Wormholes Untangle a Black Hole Paradox
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Stephen Hawking: 'There Are No Black Holes' Notion of an 'Event Horizon', from Which Nothing Can Escape, Is Incompatible with Quantum Theory, Physicist Claims
NATURE | NEWS Stephen Hawking: 'There are no black holes' Notion of an 'event horizon', from which nothing can escape, is incompatible with quantum theory, physicist claims. Zeeya Merali 24 January 2014 Artist's impression VICTOR HABBICK VISIONS/SPL/Getty The defining characteristic of a black hole may have to give, if the two pillars of modern physics — general relativity and quantum theory — are both correct. Most physicists foolhardy enough to write a paper claiming that “there are no black holes” — at least not in the sense we usually imagine — would probably be dismissed as cranks. But when the call to redefine these cosmic crunchers comes from Stephen Hawking, it’s worth taking notice. In a paper posted online, the physicist, based at the University of Cambridge, UK, and one of the creators of modern black-hole theory, does away with the notion of an event horizon, the invisible boundary thought to shroud every black hole, beyond which nothing, not even light, can escape. In its stead, Hawking’s radical proposal is a much more benign “apparent horizon”, “There is no escape from which only temporarily holds matter and energy prisoner before eventually a black hole in classical releasing them, albeit in a more garbled form. theory, but quantum theory enables energy “There is no escape from a black hole in classical theory,” Hawking told Nature. Peter van den Berg/Photoshot and information to Quantum theory, however, “enables energy and information to escape from a escape.” black hole”. A full explanation of the process, the physicist admits, would require a theory that successfully merges gravity with the other fundamental forces of nature. -
It from Qubit Simons Collaboration on Quantum Fields, Gravity, and Information
It from Qubit Simons Collaboration on Quantum Fields, Gravity, and Information GOALS Developments over the past ten years have shown that major advances in our understanding of quantum gravity, quantum field theory, and other aspects of fundamental physics can be achieved by bringing to bear insights and techniques from quantum information theory. Nonetheless, fundamental physics and quantum information theory remain distinct disciplines and communities, separated by significant barriers to communication and collaboration. Funded by a grant from the Simons Foundation, It from Qubit is a large-scale effort by some of the leading researchers in both communities to foster communication, education, and collaboration between them, thereby advancing both fields and ultimately solving some of the deepest problems in physics. The overarching scientific questions motivating the Collaboration include: ● Does spacetime emerge from entanglement? ● Do black holes have interiors? Does the universe exist outside our horizon? ● What is the information-theoretic structure of quantum field theories? ● Can quantum computers simulate all physical phenomena? ● How does quantum information flow in time? MEMBERSHIP It from Qubit is led by 16 Principal Investigators from 15 institutions in 6 countries: ● Patrick Hayden, Director (Stanford University) ● Matthew Headrick, Deputy Director (Brandeis University) ● Scott Aaronson (MIT) ● Dorit Aharonov (Hebrew University) ● Vijay Balasubramanian (University of Pennsylvania) ● Horacio Casini (Bariloche -
Black Hole Weather Forcasting
NTU Physics Department Chih-Hung Wu 吳智弘 I. Spacetime Locality and ER=EPR Conjecture II. Construction of the Counter-example III. Debate with Professor J. Maldacena J. Maldacena and L.Susskind, “Cool horizon for entangled black holes”, Fortsch. Phys. 61 (2013) 781-811 arXiv:1306.0533 Pisin Chen, Chih-Hung Wu, Dong-hanYeom. ”Broken bridges: A counter-example of the ER=EPR conjecture”, arXiv:1608.08695, Aug 30, 2016 Locality(Impossibility of superluminal signal) 1.Quantum Theory-EPR entanglement 2.General Relativity-ER bridge Violation of Locality?---NO! ER bridge should remain un-traversable even in the quantum theory. En /2 e nLR m n In AdS/CFT framework, an eternal AdS- Schwarzschild BH and the Penrose diagram: En /2 e nLR m n Maximally entangled J. Maldacena, “Eternal black hole in AdS” JHEP 0304 (2003) 021 ,arXiv:0106112 Consider such a scenario: A large number of particles, entangled into separate Bell pairs, and separate them when we collapse each side to form two distant black holes, the two black holes will be entangled. Now they make a conjecture that they will also be connected by an Einstein-Rosen bridge. ER=EPR Known: EREPR Conjecture: EPRER How to realize in the usual Hawking radiation scenario? Second black hole= early half of HR. Step 1: Generate an entangled system Step 2: Formation of the ER bridge Step 3: Collapsing of the bubble Step 4: Evaporation of the black hole Step 5: Communication via ER bridge Assumption: GR with N massless scalar fields 11N S gd4 x ()()() 2 U f 2 i 22i1 The potential has two minima: (AdS space) Background (false vacuum) True vacuum 0 Prepared in advance (e.g. -
Finite-Cutoff JT Gravity and Self-Avoiding Loops Arxiv
Finite-cutoff JT gravity and self-avoiding loops Douglas Stanford and Zhenbin Yang Stanford Institute for Theoretical Physics, Stanford University, Stanford, CA 94305 Abstract We study quantum JT gravity at finite cutoff using a mapping to the statistical mechanics of a self-avoiding loop in hyperbolic space, with positive pressure and fixed length. The semiclassical limit (small GN ) corresponds to large pressure, and we solve the problem in that limit in three overlapping regimes that apply for different loop sizes. For intermediate loop sizes, a semiclassical effective description is valid, but for very large or very small loops, fluctuations dominate. For large loops, this quantum regime is controlled by the Schwarzian theory. For small loops, the effective description fails altogether, but the problem is controlled using a conjecture from the theory of self-avoiding walks. arXiv:2004.08005v1 [hep-th] 17 Apr 2020 Contents 1 Introduction 2 2 Brief review of JT gravity 4 3 JT gravity and the self-avoiding loop measure 5 3.1 Flat space JT gravity . .5 3.2 Ordinary (hyperbolic) JT gravity . .8 3.3 The small β limit . .8 4 The flat space regime 9 5 The intermediate regime 11 5.1 Classical computations . 11 5.2 One-loop computations . 13 6 The Schwarzian regime 18 7 Discussion 19 7.1 A free particle analogy . 20 7.2 JT gravity as an effective description of JT gravity . 21 A Deriving the density of states from the RGJ formula 23 B Large argument asymptotics of the RGJ formula 24 C Monte Carlo estimation of c2 25 D CGHS model and flat space JT 26 E Large unpressurized loops 27 1 푝 2/3 -2 푝 푝 = ℓ β large pressure effective theory Schwarzian theory flat-space (RGJ) theory 4/3 β = ℓ -3/2 = ℓ4β3/2 푝 = β 푝 푝 = ℓ-2 0 0 0 β 0 β Figure 1: The three approximations used in this paper are valid well inside the respective shaded regions. -
A Hole in the Black Hole
Open Journal of Mathematics and Physics | Volume 2, Article 78, 2020 | ISSN: 2674-5747 https://doi.org/10.31219/osf.io/js7rf | published: 7 Feb 2020 | https://ojmp.wordpress.com DA [microresearch] Diamond Open Access A hole in the black hole Open Physics Collaboration∗† April 19, 2020 Abstract Supposedly, matter falls inside the black hole whenever it reaches its event horizon. The Planck scale, however, imposes a limit on how much matter can occupy the center of a black hole. It is shown here that the density of matter exceeds Planck density in the singularity, and as a result, spacetime tears apart. After the black hole is formed, matter flows from its center to its border due to a topological force, namely, the increase on the tear of spacetime due to its limit until it reaches back to the event horizon, generating the firewall phenomenon. We conclude that there is no spacetime inside black holes. We propose a solution to the black hole information paradox. keywords: black hole information paradox, singularity, firewall, entropy, topology, quantum gravity Introduction 1. Black holes are controversial astronomical objects [1] exhibiting such a strong gravitational field that nothing–not even light–can escape from inside it [2]. ∗All authors with their affiliations appear at the end of this paper. †Corresponding author: [email protected] | Join the Open Physics Collaboration 1 2. A black hole is formed when the density of matter exceeds the amount supported by spacetime. 3. It is believed that at or near the event horizon, there are high-energy quanta, known as the black hole firewall [3]. -
Diagnosing Chaos Using Four-Point Functions in Two-Dimensional Conformal Field Theory
Diagnosing Chaos Using Four-Point Functions in Two-Dimensional Conformal Field Theory The MIT Faculty has made this article openly available. Please share how this access benefits you. Your story matters. Citation Roberts, Daniel A., and Douglas Stanford. "Diagnosing Chaos Using Four-Point Functions in Two-Dimensional Conformal Field Theory." Phys. Rev. Lett. 115, 131603 (September 2015). © 2015 American Physical Society As Published http://dx.doi.org/10.1103/PhysRevLett.115.131603 Publisher American Physical Society Version Final published version Citable link http://hdl.handle.net/1721.1/98897 Terms of Use Article is made available in accordance with the publisher's policy and may be subject to US copyright law. Please refer to the publisher's site for terms of use. week ending PRL 115, 131603 (2015) PHYSICAL REVIEW LETTERS 25 SEPTEMBER 2015 Diagnosing Chaos Using Four-Point Functions in Two-Dimensional Conformal Field Theory Daniel A. Roberts* Center for Theoretical Physics and Department of Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA † Douglas Stanford School of Natural Sciences, Institute for Advanced Study, Princeton, New Jersey 08540, USA (Received 10 March 2015; revised manuscript received 14 May 2015; published 22 September 2015) We study chaotic dynamics in two-dimensional conformal field theory through out-of-time-order thermal correlators of the form hWðtÞVWðtÞVi. We reproduce holographic calculations similar to those of Shenker and Stanford, by studying the large c Virasoro identity conformal block. The contribution of this block to the above correlation function begins to decrease exponentially after a delay of ∼t − β=2π β2E E t β=2π c E ;E à ð Þ log w v, where à is the fast scrambling time ð Þ log and w v are the energy scales of the W;V operators. -
Naked Firewalls Phys
Naked Firewalls Phys. Rev. Lett. 116, 161304 (2016) Pisin Chen, Yen Chin Ong, Don N. Page, Misao Sasaki, and Dong-han Yeom 2016 May 19 Introduction In the firewall proposal, it is assumed that the firewall lies near the event horizon and should not be observable except by infalling observers, who are presumably terminated at the firewall. However, if the firewall is located near where the horizon would have been, based on the spacetime evolution up to that time, later quantum fluctuations of the Hawking emission rate can cause the `teleological' event horizon to have migrated to the inside of the firewall location, rendering the firewall naked. In principle, the firewall can be arbitrarily far outside the horizon. This casts doubt about the notion that a firewall is the `most conservative' solution to the information loss paradox. The AMPS Argument Almheiri, Marolf, Polchinski and Sully (AMPS) argued that local quantum field theory, unitarity, and no-drama (the assumption that infalling observers should not experience anything unusual at the event horizon if the black hole is sufficiently large) cannot all be consistent with each other for the Hawking evaporation of a black hole with a finite number of quantum states given by the Bekenstein-Hawking entropy. AMPS suggested that the `most conservative' resolution to this inherent inconsistency between the various assumptions is to give up no-drama. Instead, an infalling observer would be terminated once he or she hits the so-called firewall. This seems rather surprising, because the curvature is negligibly small at the event horizon of a sufficiently large black hole, and thus one would expect nothing special but low energy physics. -
Firewalls and the Quantum Properties of Black Holes
Firewalls and the Quantum Properties of Black Holes A thesis submitted in partial fulfillment of the requirements for the degree of Bachelor of Science degree in Physics from the College of William and Mary by Dylan Louis Veyrat Advisor: Marc Sher Senior Research Coordinator: Gina Hoatson Date: May 10, 2015 1 Abstract With the proposal of black hole complementarity as a solution to the information paradox resulting from the existence of black holes, a new problem has become apparent. Complementarity requires a vio- lation of monogamy of entanglement that can be avoided in one of two ways: a violation of Einstein’s equivalence principle, or a reworking of Quantum Field Theory [1]. The existence of a barrier of high-energy quanta - or “firewall” - at the event horizon is the first of these two resolutions, and this paper aims to discuss it, for Schwarzschild as well as Kerr and Reissner-Nordstr¨omblack holes, and to compare it to alternate proposals. 1 Introduction, Hawking Radiation While black holes continue to present problems for the physical theories of today, quite a few steps have been made in the direction of understanding the physics describing them, and, consequently, in the direction of a consistent theory of quantum gravity. Two of the most central concepts in the effort to understand black holes are the black hole information paradox and the existence of Hawking radiation [2]. Perhaps the most apparent result of black holes (which are a consequence of general relativity) that disagrees with quantum principles is the possibility of information loss. Since the only possible direction in which to pass through the event horizon is in, toward the singularity, it would seem that information 2 entering a black hole could never be retrieved. -
UC Santa Barbara UC Santa Barbara Previously Published Works
UC Santa Barbara UC Santa Barbara Previously Published Works Title An apologia for firewalls Permalink https://escholarship.org/uc/item/9b33h6fw Journal Journal of High Energy Physics, 2013(9) ISSN 1126-6708 Authors Almheiri, A Marolf, D Polchinski, J et al. Publication Date 2013 DOI 10.1007/JHEP09(2013)018 Peer reviewed eScholarship.org Powered by the California Digital Library University of California An Apologia for Firewalls Ahmed Almheiri,1* Donald Marolf,2* Joseph Polchinski,3*y Douglas Stanford,4yz and James Sully5* *Department of Physics University of California Santa Barbara, CA 93106 USA yKavli Institute for Theoretical Physics University of California Santa Barbara, CA 93106-4030 USA zStanford Institute for Theoretical Physics and Department of Physics, Stanford University Stanford, CA 94305, USA Abstract We address claimed alternatives to the black hole firewall. We show that embedding the interior Hilbert space of an old black hole into the Hilbert space of the early radiation is inconsistent, as is embedding the semi-classical interior of an AdS black hole into any dual CFT Hilbert space. We develop the use of large AdS black holes as a system to sharpen the firewall argument. We also reiterate arguments that unitary non-local theories can avoid firewalls only if the non-localities are suitably dramatic. arXiv:1304.6483v2 [hep-th] 21 Jun 2013 [email protected] [email protected] [email protected] [email protected] [email protected] Contents 1 Introduction 2 2 Problems with B~ ⊂ E 4 3 Problems with nonlocal interactions 9 4 Evaporating AdS black holes 13 4.1 Boundary conditions and couplings . -
Mimicking Black Hole Event Horizons in Atomic and Solid-State Systems
Mimicking black hole event horizons in atomic and solid-state systems M. Franz1, 2 and M. Rozali1 1Department of Physics and Astronomy, University of British Columbia, Vancouver, BC, Canada V6T 1Z1 2Quantum Matter Institute, University of British Columbia, Vancouver BC, Canada V6T 1Z4 (Dated: August 3, 2018) Holographic quantum matter exhibits an intriguing connection between quantum black holes and more conventional (albeit strongly interacting) quantum many-body systems. This connection is manifested in the study of their thermodynamics, statistical mechanics and many-body quantum chaos. After explaining some of those connections and their significance, we focus on the most promising example to date of holographic quantum matter, the family of Sachdev-Ye-Kitaev (SYK) models. Those are simple quantum mechanical models that are thought to realize, holographically, quantum black holes. We review and assess various proposals for experimental realizations of the SYK models. Such experimental realization offers the exciting prospect of accessing black hole physics, and thus addressing many mysterious questions in quantum gravity, in tabletop experiments. I. INTRODUCTION tory a specific class of systems that give rise to holo- graphic quantum matter. They are described by the so called Sachdev-Ye-Kitaev (SYK) models [6{8] which are Among the greatest challenges facing modern physical \dual", in the sense described above, to a 1+1 dimen- sciences is the relation between quantum mechanics and sional gravitating "bulk" containing a black hole. We gravitational physics, described classically by Einstein's first review some of the background material on black general theory of relativity. Well known paradoxes arise hole thermodynamics, statistical mechanics and its rela- when the two theories are combined, for example when tion to many-body quantum chaos. -
Black Hole Physics
Black Hole Entropy, Hawking Radiation and Information Paradox 王卓骁 Major: planetary formation THCA Student Seminar Advisor: Doug Lin 2017/11/24 Outline • Over view of black hole physics • Black hole thermodynamics, black hole entropy • Hawking radiation • Information paradox • Recent ambitious hypothesis: Over view of black hole physics • 1784, first idea about black hole, John Michell and Laplace • 1915, general relativity built by Einstein, curvature V.S. matter • 1916, Schwarzschild got the general spherically symmetric, vacuum solution 2GM r = s c2 Over view of black hole physics Event Horizon 2GM r = s c2 Event Horizon Over view of black hole physics Event Horizon • What is event horizon? Schwarzschild solution e.g. world line light cone • Far away observer: space timeslope boundary, “point of no return” Schwarzschild Coordinates. Red line denoted outgoing light rays, while blue for ingoing. Fig. by Quinzacara 2014 Over view of black hole physics Event Horizon • What is event horizon? Schwarzschild solution e.g. • Far away observer: space time boundary, “point of no return” Equivalence Principle. • Traveling astronaut: nothing strange when passing through credit: Andrew Hamilton (JILA) t⇤ = t (r⇤ r) ± − Eddington-Finkelstein Coordinates. Red line denoted outgoing light rays, while blue for ingoing. Fig. by Quinzacara 2014 Over view of black hole physics Stellar evolution Chandrasekhar, 1931 < 1.4 M☉ Oppenheimer, 1939 < 3 M☉ credit: http://chandra.harvard.edu/xray_sources/stellar_evolution.html Over view of black hole physics • 1960s, Kerr solution, Newman solution, no-hair theorem • 1967, pulsar discovered, compact objects became realistic • 1970s, Bardeen, Bekenstein, Carter, Hawking led to BH thermodynamics. Involving QFT, Hawking radiation emerged. -
Many Physicists Believe That Entanglement Is the Essence Of
NEWS FEATURE SPACE. TIME. ENTANGLEMENT. n early 2009, determined to make the most annual essay contest run by the Gravity Many physicists believe of his first sabbatical from teaching, Mark Research Foundation in Wellesley, Massachu- Van Raamsdonk decided to tackle one of setts. Not only did he win first prize, but he also that entanglement is Ithe deepest mysteries in physics: the relation- got to savour a particularly satisfying irony: the the essence of quantum ship between quantum mechanics and gravity. honour included guaranteed publication in After a year of work and consultation with col- General Relativity and Gravitation. The journal PICTURES PARAMOUNT weirdness — and some now leagues, he submitted a paper on the topic to published the shorter essay1 in June 2010. suspect that it may also be the Journal of High Energy Physics. Still, the editors had good reason to be BROS. ENTERTAINMENT/ WARNER In April 2010, the journal sent him a rejec- cautious. A successful unification of quantum the essence of space-time. tion — with a referee’s report implying that mechanics and gravity has eluded physicists Van Raamsdonk, a physicist at the University of for nearly a century. Quantum mechanics gov- British Columbia in Vancouver, was a crackpot. erns the world of the small — the weird realm His next submission, to General Relativity in which an atom or particle can be in many BY RON COWEN and Gravitation, fared little better: the referee’s places at the same time, and can simultaneously report was scathing, and the journal’s editor spin both clockwise and anticlockwise. Gravity asked for a complete rewrite.