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Introduction Pulsar-Black Hole Binaries Lensing Summary A Potential Astrophysical Test of Quantum Gravity Ue-Li Pen CITA November 12, 2013 U. Pen A Potential Astrophysical Test of Quantum Gravity Introduction Pulsar-Black Hole Binaries


  1. Introduction Pulsar-Black Hole Binaries Lensing Summary A Potential Astrophysical Test of Quantum Gravity Ue-Li Pen CITA November 12, 2013 U. Pen A Potential Astrophysical Test of Quantum Gravity

  2. Introduction Pulsar-Black Hole Binaries Lensing Summary Overview ◮ First pulsar orbiting black discovered in 2013! ◮ Hawking Information problem ◮ Fuzzballs ◮ Pulsar lensing U. Pen A Potential Astrophysical Test of Quantum Gravity

  3. Introduction Pulsar-Black Hole Binaries Strings Lensing Summary Magnetar PSR J1745-2900 (credit: MPIfR/Ralph Eatough) mysterious discovery in 2013, orbiting galactic center black hole. Rafikov-Lai (2006): precision GR test? U. Pen A Potential Astrophysical Test of Quantum Gravity

  4. Introduction Pulsar-Black Hole Binaries Strings Lensing Summary Black Hole Information Hawking (1974): black holes radiate: T = hc / k B r s ∼ µ K. High entropy: number of photons emitted S / k B ∼ 10 77 . Very slow: one photon of λ ∼ r s ∼ km each λ/ c ∼ ms. (1981): information loss? Evaporation is a Schwinger mechanism, does not depend on inside of black hole. U. Pen A Potential Astrophysical Test of Quantum Gravity

  5. Introduction Pulsar-Black Hole Binaries Strings Lensing Summary Dilemma ◮ No Hair: all black holes look identical after a short time (hour?) ◮ radiation only depends on outside of BH ◮ emitted radiation does not depend on formation history ◮ leads to microscopic time irreversibility of physics! ◮ breakdown of causality/unitarity? ◮ An initial pure state evolves into mixed state after a Page time (half the mass is lost). U. Pen A Potential Astrophysical Test of Quantum Gravity

  6. Introduction Pulsar-Black Hole Binaries Strings Lensing Summary Entropy solution ◮ string theory to the rescue! ◮ Strominger-Vafa (1996): counting of microstates ◮ unitarity saved? ◮ Stringy counting not possible in classical limit: what happens with Hawking’s argument? U. Pen A Potential Astrophysical Test of Quantum Gravity

  7. Introduction Pulsar-Black Hole Binaries Strings Lensing Summary Fuzzballs Samir Mathur+ (2002+): solutions to Hawking problem must be either non-local or hairy. U. Pen A Potential Astrophysical Test of Quantum Gravity

  8. Introduction Pulsar-Black Hole Binaries Strings Lensing Summary Orders of orders of magnitude � � ◮ Saha, partition function: P ( n 1 ) P ( n 0 ) = g 1 − ∆ E g 0 exp k B T ◮ probability to observe in substantially non-schwarzschild state: ◮ ∆ E ∼ mc 2 k B T ∼ 10 77 ∆ E ◮ ◮ S 1 ∼ k B log g 1 � 10 77 ◮ no-hair may be a great mis-estimate, off by 10 77 orders of magnitude! U. Pen A Potential Astrophysical Test of Quantum Gravity

  9. Introduction Pulsar-Black Hole Binaries Strings Lensing Summary Fuzzballs ◮ round black holes have minimum surface, are most unlikely! ◮ constructive stringy solutions of some eigenstates: no horizon for no entropy ◮ classical Black Holes are superpositions of “naked” microstates ◮ evades Hawking’s argument: no scharzschild background ◮ multipole deviation from GR ∼ ( r S / r ) l +2 U. Pen A Potential Astrophysical Test of Quantum Gravity

  10. Introduction Pulsar-Black Hole Binaries Strings Lensing Summary Landscape ◮ Firewall: aging of BH, destruction of observer ◮ remnants (Cornucopions) ◮ loops ◮ loss of unitarity/causality ◮ scientific test? U. Pen A Potential Astrophysical Test of Quantum Gravity

  11. Introduction Pulsar-Black Hole Binaries Lensing Summary Lens (credit: wikipedia) multiple imaging of pulsars: Boyle+ (2011+), Pen+ (2011+): interference of lensed images. Measure space-time metric to ∼ mm at Einstein radius. U. Pen A Potential Astrophysical Test of Quantum Gravity

  12. Introduction Pulsar-Black Hole Binaries Lensing Summary Lensing Prospects ◮ ideal setup: pulsar orbiting BH at ∼ 10 , 000 r S ◮ inclination similar to Einstein radius ∼ 1 o ◮ two main images form double slit interferometer (Young) near conjunction ◮ quantum lens: expect image decoherence ∼ 10 − 6 r S ∼ cm ◮ order unity effect in scintillation pattern U. Pen A Potential Astrophysical Test of Quantum Gravity

  13. Introduction Pulsar-Black Hole Binaries Lensing Summary New surveys 11 pulsar-neutron star binaries, 1 pulsar-BH binary known. New surveys (e.g. SKA, CHIME+) will increase number 10-fold. U. Pen A Potential Astrophysical Test of Quantum Gravity

  14. Introduction Pulsar-Black Hole Binaries Lensing Summary Conclusions ◮ Astrophysical test of quantum gravity? ◮ Promising future if high inclination BH-PSR binaries are discovered ◮ large cylinder telescopes (e.g. CHIME+) for searching ◮ scientific test for some scenarios of quantum gravity: coherence of pulsar scintillation U. Pen A Potential Astrophysical Test of Quantum Gravity

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