Strings & Gravity at University of Barcelona
|
|
|
- Suzan Stokes
- 5 years ago
- Views:
Transcription
1 Strings & Gravity at University of Barcelona Higher-dimensional black holes [R. Emparan, M.J. Rodríguez, J. Camps, M. Caldarelli, M. Ortaggio, B. Fiol, O. Dias] Microscopic description of black holes [R. Emparan, O. Dias, A. Maccarrone] Classification of SUGRA solutions [D. Roest, A. Celi, M. Caldarelli] Non-relativistic strings [J. Gomis] Symmetries of string & M-theory [J. Gomis, D. Roest] UV properties of strings and SUGRA [J. Russo] Decay of massive string states [J. Russo] Strings in magnetic backgrounds [J. Russo, J. López] AdS/CFT [AdS/QCD: J.M. Pons; Wilson loops: B. Fiol; etc]
2 Strings & Gravity at University of Barcelona Higher-dimensional black holes [R. Emparan, M.J. Rodríguez, J. Camps, M. Caldarelli, M. Ortaggio, B. Fiol, O. Dias] Microscopic description of black holes [R. Emparan, O. Dias, A. Maccarrone] Classification of SUGRA solutions [D. Roest, A. Celi, M. Caldarelli] Non-relativistic strings [J. Gomis] Symmetries of string & M-theory [J. Gomis, D. Roest] UV properties of strings and SUGRA [J. Russo] Decay of massive string states [J. Russo] Strings in magnetic backgrounds [J. Russo, J. López] AdS/CFT [AdS/QCD: J.M. Pons; Wilson loops: B. Fiol; etc]
3 Strings & Gravity at University of Barcelona Higher-dimensional black holes [R. Emparan, M.J. Rodríguez, J. Camps, M. Caldarelli, M. Ortaggio, B. Fiol, O. Dias] Microscopic description of black holes [R. Emparan, O. Dias, A. Maccarrone] Classification of SUGRA solutions [D. Roest, A. Celi, M. Caldarelli] Non-relativistic strings [J. Gomis] Symmetries of string & M-theory [J. Gomis, D. Roest] UV properties of strings and SUGRA [J. Russo] Decay of massive string states [J. Russo] Strings in magnetic backgrounds [J. Russo, J. López] AdS/CFT [AdS/QCD: J.M. Pons; Wilson loops: B. Fiol; etc]
4 Strings & Gravity at University of Barcelona Higher-dimensional black holes [R. Emparan, M.J. Rodríguez, J. Camps, M. Caldarelli, M. Ortaggio, B. Fiol, O. Dias] Microscopic description of black holes [R. Emparan, O. Dias, A. Maccarrone] Classification of SUGRA solutions [D. Roest, A. Celi, M. Caldarelli] Non-relativistic strings [J. Gomis] Symmetries of string & M-theory [J. Gomis, D. Roest] UV properties of strings and SUGRA [J. Russo] Decay of massive string states [J. Russo] Strings in magnetic backgrounds [J. Russo, J. López] AdS/CFT [AdS/QCD: J.M. Pons; Wilson loops: B. Fiol; etc]
5 Strings & Gravity at University of Barcelona Higher-dimensional black holes [R. Emparan, M.J. Rodríguez, J. Camps, M. Caldarelli, M. Ortaggio, B. Fiol, O. Dias] Microscopic description of black holes [R. Emparan, O. Dias, A. Maccarrone] Classification of SUGRA solutions [D. Roest, A. Celi, M. Caldarelli] Non-relativistic strings [J. Gomis] Symmetries of string & M-theory [J. Gomis, D. Roest] UV properties of strings and SUGRA [J. Russo] Decay of massive string states [J. Russo] Strings in magnetic backgrounds [J. Russo, J. López] AdS/CFT [AdS/QCD: J.M. Pons; Wilson loops: B. Fiol; etc]
6 Strings & Gravity at University of Barcelona Higher-dimensional black holes [R. Emparan, M.J. Rodríguez, J. Camps, M. Caldarelli, M. Ortaggio, B. Fiol, O. Dias] Microscopic description of black holes [R. Emparan, O. Dias, A. Maccarrone] Classification of SUGRA solutions [D. Roest, A. Celi, M. Caldarelli] Non-relativistic strings [J. Gomis] Symmetries of string & M-theory [J. Gomis, D. Roest] UV properties of strings and SUGRA [J. Russo] Decay of massive string states [J. Russo] Strings in magnetic backgrounds [J. Russo, J. López] AdS/CFT [AdS/QCD: J.M. Pons; Wilson loops: B. Fiol; etc]
7 Microscopic analysis of Black Hole superradiance Alessandro Maccarrone 3rd RTN Workshop, Valencia 2007 Based on work with R. Emparan & O. Dias
8 Motivation String theory provides a microscopic description of some properties of BHs: Entropy matching [A. Strominger & C. Vafa (1996),etc] Hawking radiation [C.G. Callan & J.M. Maldacena (1996)]
9 Motivation String theory provides a microscopic description of some properties of BHs: Entropy matching [A. Strominger & C. Vafa (1996),etc] Hawking radiation [C.G. Callan & J.M. Maldacena (1996)] Superradiance?
10 Superradiance Classical effect in rotating BHs due to the presence of an Ergoregion, so negative energy states are allowed. A wave can be scattered off the BH with a reflection coefficient greater than one (Superradiance) If ª(x ¹ )» f(r; µ)e i(²t má)! H SR condition: ² <! H m
11 Superradiance Classical effect in rotating BHs due to the presence of an Ergoregion, so negative energy states are allowed. A wave can be scattered off the BH with a reflection coefficient greater than one (Superradiance) If ª(x ¹ )» f(r; µ)e i(²t má)! H SR condition: ² <! H m This is the stimulated process, but there is also superradiant spontaneous emission.
12 D1-D5-P system For concreteness let us focus on D1-D5-P rotating BHs. The system can be described in terms of the CFT of an effective string carrying momentum excitations in two sectors (Left & Right). Bulk angular momentum is provided by coherent polarization of the fermionic excitations on the string. R L
13 Microscopic Hawking radiation In this picture Hawking Radiation is explained as emission of closed strings due to the collision of a Right and a Left mode. R L
14 Microscopic Hawking radiation In this picture Hawking Radiation is explained as emission of closed strings due to the collision of a Right and a Left mode. R R L BPS limit
15 Hawking vs. Superradiant emission The same mechanism allows to describe Superradiance. In rotating black holes, Hawking and superradiant emission are highly entangled. Extremal ( T H = 0) solutions are a suitable set-up to focus on superradiance, since Hawking radiation is not present in these backgrounds.
16 Non-BPS Extremal Black-Hole Rotating solution! H 6= 0
17 Non-BPS Extremal Black-Hole Rotating solution! H 6= 0 One sector described by polarized fermionic excitations filling up a Fermi Sea T H! 0
18 Non-BPS Extremal Black-Hole Rotating solution! H 6= 0 One sector described by polarized fermionic excitations filling up a Fermi Sea T H! 0 R L
19 Superradiance condition Fermi Sea is described by a distribution of the form: ( is the Fermi Energy) ½ F (²; m)! µ(! H m ²)! H m T H! 0
20 Superradiance condition Fermi Sea is described by a distribution of the form: ½ F (²; m)! µ(! H m ²) T H! 0! H m ( is the Fermi Energy) Excitations in this sector verify: ² <! H m
21 Superradiance condition Fermi Sea is described by a distribution of the form: ½ F (²; m)! µ(! H m ²) T H! 0! H m ( is the Fermi Energy) Excitations in this sector verify: ² <! H m This is the Superradiance condition.
22 Thanks for your attention.
Momentum-carrying waves on D1-D5 microstate geometries
Momentum-carrying waves on D1-D5 microstate geometries David Turton Ohio State Great Lakes Strings Conference, Purdue, Mar 4 2012 Based on 1112.6413 and 1202.6421 with Samir Mathur Outline 1. Black holes
Entropy of asymptotically flat black holes in gauged supergravit
Entropy of asymptotically flat black holes in gauged supergravity with Nava Gaddam, Alessandra Gnecchi (Utrecht), Oscar Varela (Harvard) - work in progress. BPS Black Holes BPS Black holes in flat space
Quantum mechanics and the geometry of spacetime
Quantum mechanics and the geometry of spacetime Juan Maldacena PPCM Conference May 2014 Outline Brief review of the gauge/gravity duality Role of strong coupling in the emergence of the interior Role of
Radiation from the non-extremal fuzzball
adiation from the non-extremal fuzzball Borun D. Chowdhury The Ohio State University The Great Lakes Strings Conference 2008 work in collaboration with Samir D. Mathur (arxiv:0711.4817) Plan Describe non-extremal
Three-Charge Black Holes and ¼ BPS States in Little String Theory
Three-Charge Black Holes and ¼ BPS States in Little String Theory SUNGJAY LEE KOREA INSTITUTE FOR ADVANCED STUDIES Joint work (JHEP 1512, 145) with Amit Giveon, Jeff Harvey, David Kutasov East Asia Joint
Holography for Black Hole Microstates
1 / 24 Holography for Black Hole Microstates Stefano Giusto University of Padua Theoretical Frontiers in Black Holes and Cosmology, IIP, Natal, June 2015 2 / 24 Based on: 1110.2781, 1306.1745, 1311.5536,
Strings and Black Holes
Particules Élémentaires, Gravitation et Cosmologie Année 2006-2007 String Theory: : basic concepts and applications Lecture 3: 27 February 2007 Strings and Black Holes 27 february 2007 Lecture 3 1 Outline
21 July 2011, USTC-ICTS. Chiang-Mei Chen 陳江梅 Department of Physics, National Central University
21 July 2011, Seminar @ USTC-ICTS Chiang-Mei Chen 陳江梅 Department of Physics, National Central University Outline Black Hole Holographic Principle Kerr/CFT Correspondence Reissner-Nordstrom /CFT Correspondence
Quantum gravity and entanglement
Quantum gravity and entanglement Ashoke Sen Harish-Chandra Research Institute, Allahabad, India HRI, February 2011 PLAN 1. Entanglement in quantum gravity 2. Entanglement from quantum gravity I shall use
Entanglement Entropy and AdS/CFT
Entanglement Entropy and AdS/CFT Christian Ecker 2 nd DK Colloquium January 19, 2015 The main messages of this talk Entanglement entropy is a measure for entanglement in quantum systems. (Other measures
Duality and Holography
Duality and Holography? Joseph Polchinski UC Davis, 5/16/11 Which of these interactions doesn t belong? a) Electromagnetism b) Weak nuclear c) Strong nuclear d) a) Electromagnetism b) Weak nuclear c) Strong
AdS/CFT Correspondence and Entanglement Entropy
AdS/CFT Correspondence and Entanglement Entropy Tadashi Takayanagi (Kyoto U.) Based on hep-th/0603001 [Phys.Rev.Lett.96(2006)181602] hep-th/0605073 [JHEP 0608(2006)045] with Shinsei Ryu (KITP) hep-th/0608213
Quantization of gravity, giants and sound waves p.1/12
Quantization of gravity, giants and sound waves Gautam Mandal ISM06 December 14, 2006 Quantization of gravity, giants and sound waves p.1/12 Based on... GM 0502104 A.Dhar, GM, N.Suryanarayana 0509164 A.Dhar,
Quantum mechanics and the geometry of space4me
Quantum mechanics and the geometry of space4me Juan Maldacena PPCM Conference May 2014 Outline Brief review of the gauge/gravity duality Role of strong coupling in the emergence of the interior Role of
Counting Schwarzschild and Charged Black Holes
SLAC-PUB-984 SU-ITP-9-40 September 199 hep-th/909075 Counting Schwarzschild and Charged Black Holes Edi Halyo 1, Barak Kol 1, Arvind Rajaraman 2 and Leonard Susskind 1 1 Department of Physics, Stanford
Thermodynamics of black branes as interacting branes
Thermodynamics of black branes as interacting branes Shotaro Shiba (KEK, Japan) East Asia Joint Workshop on Fields and Strings on May 29, 2016 Branes in supergravity 4d Einstein gravity Blackhole solutions
Emergent Quantum Criticality
(Non-)Fermi Liquids and Emergent Quantum Criticality from gravity Hong Liu Massachusetts setts Institute te of Technology HL, John McGreevy, David Vegh, 0903.2477 Tom Faulkner, HL, JM, DV, to appear Sung-Sik
Strings and Black Holes
Strings and Black Holes Erik Verlinde Institute for Theoretical Physics University of Amsterdam General Relativity R Rg GT µν µν = 8π µν Gravity = geometry Einstein: geometry => physics Strings: physics
Black Hole Entropy and Gauge/Gravity Duality
Tatsuma Nishioka (Kyoto,IPMU) based on PRD 77:064005,2008 with T. Azeyanagi and T. Takayanagi JHEP 0904:019,2009 with T. Hartman, K. Murata and A. Strominger JHEP 0905:077,2009 with G. Compere and K. Murata
Particles and Strings Probing the Structure of Matter and Space-Time
Particles and Strings Probing the Structure of Matter and Space-Time University Hamburg DPG-Jahrestagung, Berlin, March 2005 2 Physics in the 20 th century Quantum Theory (QT) Planck, Bohr, Heisenberg,...
A Holographic Description of Black Hole Singularities. Gary Horowitz UC Santa Barbara
A Holographic Description of Black Hole Singularities Gary Horowitz UC Santa Barbara Global event horizons do not exist in quantum gravity: String theory predicts that quantum gravity is holographic:
ON THE BLACK HOLE SPECIES
Paris ON THE BLACK HOLE SPECIES (by means of natural selection) Maria J. Rodriguez 16.07.09 Dumitru Astefanesei and MJR ( to appear) Marco Calderelli, Roberto Emparan and MJR ( 0806.1954 [hep-th] ) Henriette
Themodynamics at strong coupling from Holographic QCD
Themodynamics at strong coupling from Holographic QCD p. 1 Themodynamics at strong coupling from Holographic QCD Francesco Nitti APC, U. Paris VII Excited QCD Les Houches, February 23 2011 Work with E.
Holographic Entanglement and Interaction
Holographic Entanglement and Interaction Shigenori Seki RINS, Hanyang University and Institut des Hautes Études Scientifiques Intrication holographique et interaction à l IHES le 30 janvier 2014 1 Contents
BPS non-local operators in AdS/CFT correspondence. Satoshi Yamaguchi (Seoul National University) E. Koh, SY, arxiv: to appear in JHEP
BPS non-local operators in AdS/CFT correspondence Satoshi Yamaguchi (Seoul National University) E. Koh, SY, arxiv:0812.1420 to appear in JHEP Introduction Non-local operators in quantum field theories
String theory effects on 5D black strings
String theory effects on 5D black strings Alejandra Castro University of Michigan Work in collaboration with J. Davis, P. Kraus and F. Larsen hep-th/0702072, hep-th/0703087, 0705.1847[hep-th], 0801.1863
From Black holes to Qubits through String Theoretic Microscopes
ICHEP Formal Theory Development, July 10 th, 2018 @ Seoul From Black holes to Qubits through String Theoretic Microscopes Tadashi Takayanagi Yukawa Institute for Theoretical Physics Kyoto University 1
The holographic approach to critical points. Johannes Oberreuter (University of Amsterdam)
The holographic approach to critical points Johannes Oberreuter (University of Amsterdam) Scale invariance power spectrum of CMB P s (k) / k n s 1 Lambda archive WMAP We need to understand critical points!
Partial deconfinement phases in gauged multi-matrix quantum mechanics.
Partial deconfinement phases in gauged multi-matrix quantum mechanics. David Berenstein, UCSB based on arxiv:1806.05729 Vienna, July 12, 2018 Research supported by gauge/gravity Gauged matrix quantum mechanics
The Gauge/Gravity correspondence: linking General Relativity and Quantum Field theory
The Gauge/Gravity correspondence: linking General Relativity and Quantum Field theory Alfonso V. Ramallo Univ. Santiago IFIC, Valencia, April 11, 2014 Main result: a duality relating QFT and gravity Quantum
Three-Charge Black Holes and ¼ BPS States in Little String Theory I
Three-Charge Black Holes and ¼ BPS States in Little String Theory I SUNGJAY LEE KOREA INSTITUTE FOR ADVANCED STUDIES UNIVERSITY OF CHICAGO Joint work (1508.04437) with Amit Giveon, Jeff Harvey, David Kutasov
HIGHER SPIN DUALITY from THERMOFIELD DOUBLE QFT. AJ+Kenta Suzuki+Jung-Gi Yoon Workshop on Double Field Theory ITS, ETH Zurich, Jan 20-23,2016
HIGHER SPIN DUALITY from THERMOFIELD DOUBLE QFT AJ+Kenta Suzuki+Jung-Gi Yoon Workshop on Double Field Theory ITS, ETH Zurich, Jan 20-23,2016 Overview } Construction of AdS HS Gravity from CFT } Simplest
Introduction to AdS/CFT
Introduction to AdS/CFT Who? From? Where? When? Nina Miekley University of Würzburg Young Scientists Workshop 2017 July 17, 2017 (Figure by Stan Brodsky) Intuitive motivation What is meant by holography?
Numerical observation of Hawking radiation from acoustic black holes in atomic Bose-Einstein condensates
Numerical observation of Hawking radiation from acoustic black holes in atomic Bose-Einstein condensates Iacopo Carusotto BEC CNR-INFM and Università di Trento, Italy In collaboration with: Alessio Recati
Black Holes in String Theory
Black Holes in String Theory University of Southampton Dec 6, 2018 Based on: Bena, Giusto, Martinec, Russo, Shigemori, DT, Warner 1607.03908, PRL Bossard, Katmadas, DT 1711.04784, JHEP Martinec, Massai,
Quark-gluon plasma from AdS/CFT Correspondence
Quark-gluon plasma from AdS/CFT Correspondence Yi-Ming Zhong Graduate Seminar Department of physics and Astronomy SUNY Stony Brook November 1st, 2010 Yi-Ming Zhong (SUNY Stony Brook) QGP from AdS/CFT Correspondence
Six-point gluon scattering amplitudes from -symmetric integrable model
YITP Workshop 2010 Six-point gluon scattering amplitudes from -symmetric integrable model Yasuyuki Hatsuda (YITP) Based on arxiv:1005.4487 [hep-th] in collaboration with K. Ito (TITECH), K. Sakai (Keio
Gravity, Strings and Branes
Gravity, Strings and Branes Joaquim Gomis Universitat Barcelona Miami, 23 April 2009 Fundamental Forces Strong Weak Electromagnetism QCD Electroweak SM Gravity Standard Model Basic building blocks, quarks,
Topological String Theory
Topological String Theory Hirosi Ooguri (Caltech) Strings 2005, Toronto, Canada If String Theory is an answer, what is the question? What is String Theory? If Topological String Theory is an answer, what
M2-branes ending on M5-branes
M2-branes ending on M5-branes Vasilis Niarchos Crete Center for Theoretical Physics, University of Crete 7th Crete Regional Meeting on String Theory, 27/06/2013 based on recent work with K. Siampos 1302.0854,
The black hole information paradox
The black hole information paradox Samir D. Mathur The Ohio State University Outline 1. Review the black hole information paradox 2. What is the resolution in string theory? The fuzzball paradigm Quantum
Exact holography and entanglement entropy from one-point functions
Exact holography and entanglement entropy from one-point functions O-Kab Kwon (Sungkyunkwan University) In collaboration with Dongmin Jang, Yoonbai Kim, Driba Tolla arxiv:1612.05066, 1610.01490 1605.00849
Holographic vortex pair annihilation in superfluid turbulence
Holographic vortex pair annihilation in superfluid turbulence Vrije Universiteit Brussel and International Solvay Institutes Based mainly on arxiv:1412.8417 with: Yiqiang Du and Yu Tian(UCAS,CAS) Chao
WHY BLACK HOLES PHYSICS?
WHY BLACK HOLES PHYSICS? Nicolò Petri 13/10/2015 Nicolò Petri 13/10/2015 1 / 13 General motivations I Find a microscopic description of gravity, compatibile with the Standard Model (SM) and whose low-energy
arxiv:hep-ph/ v1 8 Feb 2000
Gravity, Particle Physics and their Unification 1 J. M. Maldacena Department of Physics Harvard University, Cambridge, Massachusetts 02138 arxiv:hep-ph/0002092v1 8 Feb 2000 1 Introduction Our present world
Heavy Quark Diffusion in AdS/CFT
Purdue University January 5th 2011 AdS/CFT is a correspondence that relates certain Quantum Field Theories and certain String Theories. Some characteristics of the correspondence. Large N c N = 4 SYM theory
Holography and (Lorentzian) black holes
Holography and (Lorentzian) black holes Simon Ross Centre for Particle Theory The State of the Universe, Cambridge, January 2012 Simon Ross (Durham) Holography and black holes Cambridge 7 January 2012
Towards a holographic formulation of cosmology
Towards a holographic formulation of cosmology Gonzalo Torroba Stanford University Topics in holography, supersymmetry and higher derivatives Mitchell Institute, Texas A&M, April 2013 During the last century,
Insight into strong coupling
Thank you 2012 Insight into strong coupling Many faces of holography: Top-down studies (string/m-theory based) Bottom-up approaches pheno applications to QCD-like and condensed matter systems (e.g. Umut
Talk online: sachdev.physics.harvard.edu
Talk online: sachdev.physics.harvard.edu Particle theorists Condensed matter theorists Quantum Entanglement Hydrogen atom: Hydrogen molecule: = _ = 1 2 ( ) Superposition of two electron states leads to
Emergent geometry: seeing further from the shoulders of giants.
Emergent geometry: seeing further from the shoulders of giants. David Berenstein, UCSB. Chapel Hill, May 8, 2014 Based mostly on arxiv:1301.3519 + arxiv:1305.2394 w. E. Dzienkowski + work in progress.
Black hole instabilities and violation of the weak cosmic censorship in higher dimensions
Black hole instabilities and violation of the weak cosmic censorship in higher dimensions Pau Figueras School of Mathematical Sciences, Queen Mary University of London w/ Markus Kunesch, Luis Lehner and
Recent developments in Monte Carlo studies of superstring theory
Recent developments in Monte Carlo studies of superstring theory Jun Nishimura (KEK & SOKENDAI) 12-16 August, 2013 Current Themes in High Energy Physics and Cosmology Niels Bohr Institute, Copenhagen Large-N
A toy model for the Kerr/CFT. correspondence
A toy model for the Kerr/CFT correspondence Monica Guică University of Pennsylvania with G. Compѐre, M.J. Rodriguez Motivation universal entropy for black holes good microscopic understanding only for
Conformal Symmetry of General Black Holes. Mirjam Cvetič
Conformal Symmetry of General Black Holes Mirjam Cvetič Progress to extract from geometry (mesoscopic approach) an underlying conformal symmetry & promoting it to two-dimensional conformal field theory
Masaki Shigemori. September 10, 2015 Int l Workshop on Strings, Black Holes and Quantum Info Tohoku Forum for Creativity, Tohoku U
Masaki Shigemori September 10, 2015 Int l Workshop on Strings, Black Holes and Quantum Info Tohoku Forum for Creativity, Tohoku U https://en.wikipedia.org/wiki/file:bh_lmc.png Plan BH microstates Microstate
Lectures on gauge-gravity duality
Lectures on gauge-gravity duality Annamaria Sinkovics Department of Applied Mathematics and Theoretical Physics Cambridge University Tihany, 25 August 2009 1. Review of AdS/CFT i. D-branes: open and closed
CFTs with O(N) and Sp(N) Symmetry and Higher Spins in (A)dS Space
CFTs with O(N) and Sp(N) Symmetry and Higher Spins in (A)dS Space Igor Klebanov Talk at New England Strings Meeting Brown University November 6, 2015 Based mainly on L. Fei, S. Giombi, IK, arxiv:1404.1094
On a holographic quantum quench with a finite size effect
On a holographic quantum quench with a finite size effect Tomonori Ugajin (U. Tokyo KITP) Based on work in progress with G.Mandal, R.Sinha Holographic Vistas on gravity and strings YITP, 2014 Introduction
Planar diagrams in light-cone gauge
Planar diagrams in light-cone gauge M. Kruczenski Purdue University Based on: hep-th/0603202 Summary Introduction Motivation: large-n, D-branes, AdS/CFT, results D-brane interactions: lowest order, light-cone
Three-Dimensional Black Holes and String Theory. Danny Birmingham 1. University College Dublin, Department of Mathematical Physics
DIAS-STP-97-10 Three-Dimensional Black Holes and String Theory Danny Birmingham 1 University College Dublin, Department of Mathematical Physics Beleld, Dublin 4, Ireland Ivo Sachs Dublin Institute for
Yun Soo Myung Inje University
On the Lifshitz black holes Yun Soo Myung Inje University in collaboration with T. Moon Contents 1. Introduction. Transition between Lifshitz black holes and other configurations 3. Quasinormal modes and
One Loop Tests of Higher Spin AdS/CFT
One Loop Tests of Higher Spin AdS/CFT Simone Giombi UNC-Chapel Hill, Jan. 30 2014 Based on 1308.2337 with I. Klebanov and 1401.0825 with I. Klebanov and B. Safdi Massless higher spins Consistent interactions
Theoretical Aspects of Black Hole Physics
Les Chercheurs Luxembourgeois à l Etranger, Luxembourg-Ville, October 24, 2011 Hawking & Ellis Theoretical Aspects of Black Hole Physics Glenn Barnich Physique théorique et mathématique Université Libre
Orientiholes Γ 2 Γ 1. Frederik Denef, Mboyo Esole and Megha Padi, arxiv:
Orientiholes Γ 2 Γ 1 Γ 0 Γ 1 Γ 2 Frederik Denef, Mboyo Esole and Megha Padi, arxiv:0901.2540 Outline Motivation and basic idea Review of N = 2 black hole bound states Type IIA orientiholes Motivation and
Non-relativistic holography
University of Amsterdam AdS/CMT, Imperial College, January 2011 Why non-relativistic holography? Gauge/gravity dualities have become an important new tool in extracting strong coupling physics. The best
Black holes in AdS/CFT
Black holes in AdS/CFT Seok Kim (Seoul National University) String theory and QFT, Fudan University Mar 15, 2019 Statistical approaches to BH 5d BPS BHs from D1-D5-P. Cardy formula of 2d CFT [Strominger,
Black Hole dynamics at large D
Black Hole dynamics at large D Roberto Emparan ICREA & U. Barcelona & YITP Kyoto w/ Kentaro Tanabe, Ryotaku Suzuki Einstein s eqns even in simplest cases encode a vast amount of physics Black holes colliding,
The fuzzball paradigm for black holes: FAQ
The fuzzball paradigm for black holes: FAQ Samir D. Mathur June 6, 2008 Contents 1 What is the black hole information paradox? 3 1.1 Can small quantum gravity effects encode information in the outgoing
Quantum entanglement and light propagation through Bose-Einstein condensate (BEC) M. Emre Taşgın
Quantum entanglement and light propagation through Bose-Einstein condensate (BEC) M. Emre Taşgın Advisor: M. Özgür Oktel Co-Advisor: Özgür E. Müstecaplıoğlu Outline Superradiance and BEC Superradiance
Entanglement and the Bekenstein-Hawking entropy
Entanglement and the Bekenstein-Hawking entropy Eugenio Bianchi relativity.phys.lsu.edu/ilqgs International Loop Quantum Gravity Seminar Black hole entropy Bekenstein-Hawking 1974 Process: matter falling
Holographic methods for cosmology. Gonzalo Torroba Stanford University
Holographic methods for cosmology Gonzalo Torroba Stanford University Observations and Theoretical Challenges in Primordial Cosmology KITP, UCSB, April 2013 Members of the collaboration Matt Dodelson Shunji
Holographic thermalization of 2D CFT
Holographic thermalization of 2D CFT Shu Lin ( 林树 ) Sun Yat-Sen University ICTS, USTC, 9/8/2016 SL, Shuryak, PRD 2008 SL, PRD 2016 Outline Phenomenon of thermalization in physics Holographic description
GRAVITY DUALS OF 2D SUSY GAUGE THEORIES
GRAVITY DUALS OF 2D SUSY GAUGE THEORIES BASED ON: 0909.3106 with E. Conde and A.V. Ramallo (Santiago de Compostela) [See also 0810.1053 with C. Núñez, P. Merlatti and A.V. Ramallo] Daniel Areán Milos,
Black hole near-horizon geometries
Black hole near-horizon geometries James Lucietti Durham University Imperial College, March 5, 2008 Point of this talk: To highlight that a precise concept of a black hole near-horizon geometry can be
Away-Side Angular Correlations Associated with Heavy Quark Jets
Away-Side Angular Correlations Associated with Heavy Quark Jets Jorge Noronha Presented by: William Horowitz The Ohio State University Based on: J.N, Gyulassy, Torrieri, arxiv:0807.1038 [hep-ph] and Betz,
CONTENTS. vii. CHAPTER 2 Operators 15
CHAPTER 1 Why Quantum Mechanics? 1 1.1 Newtonian Mechanics and Classical Electromagnetism 1 (a) Newtonian Mechanics 1 (b) Electromagnetism 2 1.2 Black Body Radiation 3 1.3 The Heat Capacity of Solids and
M-theory S-Matrix from 3d SCFT
M-theory S-Matrix from 3d SCFT Silviu S. Pufu, Princeton University Based on: arxiv:1711.07343 with N. Agmon and S. Chester arxiv:1804.00949 with S. Chester and X. Yin Also: arxiv:1406.4814, arxiv:1412.0334
Towards solution of string theory in AdS3 x S 3
Towards solution of string theory in AdS3 x S 3 Arkady Tseytlin based on work with Ben Hoare: arxiv:1303.1037, 1304.4099 Introduction / Review S-matrix for string in AdS3 x S3 x T4 with RR and NSNS flux
Lecture 4: 2 March 2007
Particules Élémentaires, Gravitation et Cosmologie Année 2006-2007 String Theory: : basic concepts and applications Lecture 4: 2 March 2007 Transplanckian String Collisions 2 march 2007 Lecture 4 1 Super-planckian-energy
Theory of Quantum Matter: from Quantum Fields to Strings
Theory of Quantum Matter: from Quantum Fields to Strings Salam Distinguished Lectures The Abdus Salam International Center for Theoretical Physics Trieste, Italy January 27-30, 2014 Subir Sachdev Talk
F o rce s U n i v e rs e
F o rce s U n i v e rs e @ N ap o l i Wolfgang Mück Università di Napoli Federico II and INFN, Sezione di Napoli Castel dell'ovo Napoli - Place of the 2nd RTN Workshop and Midterm Meeting 2006 Napoli in
Entanglement Entropy in Flat Holography
Entanglement Entropy in Flat Holography Based on work with Qiang Wen, Jianfei Xu( THU), and Hongliang Jiang( The HKUST) East Asian Joint Workshop KEK Theory workshop 2017 Bekenstein Bardeen-Carter-Hawking
Quantum Fields in Curved Spacetime
Quantum Fields in Curved Spacetime Lecture 3 Finn Larsen Michigan Center for Theoretical Physics Yerevan, August 22, 2016. Recap AdS 3 is an instructive application of quantum fields in curved space. The
HOLOGRAPHIC PROBES! COLLAPSING BLACK HOLES OF! Veronika Hubeny! Durham University & Institute for Advanced Study
HOLOGRAPHIC PROBES! OF! COLLAPSING BLACK HOLES Veronika Hubeny! Durham University & Institute for Advanced Study New frontiers in dynamical gravity workshop Cambridge, March 26, 2014 Based on work w/ H.
AdS/CFT duality, spin chains and 2d effective actions
AdS/CFT duality, spin chains and 2d effective actions R. Roiban, A. Tirziu and A. A. Tseytlin Asymptotic Bethe ansatz S-matrix and Landau-Lifshitz type effective 2-d actions, hep-th/0604199 also talks
Holographic superconductors
Holographic superconductors Sean Hartnoll Harvard University Work in collaboration with Chris Herzog and Gary Horowitz : 0801.1693, 0810.1563. Frederik Denef : 0901.1160. Frederik Denef and Subir Sachdev
Bosonization of a Finite Number of Non-Relativistic Fermions and Applications
Bosonization of a Finite Number of Non-Relativistic Fermions and Applications p. 1/4 Bosonization of a Finite Number of Non-Relativistic Fermions and Applications Avinash Dhar Tata Institute of Fundamental
Quantum Entanglement, Strange metals, and black holes. Subir Sachdev, Harvard University
Quantum Entanglement, Strange metals, and black holes Subir Sachdev, Harvard University Quantum entanglement Quantum Entanglement: quantum superposition with more than one particle Hydrogen atom: Hydrogen
A BRIEF TOUR OF STRING THEORY
A BRIEF TOUR OF STRING THEORY Gautam Mandal VSRP talk May 26, 2011 TIFR. In the beginning... The 20th century revolutions: Special relativity (1905) General Relativity (1915) Quantum Mechanics (1926) metamorphosed
Black Hole Entropy: An ADM Approach Steve Carlip U.C. Davis
Black Hole Entropy: An ADM Approach Steve Carlip U.C. Davis ADM-50 College Station, Texas November 2009 Black holes behave as thermodynamic objects T = κ 2πc S BH = A 4 G Quantum ( ) and gravitational
Gauge/Gravity Duality and the Black Hole Interior
Gauge/Gravity Duality and the Black Hole Interior Joseph Polchinski Kavli Institute for Theoretical Physics University of California at Santa Barbara KIAS-YITP joint workshop String Theory, Black Holes
Dualities and Topological Strings
Dualities and Topological Strings Strings 2006, Beijing - RD, C. Vafa, E.Verlinde, hep-th/0602087 - work in progress w/ C. Vafa & C. Beasley, L. Hollands Robbert Dijkgraaf University of Amsterdam Topological
Quantum Criticality and Black Holes
Quantum Criticality and Black Holes ubir Sachde Talk online at http://sachdev.physics.harvard.edu Quantum Entanglement Hydrogen atom: Hydrogen molecule: = _ = 1 2 ( ) Superposition of two electron states
Modelling the evolution of small black holes
Modelling the evolution of small black holes Elizabeth Winstanley Astro-Particle Theory and Cosmology Group School of Mathematics and Statistics University of Sheffield United Kingdom Thanks to STFC UK
AdS/CFT duality. Agnese Bissi. March 26, Fundamental Problems in Quantum Physics Erice. Mathematical Institute University of Oxford
AdS/CFT duality Agnese Bissi Mathematical Institute University of Oxford March 26, 2015 Fundamental Problems in Quantum Physics Erice What is it about? AdS=Anti de Sitter Maximally symmetric solution of
Quantum Field Theory and the Limits of Knowledge. Sean Carroll, Caltech
Quantum Field Theory and the Limits of Knowledge Sean Carroll, Caltech Two claims: 1. The laws of physics underlying everyday life are completely known. 2. The structure of quantum field theory provides
Talk based on: arxiv: arxiv: arxiv: arxiv: arxiv:1106.xxxx. In collaboration with:
Talk based on: arxiv:0812.3572 arxiv:0903.3244 arxiv:0910.5159 arxiv:1007.2963 arxiv:1106.xxxx In collaboration with: A. Buchel (Perimeter Institute) J. Liu, K. Hanaki, P. Szepietowski (Michigan) The behavior
Holographic Second Laws of Black Hole Thermodynamics
Holographic Second Laws of Black Hole Thermodynamics Federico Galli Gauge/Gravity Duality 018, Würzburg, 31 July 018 Based on arxiv: 1803.03633 with A. Bernamonti, R. Myers and J. Oppenheim Second Law
Microstates for non-extremal black holes
Microstates for non-extremal black holes Bert Vercnocke CEA Saclay ArXiv: 1109.5180 + 1208.3468 with Iosif Bena and Andrea Puhm (Saclay) 1110.5641 + in progress with Borun Chowdhury (Amsterdam) Corfu,