OBSERVERS IN QUANTUM GRAVITY

Size: px
Start display at page:

Download "OBSERVERS IN QUANTUM GRAVITY"

Transcription

1 OBSERVERS IN QUANTUM GRAVITY PROGRAM MONDAY Jan 22nd Flavio Mercati (chairman): welcome Jeremy Butterfield (**) COFFEE BREAK Flaminia Giacomini (*) LUNCH BREAK Michele Arzano (*) Angel Ballesteros (*) COFFEE BREAK Henrique Gomes (*) Časlav Brukner (*) TUESDAY Jan 23 rd Julian Barbour (**) Henrique Gomes (**) COFFEE BREAK Časlav Brukner (**) LUNCH BREAK Maximilian Lock (*) Markus Mueller (***) COFFEE BREAK Jose Manuel Carmona (***) Giovanni Amelino-Camelia (***) SESSION 1 (*) Quantum Reference frames, Quantum Causal Relations 2 (**) Many-world interpretation(s), Quantum Cosmology, Measurement Problem 3 (***) Emergence of Spacetime

2 Flavio Mercati (Sapienza University of Rome) Welcome and Introduction Jeremy Butterfield (Oxford University) Title - The Observer in Cosmology: joint work with Feraz Azhar Abstract: We review conceptual issues about the role of the observer, i.e. the various ways in which the process of observation contributes to the scope, and indeed content, of physical knowledge: especially in cosmology, both classical and quantum. We proceed in three stages. First, we discuss the role of the observer, independently of the details of physics, whether classical or quantum. Second, we discuss the role of the observer in classical physics, especially classical cosmology: i.e. in a cosmology for a classical (not quantum) world. Thus this second stage considers issues about selection effects. Third, we discuss the role of the observer in quantum physics in general: and especially in quantum cosmology. Here we focus attention on the research programme of Hartle, Hawking and Hertog, especially the relation of their proposed no-boundary state to inflation, and to selection effects. Flaminia Giacomini (Vienna University) Title - Quantum mechanics and the covariance of physical laws in quantum reference frames Abstract: In physics, every observation is made with respect to a frame of reference. Although reference frames are usually not considered as degrees of freedom, in all practical situations it is a physical system which constitutes a reference frame. Can a quantum system be considered as a reference frame and, if so, which description would it give of the world? The relational approach to physics suggests that all the features of a system - such as entanglement and superposition - are observer-dependent: what appears classical from our usual laboratory description might appear to be in a superposition, or entangled, from the point of view of such a quantum reference frame. In this work, we develop an operational framework for quantum theory to be applied within quantum reference frames. We find that, when reference frames are treated as quantum degrees of freedom, a more general transformation between reference frames has to be introduced. With this transformation we describe states, measurement, and dynamical evolution in different quantum reference frames, without appealing to an external, absolute reference frame. The transformation also leads to a generalisation of the notion of covariance of dynamical physical laws, which we explore in the case of `superposition of Galilean translations' and `superposition of Galilean boosts'. In addition, we consider the situation when the reference frame moves in a `superposition of accelerations', which leads us to extend the validity of the weak equivalence principle to quantum reference frames. Finally, this approach to quantum reference frames also has natural applications in defining the notion of the rest frame of a quantum system when it is in a superposition of momenta with respect to the laboratory frame of reference. Michele Arzano (University of Rome La Sapienza)

3 Title - Accelerated observers and horizons at the Planck scale Abstract: We extend the concept of accelerated horizons to the framework of deformed relativistic kinematics at the Planck scale. We show that the non-trivial effects due to symmetry deformation lead to a blurring of the horizon which manifests in a finite redshift for signals sent by an observer which approaches the horizon. Angel Ballesteros (Burgos University) Title - From quantum groups to noncommutative spacetimes and worldlines Abstract: The construction of noncommutative Lorentzian spacetimes and their associated noncommutative spaces of worldlines is reviewed. In the commutative case both spaces are constructed as homogeneous spaces of the (A)dS and Poincaré groups, and their noncommutative analogues arise as quantizations of the corresponding Poisson homogeneous spaces that are invariant under the appropriate (co)action from (A)dS or Poincaré quantum groups. In this construction, a new duality between reductive homogeneous spaces and coisotropic Lie bialgebras can be envisaged. In particular, the noncommutative spaces arising from the well-known kappa- (A)dS and Poincaré quantum groups are explicitly given, and the role of the cosmological constant is outlined. Moreover, a proposal for the description of quantum observers as coordinates on the non-commutative space of time-like worldlines is sketched. Monday 22 talk Henrique Gomes (Perimeter Institute for Theoretical Physics) Title - Observers, gauge symmetries, and best-matching. Abstract: One problem of gauge theories in general, but general relativity in particular, is determining a local basis of observables. E.g. a Wilson loop is not gauge-invariant within a region whose boundary intersects it. Recently, interest in defining boundary degrees of freedom which restore gauge-invariance for such types of observables has resurged. Donnelly and Freidel have related such degrees of freedom (edge-modes) to choices of local frames, which can in their turn be related to choices of local observers. In this talk, I will provide a relation between these modes, BRST ghosts, and a generalization of Barbour and Bertotti's 'best-matching'. Tuesday 23 talk Title - What is an observer in quantum geometrodynamics? Abstract: General relativity has a notorious problem: parametrizing its physical configuration space, even at an abstract level, is beyond our current knowledge. Replacing refoliation invariance with conformal transformations as a local gauge-symmetry allows one to parametrize the physical configuration space. Nonetheless, each point in this reduced configuration space contains non-local

4 information about the fields throughout physical space. It is essentially a space of relations. I will argue for a notion of "instantaneous states of observers" as consistent subsets of these relations. Such subsets define not points, but submanifolds in configuration space, corresponding to the configurations of the entire universe compatible with that instantaneous state of the observer. Relative quantum volumes of such regions define relative probabilities for different outcomes as perceived by observers. According to such outcomes, observers update their proposal for the wavefunction. Monday 22 talk Title - Bell s theorem for temporal order Caslav Brukner University of Vienna Abstract: In general relativity causal relations between any pair of events is uniquely determined by locally predefined variables the distribution of matter-energy degrees of freedom in the events past light-cone. Under the assumption of locally predefined causal order, agents performing freely chosen local operations on an initially local quantum state cannot violate Bell inequalities. However, superposition of massive objects can effectively lead to entanglement in the temporal order between groups of local operations, enabling the violation of the inequalities. This shows that temporal orders between events can be indefinite in non-classical space-times. Tuesday 23 talk Title - A no-go theorem for ``facts of the world'' Abstract: Wigner's friend is a thought experiment in which, from the point of view of Wigner, the friend, who measures a quantum system, is entangled with the state of the system. Both Wigner and the friend can in principle confirm their state assignment by performing an appropriate measurement. The result of each of these measurements as manifested trough a click in a detector or a specific position of the pointer -- can be seen as a fact. I will show that the view that holds the coexistence of the "facts of the world" common both for Wigner and the friend runs into the problem of the hidden variable program, for which I will derive a Bell-type theorem. A possible implication of theorem would be that facts are defined only relative to an observer. Still considering Wigner's friend thought experiment I will show how the friend can prove herself that she is in a superposition, and how in such a situation the application of standard quantum formalism seems to fail. Reference: arxiv: Julian Barbour (Oxford University) Title The End of Time and the Many-Instants interpretation of Quantum Mechanics Abstract: I will review temporal relationalism, and the timeless approach to physics, with particular attention to its implications for quantum mechanics. A variant of Everett s many-worlds interpretation of quantum mechanics emerges as a consequence of this point of view. I named

5 this approach the `many instants interpretation of quantum mechanics. I will describe its features, and comment on its implications in light of recent findings, by my collaborators and me, regarding the cosmological arrow of time and the nature of the Big Bang. Maximilian Lock (Imperial College London/University of Vienna) Title - A quantum version of the relativistic light-clock Abstract: The conflict between quantum theory and the theory of relativity is exemplified in their treatment of time. We examine the ways in which their conceptions differ, and consider a quantum version of the light-clock thought experiment commonly used to illustrate relativistic time dilation. This ``semiclassical'' clock model combines elements of both theories, and exhibits both quantitative and qualitative differences from the corresponding proper time of an ideal pointlike observer. Einstein begins his original formulation of relativity with a kind of operationalism, defining simultaneity by the ability of two separated clocks to synchronise. Our results show that a similarly operational definition of time, now accounting for quantum mechanics, must include extra considerations. Markus Mueller (University of Vienna) Title - Quantum theory and the structure of spacetime in the light of operationalism Abstract: Quantum theory and the structure of spacetime in the light of operationalism Some approaches to quantum gravity, e.g. the AdS/CFT correspondence or Sean Carroll s approach, promote the idea that spacetime can ultimately be reconstructed from the structure of (some underlying) quantum theory. In this talk, I sketch a research program that aims at studying aspects of this idea without committing to a particular model or ansatz. Namely, simple thought experiments of communicating observers, based only on what we currently know about physics, can shed light on the structural relation between quantum theory and spacetime in both directions. I will first present a simple thought experiment that shows how relativity of simultaneity constrains the structure of the quantum bit, without assuming the validity of quantum theory from the outset [1]. Then I will show that this kind of reasoning can be extended and reversed: if we assume the validity of quantum theory and the existence of certain types of universal measurement procedures (but make no assumptions about spacetime), then observers will automatically relate their descriptions of local laboratory physics by elements of the Lorentz group SO(3,1) [2]. Thus, taking the question of how observers operate in a quantum world seriously can help illuminate the relation between two seemingly separate aspects of physics. [1] A.J.P. Garner, M.P. Mueller, and O. C. O. Dahlsten, The complex and quaternionic quantum bits from relativity of simultaneity on an interferometer, Proc. R. Soc. A 473, (2017); arxiv: [2] P.A. Hoehn and M.P. Mueller, An operational approach to spacetime symmetries: Lorentz transformations from quantum communication, New J. Phys. 18, (2016); arxiv: Jose Manuel Carmona (University of Zaragoza)

6 Title - Observers and their notion of spacetime beyond special relativity Abstract: It is plausible that quantum gravity effects may lead us to a description of Nature beyond the framework of special relativity. In this case, either the relativity principle is broken or it is maintained. These two scenarios (a violation or a deformation of special relativity) are very different, both conceptually and phenomenologically. We discuss some of their implications on the description of events for different observers and the definition of a universal or observer-dependent notion of spacetime. Amelino Camelia (University of Rome La Sapienza) Title - Scale-dependent notions of Spacetime Abstract: I will explore the possibility, motivated by certain approaches to QG, that the kinematical notion at the basis of an observer's picture of spacetime might depend on the properties of the probes the observer has access to.

PLAN OF MY TALK. 2. A story you might have not heard: Inertial Observers and Relationalism

PLAN OF MY TALK. 2. A story you might have not heard: Inertial Observers and Relationalism Fl avi omer cat i Sapi enzauni ver si t yofrome 1 1 PLAN OF MY TALK 1. Overview of the workshop 2. A story you might have not heard: Inertial Observers and Relationalism 3. My first timid step towards

More information

Symmetry protected entanglement between gravity and matter

Symmetry protected entanglement between gravity and matter Symmetry protected entanglement between gravity and matter Nikola Paunković SQIG Security and Quantum Information Group, IT Departamento de Matemática, IST in collaboration with Marko Vojinović GPF Group

More information

Why we need quantum gravity and why we don t have it

Why we need quantum gravity and why we don t have it Why we need quantum gravity and why we don t have it Steve Carlip UC Davis Quantum Gravity: Physics and Philosophy IHES, Bures-sur-Yvette October 2017 The first appearance of quantum gravity Einstein 1916:

More information

LQG, the signature-changing Poincaré algebra and spectral dimension

LQG, the signature-changing Poincaré algebra and spectral dimension LQG, the signature-changing Poincaré algebra and spectral dimension Tomasz Trześniewski Institute for Theoretical Physics, Wrocław University, Poland / Institute of Physics, Jagiellonian University, Poland

More information

Atomism and Relationalism as guiding principles for. Quantum Gravity. Francesca Vidotto

Atomism and Relationalism as guiding principles for. Quantum Gravity. Francesca Vidotto Atomism and Relationalism as guiding principles for Quantum Gravity! Frontiers of Fundamental Physics (FFP14) Marseille July 16th, 2013 CONTENT OF THE TALK RELATIONALISM!! ATOMISM! ONTOLOGY: Structural

More information

What s Observable in Special and General Relativity?

What s Observable in Special and General Relativity? What s Observable in Special and General Relativity? Oliver Pooley oliver.pooley@philosophy.oxford.ac.uk Oriel College, Oxford ESF Conference 24 March 2004; What s Observable in Special and General Relativity?

More information

Loop Quantum Gravity a general-covariant lattice gauge theory. Francesca Vidotto UNIVERSITY OF THE BASQUE COUNTRY

Loop Quantum Gravity a general-covariant lattice gauge theory. Francesca Vidotto UNIVERSITY OF THE BASQUE COUNTRY a general-covariant lattice gauge theory UNIVERSITY OF THE BASQUE COUNTRY Bad Honnef - August 2 nd, 2018 THE GRAVITATIONAL FIELD GENERAL RELATIVITY: background independence! U(1) SU(2) SU(3) SL(2,C) l

More information

String Theory. Quantum Mechanics and Gravity: Cliff Burgess, McGill. The start of a beautiful relationship?

String Theory. Quantum Mechanics and Gravity: Cliff Burgess, McGill. The start of a beautiful relationship? Quantum Mechanics and Gravity: The start of a beautiful relationship? Cliff Burgess, McGill Outline The 20 th Century Crisis Quantum Mechanics vs Relativity A Theoretical Balancing Act Possible Problems?

More information

LECTURE 1: What is wrong with the standard formulation of quantum theory?

LECTURE 1: What is wrong with the standard formulation of quantum theory? LECTURE 1: What is wrong with the standard formulation of quantum theory? Robert Oeckl IQG-FAU & CCM-UNAM IQG FAU Erlangen-Nürnberg 31 October 2013 Outline 1 Classical physics Reality in classical physics

More information

Relativity, Gravitation, and Cosmology

Relativity, Gravitation, and Cosmology Relativity, Gravitation, and Cosmology A basic introduction TA-PEI CHENG University of Missouri St. Louis OXFORD UNIVERSITY PRESS Contents Parti RELATIVITY Metric Description of Spacetime 1 Introduction

More information

Dimensional Reduction in the Early Universe

Dimensional Reduction in the Early Universe Dimensional Reduction in the Early Universe Giulia Gubitosi University of Rome Sapienza References: PLB 736 (2014) 317 PRD 88 (2013) 103524 PRD 88 (2013) 041303 PRD 87 (2013) 123532 (with G. Amelino-Camelia,

More information

Spacetime Realism and Quantum Gravity

Spacetime Realism and Quantum Gravity Spacetime Realism and Quantum Gravity Oliver Pooley Oriel College, University of Oxford oliver.pooley@philosophy.ox.ac.uk 6 July, 2000 Abstract Sophisticated substantivalism is defended as a response to

More information

Bell s Theorem. Ben Dribus. June 8, Louisiana State University

Bell s Theorem. Ben Dribus. June 8, Louisiana State University Bell s Theorem Ben Dribus Louisiana State University June 8, 2012 Introduction. Quantum Theory makes predictions that challenge intuitive notions of physical reality. Einstein and others were sufficiently

More information

EMERGENT GRAVITY AND COSMOLOGY: THERMODYNAMIC PERSPECTIVE

EMERGENT GRAVITY AND COSMOLOGY: THERMODYNAMIC PERSPECTIVE EMERGENT GRAVITY AND COSMOLOGY: THERMODYNAMIC PERSPECTIVE Master Colloquium Pranjal Dhole University of Bonn Supervisors: Prof. Dr. Claus Kiefer Prof. Dr. Pavel Kroupa May 22, 2015 Work done at: Institute

More information

Intrinsic Time Quantum Geometrodynamics (ITQG)

Intrinsic Time Quantum Geometrodynamics (ITQG) Intrinsic Time Quantum Geometrodynamics (ITQG) Assistant Professor Eyo Ita Eyo Eyo Ita Physics Department LQG International Seminar United States Naval Academy Annapolis, MD 27 October, 2015 Outline of

More information

Manifestly diffeomorphism invariant classical Exact Renormalization Group

Manifestly diffeomorphism invariant classical Exact Renormalization Group Manifestly diffeomorphism invariant classical Exact Renormalization Group Anthony W. H. Preston University of Southampton Supervised by Prof. Tim R. Morris Talk prepared for Asymptotic Safety seminar,

More information

TOPIC VII ADS/CFT DUALITY

TOPIC VII ADS/CFT DUALITY TOPIC VII ADS/CFT DUALITY The conjecture of AdS/CFT duality marked an important step in the development of string theory. Quantum gravity is expected to be a very complicated theory. String theory provides

More information

What is wrong with the standard formulation of quantum theory?

What is wrong with the standard formulation of quantum theory? What is wrong with the standard formulation of quantum theory? Robert Oeckl Centro de Ciencias Matemáticas UNAM, Morelia Seminar General Boundary Formulation 21 February 2013 Outline 1 Classical physics

More information

Chris Verhaaren Joint Theory Seminar 31 October With Zackaria Chacko, Rashmish Mishra, and Simon Riquelme

Chris Verhaaren Joint Theory Seminar 31 October With Zackaria Chacko, Rashmish Mishra, and Simon Riquelme Chris Verhaaren Joint Theory Seminar 31 October 2016 With Zackaria Chacko, Rashmish Mishra, and Simon Riquelme It s Halloween A time for exhibiting what some find frightening And seeing that it s not so

More information

A loop quantum multiverse?

A loop quantum multiverse? Space-time structure p. 1 A loop quantum multiverse? Martin Bojowald The Pennsylvania State University Institute for Gravitation and the Cosmos University Park, PA arxiv:1212.5150 Space-time structure

More information

Super Yang-Mills Theory in 10+2 dims. Another Step Toward M-theory

Super Yang-Mills Theory in 10+2 dims. Another Step Toward M-theory 1 Super Yang-Mills Theory in 10+2 dims. Another Step Toward M-theory Itzhak Bars University of Southern California Talk at 4 th Sakharov Conference, May 2009 http://physics.usc.edu/~bars/homepage/moscow2009_bars.pdf

More information

Explorations of Planck-scale Noise in Noncommutative Holographic Spacetime 1

Explorations of Planck-scale Noise in Noncommutative Holographic Spacetime 1 Explorations of Planck-scale Noise in Noncommutative Holographic Spacetime 1 Ohkyung Kwon 1 C. J. Hogan, "Interferometers as Holograpic Clocks," arxiv:1002.4880 [gr-qc] Motivation Events in spacetime are

More information

the observer s ghost or, on the properties of a connection one-form in field space

the observer s ghost or, on the properties of a connection one-form in field space the observer s ghost or, on the properties of a connection one-form in field space ilqgs 06 dec 16 in collaboration with henrique gomes based upon 1608.08226 (and more to come) aldo riello international

More information

Excluding Black Hole Firewalls with Extreme Cosmic Censorship

Excluding Black Hole Firewalls with Extreme Cosmic Censorship Excluding Black Hole Firewalls with Extreme Cosmic Censorship arxiv:1306.0562 Don N. Page University of Alberta February 14, 2014 Introduction A goal of theoretical cosmology is to find a quantum state

More information

Planck-Scale Soccer-Ball Problem: A Case of Mistaken Identity

Planck-Scale Soccer-Ball Problem: A Case of Mistaken Identity entropy Article Planck-Scale Soccer-Ball Problem: A Case of Mistaken Identity Giovanni Amelino-Camelia 1,2 1 Dipartimento di Fisica, Università di Roma La Sapienza, P.le A. Moro 2, 00185 Roma, Italy; amelino@roma1.infn.it

More information

The nature of Reality: Einstein-Podolsky-Rosen Argument in QM

The nature of Reality: Einstein-Podolsky-Rosen Argument in QM The nature of Reality: Einstein-Podolsky-Rosen Argument in QM Michele Caponigro ISHTAR, Bergamo University Abstract From conceptual point of view, we argue about the nature of reality inferred from EPR

More information

From Bohmian Mechanics to Bohmian Quantum Gravity. Antonio Vassallo Instytut Filozofii UW Section de Philosophie UNIL

From Bohmian Mechanics to Bohmian Quantum Gravity. Antonio Vassallo Instytut Filozofii UW Section de Philosophie UNIL From Bohmian Mechanics to Bohmian Quantum Gravity Antonio Vassallo Instytut Filozofii UW Section de Philosophie UNIL The Measurement Problem in Quantum Mechanics (1) The wave-function of a system is complete,

More information

Towards a manifestly diffeomorphism invariant Exact Renormalization Group

Towards a manifestly diffeomorphism invariant Exact Renormalization Group Towards a manifestly diffeomorphism invariant Exact Renormalization Group Anthony W. H. Preston University of Southampton Supervised by Prof. Tim R. Morris Talk prepared for UK QFT-V, University of Nottingham,

More information

Why spin-foam models violat~ ' Lorentz Invariance

Why spin-foam models violat~ ' Lorentz Invariance Why spin-foam models violat~ ' Lorentz Invariance Much recent interest in Lorentz violation in quantum gravity. Phenomenology progresses... theory attempts to catch up and offer predictions. Could local

More information

Non-relativistic holography

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

More information

2T-physics and the Standard Model of Particles and Forces Itzhak Bars (USC)

2T-physics and the Standard Model of Particles and Forces Itzhak Bars (USC) 2T-physics and the Standard Model of Particles and Forces Itzhak Bars (USC) hep-th/0606045 Success of 2T-physics for particles on worldlines. Field theory version of 2T-physics. Standard Model in 4+2 dimensions.

More information

Approaches to Quantum Gravity A conceptual overview

Approaches to Quantum Gravity A conceptual overview Approaches to Quantum Gravity A conceptual overview Robert Oeckl Instituto de Matemáticas UNAM, Morelia Centro de Radioastronomía y Astrofísica UNAM, Morelia 14 February 2008 Outline 1 Introduction 2 Different

More information

The spacetime of special relativity

The spacetime of special relativity 1 The spacetime of special relativity We begin our discussion of the relativistic theory of gravity by reviewing some basic notions underlying the Newtonian and special-relativistic viewpoints of space

More information

Relative Locality and gravity in quantum spacetime

Relative Locality and gravity in quantum spacetime DOTTORATO DI RICERCA IN FISICA XXV CICLO Relative Locality and gravity in quantum spacetime Candidate: Loret Niccolò Advisor: Giovanni Amelino-Camelia 25 October 2012 THEORY PHENOMENOLOGY EQUATIONS OF

More information

Doubly Special Relativity

Doubly Special Relativity Doubly Special Relativity gr-qc/0207049 preprint version 1 of Nature 418 (2002) 34-35 Giovanni AMELINO-CAMELIA Dipartimento di Fisica, Università La Sapienza, P.le Moro 2, I-00185 Roma, Italy ABSTRACT

More information

Galileon Cosmology ASTR448 final project. Yin Li December 2012

Galileon Cosmology ASTR448 final project. Yin Li December 2012 Galileon Cosmology ASTR448 final project Yin Li December 2012 Outline Theory Why modified gravity? Ostrogradski, Horndeski and scalar-tensor gravity; Galileon gravity as generalized DGP; Galileon in Minkowski

More information

Gravity, Strings and Branes

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,

More information

Entanglement and the Bekenstein-Hawking entropy

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

More information

Quantum Black Holes and Global Symmetries

Quantum Black Holes and Global Symmetries Quantum Black Holes and Global Symmetries Daniel Klaewer Max-Planck-Institute for Physics, Munich Young Scientist Workshop 217, Schloss Ringberg Outline 1) Quantum fields in curved spacetime 2) The Unruh

More information

Homework 1: Special Relativity. Reading Assignment. Essential Problems. 1 Pole-in-Barn (Hartle 4-3) 2 Black Hole Entropy and Dimensional Analysis

Homework 1: Special Relativity. Reading Assignment. Essential Problems. 1 Pole-in-Barn (Hartle 4-3) 2 Black Hole Entropy and Dimensional Analysis Homework 1: Special Relativity Course: Physics 208, General Relativity (Winter 2017) Instructor: Flip Tanedo (flip.tanedo@ucr.edu) Due Date: Tuesday, January 17 in class You are required to complete the

More information

16. Einstein and General Relativistic Spacetimes

16. Einstein and General Relativistic Spacetimes 16. Einstein and General Relativistic Spacetimes Problem: Special relativity does not account for the gravitational force. To include gravity... Geometricize it! Make it a feature of spacetime geometry.

More information

Emergent Spacetime. XXIII rd Solvay Conference in Physics December, Nathan Seiberg

Emergent Spacetime. XXIII rd Solvay Conference in Physics December, Nathan Seiberg Emergent Spacetime XXIII rd Solvay Conference in Physics December, 2005 Nathan Seiberg Legal disclaimers I ll outline my points of confusion. There will be many elementary and well known points. There

More information

Standing Waves in the Lorentz-Covariant World

Standing Waves in the Lorentz-Covariant World Foundations of Physics, Vol. 35, No. 7, July 2005 ( 2005) DOI: 10.1007/s10701-005-6410-3 Standing Waves in the Lorentz-Covariant World Y. S. Kim 1 and Marilyn E. Noz 2 Received April 11, 2005 When Einstein

More information

From Quantum Cellular Automata to Quantum Field Theory

From Quantum Cellular Automata to Quantum Field Theory From Quantum Cellular Automata to Quantum Field Theory Alessandro Bisio Frontiers of Fundamental Physics Marseille, July 15-18th 2014 in collaboration with Giacomo Mauro D Ariano Paolo Perinotti Alessandro

More information

Holographic Special Relativity:

Holographic Special Relativity: Holographic Special Relativity: Observer Space from Conformal Geometry Derek K. Wise University of Erlangen Based on 1305.3258 International Loop Quantum Gravity Seminar 15 October 2013 1 Holographic special

More information

Postulates of Special Relativity

Postulates of Special Relativity Relativity Relativity - Seen as an intricate theory that is necessary when dealing with really high speeds - Two charged initially stationary particles: Electrostatic force - In another, moving reference

More information

arxiv: v1 [gr-qc] 11 Sep 2014

arxiv: v1 [gr-qc] 11 Sep 2014 Frascati Physics Series Vol. 58 (2014) Frontier Objects in Astrophysics and Particle Physics May 18-24, 2014 arxiv:1409.3370v1 [gr-qc] 11 Sep 2014 OPEN PROBLEMS IN GRAVITATIONAL PHYSICS S. Capozziello

More information

Observer dependent background geometries arxiv:

Observer dependent background geometries arxiv: Observer dependent background geometries arxiv:1403.4005 Manuel Hohmann Laboratory of Theoretical Physics Physics Institute University of Tartu DPG-Tagung Berlin Session MP 4 18. März 2014 Manuel Hohmann

More information

Stable violation of the null energy condition and non-standard cosmologies

Stable violation of the null energy condition and non-standard cosmologies Paolo Creminelli (ICTP, Trieste) Stable violation of the null energy condition and non-standard cosmologies hep-th/0606090 with M. Luty, A. Nicolis and L. Senatore What is the NEC? Energy conditions: Singularity

More information

Quantum Gravity Phenomenology

Quantum Gravity Phenomenology Quantum Gravity Phenomenology Sabine Hossenfelder Sabine Hossenfelder, Quantum Gravity Phenomenology 1/16 Why do we need quantum gravity? Because We don t know what is the gravitational field of a quantum

More information

HIGHER SPIN PROBLEM IN FIELD THEORY

HIGHER SPIN PROBLEM IN FIELD THEORY HIGHER SPIN PROBLEM IN FIELD THEORY I.L. Buchbinder Tomsk I.L. Buchbinder (Tomsk) HIGHER SPIN PROBLEM IN FIELD THEORY Wroclaw, April, 2011 1 / 27 Aims Brief non-expert non-technical review of some old

More information

6.2 Quantum Gravity and the Quantization of Time 193

6.2 Quantum Gravity and the Quantization of Time 193 6.2 Quantum Gravity and the Quantization of Time 193 (points), assumed to possess statistical weights according to Ψ 2. In contrast to Bohm s time-dependent theory, this is no longer an initial condition

More information

Extensions of Lorentzian spacetime geometry

Extensions of Lorentzian spacetime geometry Extensions of Lorentzian spacetime geometry From Finsler to Cartan and vice versa Manuel Hohmann Teoreetilise Füüsika Labor Füüsika Instituut Tartu Ülikool LQP33 Workshop 15. November 2013 Manuel Hohmann

More information

Experiments testing macroscopic quantum superpositions must be slow

Experiments testing macroscopic quantum superpositions must be slow Experiments testing macroscopic quantum superpositions must be slow spatial (Scientic Reports (2016) - arxiv:1509.02408) Andrea Mari, Giacomo De Palma, Vittorio Giovannetti NEST - Scuola Normale Superiore

More information

Causal Sets: Overview and Status

Causal Sets: Overview and Status University of Mississippi QGA3 Conference, 25 Aug 2006 The Central Conjecture Causal Sets A causal set is a partially ordered set, meaning that x, y, z x y, y z x z x y, y x x = y which is locally finite,

More information

Deformations of Spacetime Horizons and Entropy

Deformations of Spacetime Horizons and Entropy Adv. Studies Theor. Phys., ol. 7, 2013, no. 22, 1095-1100 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/10.12988/astp.2013.39100 Deformations of Spacetime Horizons and Entropy Paul Bracken Department

More information

Cosmology meets Quantum Gravity?

Cosmology meets Quantum Gravity? Cosmology meets Quantum Gravity? Sergey Sibiryakov Benasque, 08/08/14 plethora of inflationary models vs. limited experimental information plethora of inflationary models vs. limited experimental information

More information

Fourth International Workshop on Theoretical and Phenomenological Aspects of Underground Physics, Toledo (Spain) September

Fourth International Workshop on Theoretical and Phenomenological Aspects of Underground Physics, Toledo (Spain) September Fourth International Workshop on Theoretical and Phenomenological Aspects of Underground Physics, Toledo (Spain) September 17-21 1995 COSMOLOGICAL IMPLICATIONS OF A POSSIBLE CLASS OF PARTICLES ABLE TO

More information

The Quantum Spacetime

The Quantum Spacetime The Quantum Spacetime Juan Maldacena School of Natural Sciences, Institute for Advanced Study, Princeton, NJ, USA. Abstract Rapporteur talk at the 2011 Solvay Conference 1 Opening It is a great pleasure

More information

No Fine theorem for macroscopic realism

No Fine theorem for macroscopic realism No Fine theorem for macroscopic realism Johannes Kofler Max Planck Institute of Quantum Optics (MPQ) Garching/Munich, Germany 2nd International Conference on Quantum Foundations Patna, India 17 Oct. 2016

More information

Gravity, Strings and Branes

Gravity, Strings and Branes Gravity, Strings and Branes Joaquim Gomis International Francqui Chair Inaugural Lecture Leuven, 11 February 2005 Fundamental Forces Strong Weak Electromagnetism QCD Electroweak SM Gravity Standard Model

More information

Lifting General Relativity to Observer Space

Lifting General Relativity to Observer Space Lifting General Relativity to Observer Space Derek Wise Institute for Quantum Gravity University of Erlangen Work with Steffen Gielen: 1111.7195 1206.0658 1210.0019 International Loop Quantum Gravity Seminar

More information

Shape dynamics and Mach s principles: Gravity from conformal geometrodynamics

Shape dynamics and Mach s principles: Gravity from conformal geometrodynamics arxiv:1204.0683v1 [gr-qc] 3 Apr 2012 Shape dynamics and Mach s principles: Gravity from conformal geometrodynamics by Sean Gryb A thesis presented to the University of Waterloo in fulfillment of the thesis

More information

No Fine Theorem for Macrorealism

No Fine Theorem for Macrorealism No Fine Theorem for Macrorealism Johannes Kofler Max Planck Institute of Quantum Optics (MPQ) Garching/Munich, Germany Quantum and Beyond Linnaeus University, Växjö, Sweden 14 June 2016 Acknowledgments

More information

Synchronization of thermal Clocks and entropic Corrections of Gravity

Synchronization of thermal Clocks and entropic Corrections of Gravity Synchronization of thermal Clocks and entropic Corrections of Gravity Andreas Schlatter Burghaldeweg 2F, 5024 Küttigen, Switzerland schlatter.a@bluewin.ch Abstract There are so called MOND corrections

More information

Review and Notation (Special relativity)

Review and Notation (Special relativity) Review and Notation (Special relativity) December 30, 2016 7:35 PM Special Relativity: i) The principle of special relativity: The laws of physics must be the same in any inertial reference frame. In particular,

More information

On the origin of probability in quantum mechanics

On the origin of probability in quantum mechanics On the origin of probability in quantum mechanics Steve Hsu Benasque, September 2010 Outline 1. No Collapse quantum mechanics 2. Does the Born rule (probabilities) emerge? 3. Possible resolutions R. Buniy,

More information

Holographic renormalization and reconstruction of space-time. Kostas Skenderis Southampton Theory Astrophysics and Gravity research centre

Holographic renormalization and reconstruction of space-time. Kostas Skenderis Southampton Theory Astrophysics and Gravity research centre Holographic renormalization and reconstruction of space-time Southampton Theory Astrophysics and Gravity research centre STAG CH RESEARCH ER C TE CENTER Holographic Renormalization and Entanglement Paris,

More information

Einstein Toolkit Workshop. Joshua Faber Apr

Einstein Toolkit Workshop. Joshua Faber Apr Einstein Toolkit Workshop Joshua Faber Apr 05 2012 Outline Space, time, and special relativity The metric tensor and geometry Curvature Geodesics Einstein s equations The Stress-energy tensor 3+1 formalisms

More information

EPR Paradox and Bell s Inequality

EPR Paradox and Bell s Inequality EPR Paradox and Bell s Inequality James Cross 2018-08-18 1 Introduction The field of quantum mechanics is practically synonymous with modern physics. The basics of quantum theory are taught in every introductory

More information

Classical aspects of Poincaré gauge theory of gravity

Classical aspects of Poincaré gauge theory of gravity Classical aspects of Poincaré gauge theory of gravity Jens Boos jboos@perimeterinstitute.ca Perimeter Institute for Theoretical Physics Wednesday, Nov 11, 2015 Quantum Gravity group meeting Perimeter Institute

More information

Intrinsic time quantum geometrodynamics: The. emergence of General ILQGS: 09/12/17. Eyo Eyo Ita III

Intrinsic time quantum geometrodynamics: The. emergence of General ILQGS: 09/12/17. Eyo Eyo Ita III Intrinsic time quantum geometrodynamics: The Assistant Professor Eyo Ita emergence of General Physics Department Relativity and cosmic time. United States Naval Academy ILQGS: 09/12/17 Annapolis, MD Eyo

More information

The subquantum arrow of time

The subquantum arrow of time The subquantum arrow of time Theo M. Nieuwenhuizen University of Amsterdam Emergent Quantum Mechanics 2013, EmQM13, Vienna To understand Nature we have become accustomed to inconceivable concepts Our task

More information

Cosmology with group field theory condensates

Cosmology with group field theory condensates Steffen Gielen Imperial College London 24 February 2015 Main collaborators: Daniele Oriti, Lorenzo Sindoni (AEI) Work in progress with M. Sakellariadou, A. Pithis, M. de Cesare (KCL) Supported by the FP7

More information

ENTER RELATIVITY THE HELIOCENTRISM VS GEOCENTRISM DEBATE ARISES FROM MATTER OF CHOOSING THE BEST REFERENCE POINT. GALILEAN TRANSFORMATION 8/19/2016

ENTER RELATIVITY THE HELIOCENTRISM VS GEOCENTRISM DEBATE ARISES FROM MATTER OF CHOOSING THE BEST REFERENCE POINT. GALILEAN TRANSFORMATION 8/19/2016 ENTER RELATIVITY RVBAUTISTA THE HELIOCENTRISM VS GEOCENTRISM DEBATE ARISES FROM MATTER OF CHOOSING THE BEST REFERENCE POINT. GALILEAN TRANSFORMATION The laws of mechanics must be the same in all inertial

More information

Gravity as Machian Shape Dynamics

Gravity as Machian Shape Dynamics Gravity as Machian Shape Dynamics Julian Barbour Alternative Title: Was Spacetime a Glorious Historical Accident? Time will not be fused with space but emerge from the timeless shape dynamics of space.

More information

Black Holes, Holography, and Quantum Information

Black Holes, Holography, and Quantum Information Black Holes, Holography, and Quantum Information Daniel Harlow Massachusetts Institute of Technology August 31, 2017 1 Black Holes Black holes are the most extreme objects we see in nature! Classically

More information

Lagrangian Description for Particle Interpretations of Quantum Mechanics Single-Particle Case

Lagrangian Description for Particle Interpretations of Quantum Mechanics Single-Particle Case Lagrangian Description for Particle Interpretations of Quantum Mechanics Single-Particle Case Roderick I. Sutherland Centre for Time, University of Sydney, NSW 26 Australia rod.sutherland@sydney.edu.au

More information

Quantum theory without predefined causal structure

Quantum theory without predefined causal structure Quantum theory without predefined causal structure Ognyan Oreshkov Centre for Quantum Information and Communication, niversité Libre de Bruxelles Based on work with Caslav Brukner, Nicolas Cerf, Fabio

More information

Zhong-Zhi Xianyu (CMSA Harvard) Tsinghua June 30, 2016

Zhong-Zhi Xianyu (CMSA Harvard) Tsinghua June 30, 2016 Zhong-Zhi Xianyu (CMSA Harvard) Tsinghua June 30, 2016 We are directly observing the history of the universe as we look deeply into the sky. JUN 30, 2016 ZZXianyu (CMSA) 2 At ~10 4 yrs the universe becomes

More information

Pedro and the WOLF: the quantum and the vacuum in cosmology

Pedro and the WOLF: the quantum and the vacuum in cosmology Pedro's Universes, 4 December 2018 Guillermo A. Mena Marugán, IEM-CSIC Pedro and the WOLF: the quantum and the vacuum in cosmology Pedro's Universes, 4 December 2018 Guillermo A. Mena Marugán, IEM-CSIC

More information

Lecture notes 1. Standard physics vs. new physics. 1.1 The final state boundary condition

Lecture notes 1. Standard physics vs. new physics. 1.1 The final state boundary condition Lecture notes 1 Standard physics vs. new physics The black hole information paradox has challenged our fundamental beliefs about spacetime and quantum theory. Which belief will have to change to resolve

More information

Quotations from other works that I have written

Quotations from other works that I have written Quotations from other works that I have written (Including supporting documentation from other sources) The following five groups of quotations are in numerical order of what I consider to be of the greatest

More information

Quantum interferometric visibility as a witness of general relativistic proper time. M. Zych, F. Costa, I. Pikovski, Č. Brukner

Quantum interferometric visibility as a witness of general relativistic proper time. M. Zych, F. Costa, I. Pikovski, Č. Brukner Quantum interferometric visibility as a witness of general relativistic proper time M. Zych, F. Costa, I. Pikovski, Č. Brukner Bhubaneswar, 21st December 2011 Interpretation ambiguity of gravitationally

More information

Duality and Emergent Gravity in AdS/CFT

Duality and Emergent Gravity in AdS/CFT Duality and Emergent Gravity in AdS/CFT Sebastian de Haro University of Amsterdam and University of Cambridge Equivalent Theories in Science and Metaphysics Princeton, 21 March 2015 Motivating thoughts

More information

Scale symmetry a link from quantum gravity to cosmology

Scale symmetry a link from quantum gravity to cosmology Scale symmetry a link from quantum gravity to cosmology scale symmetry fluctuations induce running couplings violation of scale symmetry well known in QCD or standard model Fixed Points Quantum scale symmetry

More information

Stellar Black Holes, and the thermodynamic origin of Cosmic Acceleration

Stellar Black Holes, and the thermodynamic origin of Cosmic Acceleration Astrophysics Seminar Institut d Astrophysique de Paris Feb. 19, 2010 Stellar Black Holes, and the thermodynamic origin of Cosmic Acceleration Niayesh Afshordi 2/35 Outline Introduction Reviving Aether

More information

Antonio L. Maroto Complutense University Madrid Modern Cosmology: Early Universe, CMB and LSS Benasque, August 3-16, 2014

Antonio L. Maroto Complutense University Madrid Modern Cosmology: Early Universe, CMB and LSS Benasque, August 3-16, 2014 Antonio L. Maroto Complutense University Madrid Modern Cosmology: Early Universe, CMB and LSS Benasque, August 3-16, 2014 A.L.M and F. Prada to appear Albareti, Cembranos, A.L.M. arxiv:1404.5946 and 1405.3900

More information

Cosmic Censorship Conjecture and Topological Censorship

Cosmic Censorship Conjecture and Topological Censorship Cosmic Censorship Conjecture and Topological Censorship 21 settembre 2009 Cosmic Censorship Conjecture 40 years ago in the Rivista Nuovo Cimento Sir Roger Penrose posed one of most important unsolved problems

More information

The Causal Set Approach to Quantum Gravity

The Causal Set Approach to Quantum Gravity Department of Physics The Causal Set Approach to Quantum Gravity Author: Yichao Hu Supervisor: Prof. Fay Dowker September 2013 Submitted in partial fulfilment of the requirements for the degree of Master

More information

Workshop on Testing Fundamental Physics Principles Corfu, September 22-28, 2017.

Workshop on Testing Fundamental Physics Principles Corfu, September 22-28, 2017. Workshop on Testing Fundamental Physics Principles Corfu, September 22-28, 2017.. Observables and Dispersion Relations in κ-minkowski and κ-frw noncommutative spacetimes Paolo Aschieri Università del Piemonte

More information

Closing the Debates on Quantum Locality and Reality: EPR Theorem, Bell's Theorem, and Quantum Information from the Brown-Twiss Vantage

Closing the Debates on Quantum Locality and Reality: EPR Theorem, Bell's Theorem, and Quantum Information from the Brown-Twiss Vantage Closing the Debates on Quantum Locality and Reality: EPR Theorem, Bell's Theorem, and Quantum Information from the Brown-Twiss Vantage C. S. Unnikrishnan Fundamental Interactions Laboratory Tata Institute

More information

The Two-State Vector Formalism

The Two-State Vector Formalism arxiv:0706.1347v1 [quant-ph] 10 Jun 007 The Two-State Vector Formalism February 1, 013 The two-state vector formalism (TSVF) [1] is a time-symmetric description of the standard quantum mechanics originated

More information

Quantum Mechanics without Spacetime II

Quantum Mechanics without Spacetime II Quantum Mechanics without Spacetime II - Noncommutative geometry and the free point particle - T. P. Singh Tata Institute of Fundamental Research Homi Bhabha Road, Mumbai 400 005, India email address:

More information

AdS/CFT duality. Agnese Bissi. March 26, Fundamental Problems in Quantum Physics Erice. Mathematical Institute University of Oxford

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

More information

TOWARD AN OBJECTIVE PRINCIPLE FOR

TOWARD AN OBJECTIVE PRINCIPLE FOR TOWARD AN OBJECTIVE PRINCIPLE FOR DECOMPOSING THE WAVEFUNCTION INTO CLASSICAL BRANCHES C. Jess Riedel (Perimeter Institute) with Charles Bennett, Wojciech Zurek, and Michael Zwolak MIT 5 December 2014

More information

Gauge invariant quantum gravitational decoherence

Gauge invariant quantum gravitational decoherence Gauge invariant quantum gravitational decoherence Teodora Oniga Department of Physics, University of Aberdeen BritGrav 15, Birmingham, 21 April 2015 Outline Open quantum systems have so far been successfully

More information

Aspects of Spontaneous Lorentz Violation

Aspects of Spontaneous Lorentz Violation Aspects of Spontaneous Lorentz Violation Robert Bluhm Colby College IUCSS School on CPT & Lorentz Violating SME, Indiana University, June 2012 Outline: I. Review & Motivations II. Spontaneous Lorentz Violation

More information

The Erlangen Program and General Relativity

The Erlangen Program and General Relativity The Erlangen Program and General Relativity Derek K. Wise University of Erlangen Department of Mathematics & Institute for Quantum Gravity Colloquium, Utah State University January 2014 What is geometry?

More information

arxiv:gr-qc/ v1 1 Dec 2004

arxiv:gr-qc/ v1 1 Dec 2004 Physics of Deformed Special Relativity: Relativity Principle revisited Florian Girelli, Etera R. Livine Perimeter Institute, 31 Caroline Street North Waterloo, Ontario Canada N2L 2Y5 arxiv:gr-qc/0412004

More information