Black Holes and quantum fields

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Black Holes and quantum fields Aurélien Barrau Laboratory for Subatomic Physics and Cosmology CNRS/IN2P3 – University Joseph Fourier – Grenoble, France Aurelien Barrau - ISN Grenoble

Problems and hopes There is not a step but a gap when trying to go from QED to quantum gravity. Things must be seen is a totally new way. Which gendenken experiment ? (as in quantum mechanics, SR and GR) Which paradox should we consider ? Quantum black holes are probably the most promising objects ! * thermodynamics (entropy) * violation of coherence * IR/UV connection String theory ? Loop quantum gravity ? Understanding the behavior of quantum fields in the vicinity of black holes is a keypoint in theoretical physics, even at the semi-classical order. Aurelien Barrau - ISN Grenoble

A general framework to study quantum fields in curved backgrounds Building the propagator at the semi-classical order analogies between general relativistic quantum mechanics and non-relativistic quantum physics of stationary systems propagator for paths at fixed proper time and then at fixed mass (solution of the inhomogeneous KG equation) check conservation laws, the domain of validity and the action functional J. Grain & A. Barrau, Nucl. Phys. B 742 (2006) 253 «  A WKB Approach to Scalar Fields Dynamics in Curved Space-Time » J. Grain & A. Barrau, submitted to Phys. Rev. D (2006) « A general formalism for semi-classical scalar wave functions in curved backgrounds » Aurelien Barrau - ISN Grenoble

As an example : Lovelock black holes in multi-dimensional space-times The framework Let’s start with 4-dimensional General Relativity Aurelien Barrau - ISN Grenoble

From general relativity to Lovelock gravity Taylor expansion in scalar curvature Lovelock gravity : no ghost, 2nd order field equations, appears as the limit of some string theories, solves the endpoint of Hawking evaporation, etc. Gauss-Bonnet theory : 2nd order truncature D. Lovelock, J. Math. Phys. 12 (1971) 498 B. Zwiebach, Phys. Lett. B 156 (1985) 316 S. Alexeyev & M. Pomazonov, Phys. Rev. D 55 (1997) 2110 S. Alexeyev, A. Barrau, G. Boudoul, O. Khovanskaya, M. Sazhin, Class. Quantum Grav. 19 (2002) 4444 … and many others ! Aurelien Barrau - ISN Grenoble

Extra-dimensions : the ADD model Hierarchy problem in the standard model Large extra dimensions Characteristic size from a Fermi (D=11) to a fraction of millimeter (D=6) →an evaporation BH is a point object compared to the extra dimensions Standard model fields confined on the brane whereas gravitons and scalars can propagate in the bulk Arkani-Hamed, Dimopoulos, Dvali Phys. Lett. B 429, 257 (1998) Aurelien Barrau - ISN Grenoble

Black holes do evaporate Emission spectrum Aurelien Barrau - ISN Grenoble

Black holes do evaporate Emission spectrum Non-thermal part: probability to escape from the BH in the intricate metric Greybody factors Thermal part: breaking the vacuum fluctuations with tidal forces Aurelien Barrau - ISN Grenoble

Black holes do evaporate Emission spectrum Mass loss rate Aurelien Barrau - ISN Grenoble

Greybody factors: example of scalar fields on the brane (1) D-dimensional Schwarzschild metric Projection on the 4-dimensional brane → Schwarzschild with D-dimensional metric function Solving the field equation with this background metric → taking into account the symmetries Aurelien Barrau - ISN Grenoble

Greybody factors: example of scalar fields on the brane (2) Radial part of the field equations Changing the variables Schrödinger-like equation Centrifugal and gravitational potential Aurelien Barrau - ISN Grenoble

Greybody factors: example of scalar fields on the brane (3) Potential for a black hole Emission from black holes Greybody factors as a scattering problem with spherical symmetry Vacuum fluctuations breaking Diffusion on the gravitational potential Radial coordinate r Aurelien Barrau - ISN Grenoble

Greybody factors : particle with spin and scalars in the bulk Field equations in the Newman-Penrose formalism Scalar field in the bulk→ D-dimensional generalization of the Klein-Gordon equation Aurelien Barrau - ISN Grenoble

Greybody factors : computation Exact results Semi-classical results (WKB) UV region : classical particles Area within the last stable orbit Allowed classical region IR region Field equation solved near horizon (hyper geometric functions) and at infinity (Bessel functions) and junction between both regions Propagator and wave function in the system (y,t) Bohr-Sommerfeld rule Tunneling Aurelien Barrau - ISN Grenoble

Greybody factors : WKB resolution Semi-classical propagator injected within the Schrödinger equation For stationary systems : frequency Fourier transform of the propagator→ the fixed frequency propagator is the WKB wave function. First order expansion in Planck constant J. Grain, A. Barrau, Nucl. Phys. B 742 (2006) 253 Aurelien Barrau - ISN Grenoble

Greybody factors : numerical investigations (1) (mandatory in the intermediate region) Field equations solved numerically from the BH horizon to space infinity. The boundary conditions are : non outgoing mode at the horizon. For r large enough, the asymptotic solutions at infinity are fitted to the numerical solution with the modes amplitudes as free coefficients. Aurelien Barrau - ISN Grenoble

Greybody factors : numerical investigations (2) For a given energy, the tunnel probability is determined for each multipolar order: The optical theorem gives the emission/absorption cross section Numerical errors under control Aurelien Barrau - ISN Grenoble

First consequence : Gauss-Bonnet black holes (1) Scalars on the brane Fermions Scalars in the bulk Jauge Bosons J. Grain, A. Barrau & P. Kanti, Phys. Rev. D 72 (2005) 104016 Aurelien Barrau - ISN Grenoble

Gauss-Bonnet black holes (2) Aurelien Barrau - ISN Grenoble

Gauss-Bonnet black holes (3) : 4-dimensions and dilatonic coupling Alexeyev & Pomazonov, Phys. Rev. D 55 (1997) 2110 Alexeyev, Grav. Cosm. 3 (1997) 161 S. Alexeyev, A. Barrau, G. Boudoul, O. Khovanskaya, M. Sazhin, Class. Quantum Grav. 19 (2002) 4444 Hawking law Aurelien Barrau - ISN Grenoble

Gauss-Bonnet black holes (4) : Universe makers ? Adapted from Frolov, Markov, Mukhanov, Phys. Lett. B 216 (1989) 272 Lee Smolin (the father of LQG) idea of cosmic natural selection needs a Universe inside a black hole. This assumes a finite value of the Riemann invariant. Lovelock gravity does not support this hypothesis (as implicitly demonstrated by Alexeyev et al.). A. Barrau, gr-qc/0612045 Aurelien Barrau - ISN Grenoble

Schwarzschild-de-Sitter black holes (1) 2 event horizons , 2 temperatures Metric function h(r) Aurelien Barrau - ISN Grenoble

Schwarzschild-de-Sitter black holes (2) The 2nd horizon leads to an infrared divergence Ultra-soft quanta due to the IR behavior P. Kanti, J. Grain & A. Barrau, Phys. Rev. D 71 (2005) 104002 Aurelien Barrau - ISN Grenoble

Analytical checks for SdS black holes Aurelien Barrau - ISN Grenoble

Anti-de-Sitter spaces (1) Metric function Stationary states with a discrete normal frequency spectrum. Tortoise coordinate Aurelien Barrau - ISN Grenoble

Back to Schwarzschild black holes : new quantum bound states J. Grain & A. Barrau, submitted to Phys. Lett (2007) For massive particles Quasi-bound states : bandwidth and characteristic lifetime can be computed at the WKB order Exist even at the monopolar order : no classical equivalent → spherical halo of scalar particles around the black hole. Potential well due to the gravitational binding energy Radial coordinate Aurelien Barrau - ISN Grenoble

Schwarzschild-Anti-de-Sitter black holes The hierarchy plays a fundamental role in the multipolar dependence of the potential well. Singular transition from SAdS to AdS ! resonances Tortoise coordinate Aurelien Barrau - ISN Grenoble

EXPERIMENTAL INVESTIGATIONS BH @ the LHC if the Planck scale ~ TeV ! Geometric cross section Estimate of the number of produced black holes Reconstruction of the dimensionality Banks, Fischler hep-th/9906038 Giddings, Thomas Phys. Rev. D 65, 056010 (2002) Dimopoulos, Landsberg Phys. Rev. Lett 87, 161602 (2001) Parler de Landsberg et giddings Donner leur resultats:section efficace nombre de BH produits evaporation, l’expliquer, peut etre ils ne le savent pas  loi de hawking donne la dimension prenne en compte une evaporation instantanée Aurelien Barrau - ISN Grenoble

Black holes at the LHC (2) Taking everything into account : it works ! The statistical analysis allows to reconstruct both the dimensionality of space-time and the Gauss-Bonnet coupling constant. Valeur differentes du couple D et lambda Reconstruction des spectres mesure par ATLAS Analyse de chi2 avec les modeles theoriques Exemple de D=8 et lambda=5 marche bien, meme resultat dans les autres cas A. Barrau, J. Grain, S. Alexeyev Phys. Lett. B 584 (2004) 114 Now we should consider Kerr-Gauss-Bonnet black holes : S. Alexeyev, N. Popov, A. Barrau, J. Grain, in prep. for Phys. Rev. Lett (2007) Also : Particle physics (light SUSY particles, Higgs, etc.) with BH as resonances Aurelien Barrau - ISN Grenoble

What about the interstellar medium ? Black holes formed in the Galaxy should evaporate and contribute to the cosmic-ray background - Compatible with CR flux - Compatible with entropy in the early universe - Compatible with dark matter ATLAS pourra mesurer Lambda et D Prendre mieux en compte la fin de vie Faire attention au chi2 A. Barrau, J. Grain, C. Féron, Astrophys. J. 630 (2005) 1015 Aurelien Barrau - ISN Grenoble

How to look for them ? Let’s consider their cosmic-ray emission ! PBHs (Primordial Black Holes) could have formed in the early Universe ! Direct formation by density fluctuations Softening of the equation if state Inflation fluctuations Phase transitions Topological defects collisions Critical phenomena etc… How to look for them ? Let’s consider their cosmic-ray emission ! Aurelien Barrau - ISN Grenoble

Antiproton individual emission Antiprotons are rare : good S/N M2Q2 Jet energy MQ Antiproton energy Aurelien Barrau - ISN Grenoble

Cumulative source total flux (2) (4) (3) (1)  (1) (2)  (3)  (4)  Antiprotons kinetic energy (GeV) The horizon size after inflation is also taken into account A possible QCD halo around the BH is also considered Aurelien Barrau - ISN Grenoble

Now, let the antiprotons propagate in the Milky way… Drawing by D. Maurin “Annecy” model Maurin, Taillet, Donato, Salati, Barrau, Boudoul, review article for “Research Signapost” (2002) [astro-ph/0212111] Aurelien Barrau - ISN Grenoble

Secondary antiprotons flux Experimental data Antiprotons flux p-p component p-He component He-p component He-He component F.Donato, D. Maurin, P. Salati, A. Barrau, G. Boudoul, R.Taillet, Astrophys. J. (2001) 536, 172 Aurelien Barrau - ISN Grenoble

Spectrum and limit on the PBH density + tertiaries A. Barrau, et al., Astronom. Astrophys., 388, 767 (2002) Aurelien Barrau - ISN Grenoble

Gamma-ray new upper limit Taking into account the expected background from (Pavlidou & fields, ApJ 575, L5-8 (2002)): - galaxies - quasars The EGRET gamma-ray flux at 100 MeV can be converted into (after integration over redshift, evolution and absorption) : Omega_PBH < 3.3 E –9 , improving by a factor 3 the Page & MacGibbon upper limit. This limit is nearly the same as with antiprotons but it relies on very different physics and assumptions. Barrau & Boudoul, IRCR 2003 proc., [asto-ph/0304528] Aurelien Barrau - ISN Grenoble

COSMOLOGICAL CONSEQUENCES WMAP 3-years Unlike the CMB or the large scale structures, PBH give information on small scale PRIMORDIAL BLACK HOLES ARE A UNIQUE COSMOLOGICAL PROBE Aurelien Barrau - ISN Grenoble

Density fluctuations in the early Universe constrained by PBHs (mass fraction of the Universe going into black holes) Using Starobinsky model for the bump Gravitational constraint Antiprotons constraint Mpeak (g) Barrau, Blais, Boudoul, Polarski, Phys. Lett. B, 551, 218 (2003) Aurelien Barrau - ISN Grenoble

The old problem of gravitinos in cosmology… Photons : gamma-gamma pair creation pair creation on nuclei scattering compton inverse-Compton D + gamma n+p T + gamma n+D T + gamma p+n+n 3He + gamma p+D 4He + gamma p+T 4He + gamma n+3He 4He + gamma p+n+D …… The reheating temperature of the Universe cannot be too high Aurelien Barrau - ISN Grenoble

Constraints on SUGRA Lower limit on the reheating temperature as a function of the 100 MeV antideuteron flux Barrau & Ponthieu, Phys. Rev. D 69 (2004) 105021 Aurelien Barrau - ISN Grenoble

Gravitinos from PBHs Khlopov & Barrau, Class. Quantum Grav. 23 (2006) 1875 n<1.18 : the most stringent limit at small scale Positive running excluded The only constrain of very small scale fluctuations Aurelien Barrau - ISN Grenoble

Dark Matter In the BSI framework, PBHs can be reconsidered as CDM candidates In two different scenarios A. Barrau, D.Blais, G.Boudoul , D. Polarski Ann. Phys. 13, 115 (2004) If MRH is very large (greater than 1015 g) , PBHs become good candidates Pour M H,e =10 -15 g p  6.5 10 -4 Experimental investigations possible above 1022 g by detection of gravitational waves If MRH is small (smaller than 109 g) , stable relics become good candidates Very large parameter space (of masses) for PBH/relics dark matter. But fine tuning of the « jump » required (unnatural ? Caution in cosmology !) Aurelien Barrau - ISN Grenoble

A new hope for detection ? Antideuterons ! Secondary noise very small (kinematics) Relativistic coalescence model in the MC PBH evaporation Improvement in sensitivity of 1-2 orders of magnitude Window for detection Background A. Barrau et al. Astronom. Astrophys. 398, 403 (2003) Aurelien Barrau - ISN Grenoble

The AMS experiment AMS-01: test fly in 1998 Antiproton sensitivity Antideuteron sensitivity Gamma-ray sensitivity AMS-01: test fly in 1998 In 2010... AMS-02 on the ISS! Aurelien Barrau - ISN Grenoble

Microscopic black holes oblige us to face unification Back to the theory Evaporating black holes encode an invaluable information on the underlying fundamental theories and on the intrinsic structure of spacetime. Primordial black holes (whether they do exist or not) allow otherwise unreachable limits on the early universe. Quantum effects near an event horizon exhibit an exceptionally rich physics. Microscopic black holes oblige us to face unification Aurelien Barrau - ISN Grenoble

Unification and diversity : gauge fields and symmetry breaking Toward a new paradigm ? Unification and diversity : gauge fields and symmetry breaking BUT… the story (of Newton and Maxwell) is changing : the number of parameters is inflating (maybe even more than the Universe did !!!) with supersymmetry and string theory. The multiverse scenario (either through black holes or through chaotic inflation) is tantalizing … if anthropic devils (ID) do not take this opportunity to spoil the foundation of free thinking. « Men are within the Universe. They are neither its reason to be –as Christian anthropocentrism has told us during centuries– nor its final cause –as contemporary atheistic anthropolatry tries, even more naïvely, to teach us today. » M. Yourcenar (from the french Academy) about the greak philosopher Empedocle d’Agrigente Aurelien Barrau - ISN Grenoble

Big black holes are fascinating A conclusion ? Big black holes are fascinating But… small black holes are much more fascinating! Aurelien Barrau - ISN Grenoble