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DARK MATTER PROBES OF SUPERMASSIVE BLACK HOLE S. HotSci 23 July 2014. Joe Silk (IAP, JHU). SMBH binaries in quasars may be common a t parsec scales, from Balmer line offsets. Liu e al 2013. Benson 2014. Stuck at the final parsec…. Mpc. Inoue + 2013.
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DARK MATTER PROBES OF SUPERMASSIVE BLACK HOLES HotSci 23 July 2014 Joe Silk (IAP, JHU)
SMBH binaries in quasars may be common at parsec scales, from Balmerline offsets Liu e al 2013
Benson 2014 Stuck at the final parsec… Mpc
Inoue + 2013 Intermediate mass BH 103-106Msun Two baryon problems: Too big to fail dwarfs & low baryon fraction in massive galaxies IMBH EXPEL BARYONS
Duc + 2013 Dubois+ 2013 Baryon fraction fraction supernovae IMBH predicted hosts, not observed Peirani + 2012 Boylan-Kirchin et al. 2011
<v> mx Density profile Plateau: nx(r)<sv> tBH ~ 1 Gondolo + JS 1999, Gnedin & Primack 2004, Sadeghian, Ferrer + Will 2013
Does cusp survive? MAYBE! Vasiliev & Zelnikov 2008 tr (GC,M31)~3Gyr ~tr ~3tr but SMBH at GC grows over 1 Gyr & tr (M87 SMBH)~105Gyr!
Kozai mechanism drives resonant infall of DM in eccentric orbits………operates for binary black hole Naoz and Silk 2014
Naoz and Silk 2014 Dark matter torus forms
supermassive black hole at Galactic Center HESS J1745-290 prediction for CTA: superexponential signature of TeV DM annihilations 30-300 GeV the near future Belikov & JS 2013 Vaiana + 2014
NEARBY AGN M87 is an attractive target Distance 2000 x GC but MBH 1000 x SagA* Flux ~ nx2<sv> (2rp)3 ~ MBH3/<sv> for low <sv> nx(rp)<sv> tBH ~ 1 Dynamical heating of spike ~ 1014yrvs 109yr(GC)
relativistic jets emanate from ergosphere, so high energy e,p collide with DM spike particles! Gomez et al 2013 Gorchtein et al 2010 M87 CenA
EXTRAGALACTIC GAMMA RAY BACKGROUND EXTRACALACTIC DIFFUSE g RAY BACKGROUND There is room for an exotic component from dark matter
0.1 TeV 1 TeV Annihilations In dark matter spikes around supermassive black holes 10 TeV NFW Belikov & Silk 2013
BLACK HOLES THE ULTIMATE PARTICLE ACCELERATOR: dark matter cusp around black hole particle horizon maximum 4.5 m Schwarzschild
NEAR KERR BLACK HOLES ergosphere Penrose process
Rotating black hole can feed Penrose effect via DM particle collisions Kerr black hole no maximum for extremal Kerr! near event-horizon particle collisions of KK particles: excitations Banados, West, JS 2009 particle horizon rS=2GM/c2 Highly controversial…but the dust hasn’t settled yet! Arina, Bringmann, Vollmann, JS 2014
Black hole shadow Event Horizon Telescope Simulated image at 1mm of M87 or SagA* black hole Resolve horizon scale GM/c2 at ~5 marcsec M87 distance 2000 x GC but MBH 1000 x SagA* Huang + 2007