatter, produce identical BHs. A stationary BH is characterized by only three quantities: m ass, spin and electric charge

Note: B & L num bers are also non-conserved in black hole physics

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Why study dynamics

Gravitational-wave detection, GW astrophysics Fundamental physics High-energy physics Particle physics

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Inspiral Merger Ringdow n

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“Can one hear the shape of a drum?”

Mark Kac, American Mathematical Monthly, 1966

  • H. Weyl 1911

Gordon, Webb & Wolpert, Inventiones Mathem aticae 1992

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Can one hear the shape of a BH?

Berti, Cardoso & Will PRD73, 064030(2005) Kam aretsos et al PRD85, 024018 (2012)

j=0 0.8 0.98 DL=3Gpc, rd=3%

Berti et al PRD76, 104044(2007)

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Stability, spectroscopy?

Cosmic Censorship?

  • New dynamical, long-term stable solutions?

Universal limit on maximum luminosity c^ 5/ G (10^ 59 erg/ sec)

Barrow & Gibbons MNRAS 446, 3874 (2015)

Critical behavior, etc

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Sperhake et al PRL 2009, 2013

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Sperhake et al PRL 2009, 2013

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More than 25% (35%) CM energy radiated for v=0.75 c (0.92c)! Final BH rapidly spinning

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Massive scalars

Interesting as effective description; proxy for more complex interactions Arise as interesting extensions of GR* (BD or generic ST theories; f(R)) DM candidates (boson and soliton stars, Axiverse scenarios - m oduli and coupling constant in string theory, Peccei-Quinn m echanism in QCD)

Plan

Energy extraction, bound states; evading no-hair theorems Accretion and gravitational-wave emission Bounds on ultra-light fields

* Poorly constrained for m assive fields

Strong field and fundamental fields

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Ribner, J. Acous. Soc. Am er.29 (1957)

Friction & superradiance

Tam m & Frank, Doklady AN SSSR 14 (1937)

  • G. H. Darw in, Philos. Trans.
  • R. Soc. London 171 (1880)

Pierce (& Kom pfner), Bell Lab Series (1947) Ginzburg, anomalous Doppler year

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Zel’dovich, Pis’ma Zh. Eksp. Teor. Fiz. 14 (1971)

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Black holes and superradiance

Friction built-in through one-way membrane (horizon)

Zel’dovich, Pis’ma Zh. Eksp. Teor. Fiz. 14 (1971), Brito et al, arXiv:1501.06570

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Brito, Cardoso & Pani , arXiv:1501.06570

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(Rotational) superradiance in the lab?

Need absorbing surface, characterized by com plex acoustic im pedance Z

Cardoso, Coutant , Richartz & Weinfurtner, in progress

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Am plification < 100%...fundam ental bound on superradiance?

Baibhav, Cardoso and Em paran, in progress

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Binaries? Backreaction? Superradiance in stars? Direct observational effects?

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Rosa, arXiv:1501.07605

VC1

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Slide 22 VC1

Vitor Cardoso, 10/08/2015

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Superradiant instabilities

Can construct unstable states by forcing wave to bounce back

Zel’dovich, Pis’ma Zh. Eksp. Teor. Fiz. 14 (1971); Cardoso & Dias, PRD70 (2004) ; Brito, Cardoso & Pani, arXiv:1501.06570

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Massive “states” around Kerr are linearly unstable Dam our et al ‘76; Detw eiler PRD; Cardoso & Yoshida JHEP0507 (2005) 009 Dolan PRD76 (2007) 084001; Witek et al, PRD87 (2013) 4, 043513; Cardoso, Carucci, Pani, Sotiriou PRL111 (2013) 111101 See review s Brito et al arXiv:1501.06570 and Yoshino and Kodam a arXiv:1505:00714

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Okaw a et al PRD89, 104032 (2014)

Final state I: almost-hairy BHs

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Final state II: hairy black holes?

Herdeiro & Radu, PRL112, 221101 (2014)

Are themselves unstable in parts of the parameter space

Brito, Cardoso & Pani, arXiv:1501.06570

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End-state of linear instability? Gravitational-wave emission and accretion? Are hairy solutions formed?

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Accretion: Gravitational-wave emission:

Yoshino & Kodam a PTEP 2014 (043E02); Brito et al CQG32 (2015) 13, 134001

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Brito, Cardoso, Pani arXiv:1411.0686

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Bounding the boson mass

Pani et al PRL109, 131102 (2012) Bound on photon mass is model-dependent: details of accretion disks or intergalactic matter are important...but gravitons interact very weakly! Brito et al PRD88:023514 (2013); Review of Particle Physics 2014

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Yoshino and Kodam a PTEP 2015 6, 061E01

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Arvanitaki, Baryakhtar, Huang arXiv:1411.2263 (rates m ay be overly optim istic)

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Strong field gravity is a fascinating topic Fundamental fields, either in form of minimally coupled fields or under curvature couplings have a very rich and unexplored phenomenology: condensates outside BHs and compact stars act as gravitational-wave lighthouses, but can also act as dark matter. Superradiant instabilities can provide strong constraints on masses of ultra-light bosons, turning black holes into effective particle detectors.

 

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Thank you