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Symmetry and Gravity
universe Article Making a Quantum Universe: Symmetry and Gravity Houri Ziaeepour 1,2 1 Institut UTINAM, CNRS UMR 6213, Observatoire de Besançon, Université de Franche Compté, 41 bis ave. de l’Observatoire, BP 1615, 25010 Besançon, France; [email protected] or [email protected] 2 Mullard Space Science Laboratory, University College London, Holmbury St. Mary, Dorking GU5 6NT, UK Received: 05 September 2020; Accepted: 17 October 2020; Published: 23 October 2020 Abstract: So far, none of attempts to quantize gravity has led to a satisfactory model that not only describe gravity in the realm of a quantum world, but also its relation to elementary particles and other fundamental forces. Here, we outline the preliminary results for a model of quantum universe, in which gravity is fundamentally and by construction quantic. The model is based on three well motivated assumptions with compelling observational and theoretical evidence: quantum mechanics is valid at all scales; quantum systems are described by their symmetries; universe has infinite independent degrees of freedom. The last assumption means that the Hilbert space of the Universe has SUpN Ñ 8q – area preserving Diff.pS2q symmetry, which is parameterized by two angular variables. We show that, in the absence of a background spacetime, this Universe is trivial and static. Nonetheless, quantum fluctuations break the symmetry and divide the Universe to subsystems. When a subsystem is singled out as reference—observer—and another as clock, two more continuous parameters arise, which can be interpreted as distance and time. We identify the classical spacetime with parameter space of the Hilbert space of the Universe. -
Jhep09(2019)100
Published for SISSA by Springer Received: July 29, 2019 Accepted: September 5, 2019 Published: September 12, 2019 A link that matters: towards phenomenological tests of unimodular asymptotic safety JHEP09(2019)100 Gustavo P. de Brito,a;b Astrid Eichhornc;b and Antonio D. Pereirad;b aCentro Brasileiro de Pesquisas F´ısicas (CBPF), Rua Dr Xavier Sigaud 150, Urca, Rio de Janeiro, RJ, Brazil, CEP 22290-180 bInstitute for Theoretical Physics, University of Heidelberg, Philosophenweg 16, 69120 Heidelberg, Germany cCP3-Origins, University of Southern Denmark, Campusvej 55, DK-5230 Odense M, Denmark dInstituto de F´ısica, Universidade Federal Fluminense, Campus da Praia Vermelha, Av. Litor^anea s/n, 24210-346, Niter´oi,RJ, Brazil E-mail: [email protected], [email protected], [email protected] Abstract: Constraining quantum gravity from observations is a challenge. We expand on the idea that the interplay of quantum gravity with matter could be key to meeting this challenge. Thus, we set out to confront different potential candidates for quantum gravity | unimodular asymptotic safety, Weyl-squared gravity and asymptotically safe gravity | with constraints arising from demanding an ultraviolet complete Standard Model. Specif- ically, we show that within approximations, demanding that quantum gravity solves the Landau-pole problems in Abelian gauge couplings and Yukawa couplings strongly con- strains the viable gravitational parameter space. In the case of Weyl-squared gravity with a dimensionless gravitational coupling, we also investigate whether the gravitational con- tribution to beta functions in the matter sector calculated from functional Renormalization Group techniques is universal, by studying the dependence on the regulator, metric field parameterization and choice of gauge. -
Variational Problem and Bigravity Nature of Modified Teleparallel Theories
Variational Problem and Bigravity Nature of Modified Teleparallel Theories Martin Krˇsˇs´ak∗ Institute of Physics, University of Tartu, W. Ostwaldi 1, Tartu 50411, Estonia August 15, 2017 Abstract We consider the variational principle in the covariant formulation of modified telepar- allel theories with second order field equations. We vary the action with respect to the spin connection and obtain a consistency condition relating the spin connection with the tetrad. We argue that since the spin connection can be calculated using an additional reference tetrad, modified teleparallel theories can be interpreted as effectively bigravity theories. We conclude with discussion about the relation of our results and those obtained in the usual, non-covariant, formulation of teleparallel theories and present the solution to the problem of choosing the tetrad in f(T ) gravity theories. 1 Introduction Teleparallel gravity is an alternative formulation of general relativity that can be traced back to Einstein’s attempt to formulate the unified field theory [1–9]. Over the last decade, various modifications of teleparallel gravity became a popular tool to address the problem of the accelerated expansion of the Universe without invoking the dark sector [10–38]. The attractiveness of modifying teleparallel gravity–rather than the usual general relativity–lies in the fact that we obtain an entirely new class of modified gravity theories, which have second arXiv:1705.01072v3 [gr-qc] 13 Aug 2017 order field equations. See [39] for the extensive review. A well-known shortcoming of the original formulation of teleparallel theories is the prob- lem of local Lorentz symmetry violation [40, 41]. -
On the Axioms of Causal Set Theory
On the Axioms of Causal Set Theory Benjamin F. Dribus Louisiana State University [email protected] November 8, 2013 Abstract Causal set theory is a promising attempt to model fundamental spacetime structure in a discrete order-theoretic context via sets equipped with special binary relations, called causal sets. The el- ements of a causal set are taken to represent spacetime events, while its binary relation is taken to encode causal relations between pairs of events. Causal set theory was introduced in 1987 by Bombelli, Lee, Meyer, and Sorkin, motivated by results of Hawking and Malament relating the causal, conformal, and metric structures of relativistic spacetime, together with earlier work on discrete causal theory by Finkelstein, Myrheim, and 't Hooft. Sorkin has coined the phrase, \order plus number equals geometry," to summarize the causal set viewpoint regarding the roles of causal structure and discreteness in the emergence of spacetime geometry. This phrase represents a specific version of what I refer to as the causal metric hypothesis, which is the idea that the properties of the physical universe, and in particular, the metric properties of classical spacetime, arise from causal structure at the fundamental scale. Causal set theory may be expressed in terms of six axioms: the binary axiom, the measure axiom, countability, transitivity, interval finiteness, and irreflexivity. The first three axioms, which fix the physical interpretation of a causal set, and restrict its \size," appear in the literature either implic- itly, or as part of the preliminary definition of a causal set. The last three axioms, which encode the essential mathematical structure of a causal set, appear in the literature as the irreflexive formula- tion of causal set theory. -
Non-Inflationary Bianchi Type VI0 Model in Rosen's Bimetric Gravity
Applications and Applied Mathematics: An International Journal (AAM) Volume 11 Issue 2 Article 25 12-2016 Non-Inflationary Bianchi Type VI0 Model in Rosen’s Bimetric Gravity M. S. Borkar R. T. M. Nagpur University N. P. Gaikwad Dharampeth M. P. Deo Memorial Science College Follow this and additional works at: https://digitalcommons.pvamu.edu/aam Part of the Other Physics Commons Recommended Citation Borkar, M. S. and Gaikwad, N. P. (2016). Non-Inflationary Bianchi Type VI0 Model in Rosen’s Bimetric Gravity, Applications and Applied Mathematics: An International Journal (AAM), Vol. 11, Iss. 2, Article 25. Available at: https://digitalcommons.pvamu.edu/aam/vol11/iss2/25 This Article is brought to you for free and open access by Digital Commons @PVAMU. It has been accepted for inclusion in Applications and Applied Mathematics: An International Journal (AAM) by an authorized editor of Digital Commons @PVAMU. For more information, please contact [email protected]. Borkar and Gaikwad: Bianchi Type VI0 Model in Rosen’s Bimetric Gravity Available at http://pvamu.edu/aam Applications and Applied Appl. Appl. Math. Mathematics: ISSN: 1932-9466 An International Journal (AAM) Vol. 11, Issue 2 (December 2016), pp. 875 - 887 Non-Inflationary Bianchi Type VI0 Model in Rosen’s Bimetric Gravity M. S. Borkar1 and N. P. Gaikwad2 1Post Graduate Department of Mathematics R. T. M. Nagpur University Nagpur – 440 033, India E–mail : [email protected] 2Department of Mathematics Dharampeth M. P. Deo Memorial Science College Nagpur – 440 033, India E-mail : [email protected] Received: March 19, 2015; Accepted: July 7, 2016 Abstract In this paper, we have present the solution of Bianchi type VI0 space-time by solving the Rosen’s field equations with massless scalar field and with constant scalar potential V for flat region. -
Analytical Constraints on Bimetric Gravity
Prepared for submission to JCAP Analytical constraints on bimetric gravity Marcus H¨og˚as,Edvard M¨ortsell The Oskar Klein Centre, Department of Physics, Stockholm University, SE 106 91, Stock- holm, Sweden E-mail: [email protected], [email protected] Abstract. Ghost-free bimetric gravity is an extension of general relativity, featuring a mas- sive spin-2 field coupled to gravity. We parameterize the theory with a set of observables having specific physical interpretations. For the background cosmology and the static, spher- ically symmetric solutions (for example approximating the gravitational potential of the solar system), there are four directions in the parameter space in which general relativity is ap- proached. Requiring that there is a working screening mechanism and a nonsingular evolution of the Universe, we place analytical constraints on the parameter space which rule out many of the models studied in the literature. Cosmological solutions where the accelerated expan- sion of the Universe is explained by the dynamical interaction of the massive spin-2 field rather than by a cosmological constant, are still viable. arXiv:2101.08794v2 [gr-qc] 10 May 2021 Contents 1 Introduction and summary1 2 Bimetric gravity3 3 Physical parameterization4 4 Local solutions6 4.1 Linearized solutions6 4.2 Vainsthein screening8 5 Background cosmology 11 5.1 Infinite branch (inconsistent) 13 5.2 Finite branch (consistent) 13 6 General relativity limits 15 6.1 Local solutions 15 6.2 Background cosmology 16 7 Constraints on the physical parameters 19 7.1 Local solutions 19 7.2 Background cosmology 20 8 Discussion and outlook 23 A List of constraints 25 B The St¨uckelberg field 26 C Constraints from the dynamical Higuchi bound 26 D Expansions 28 D.1 Around the final de Sitter point 28 D.2 mFP ! 1 limit 29 D.3 α ! 1 limit 30 D.4 β ! 1 limit 31 E Avoiding the Big Rip 32 1 Introduction and summary There are strong motivations to look for new theories of gravity, for example the unknown nature of dark matter and dark energy. -
The Multiple Realizability of General Relativity in Quantum Gravity
The multiple realizability of general relativity in quantum gravity Rasmus Jaksland∗ Forthcoming in Synthese† Abstract Must a theory of quantum gravity have some truth to it if it can recover general rela- tivity in some limit of the theory? This paper answers this question in the negative by indicating that general relativity is multiply realizable in quantum gravity. The argu- ment is inspired by spacetime functionalism – multiple realizability being a central tenet of functionalism – and proceeds via three case studies: induced gravity, thermodynamic gravity, and entanglement gravity. In these, general relativity in the form of the Ein- stein field equations can be recovered from elements that are either manifestly multiply realizable or at least of the generic nature that is suggestive of functions. If general relativity, as argued here, can inherit this multiple realizability, then a theory of quantum gravity can recover general relativity while being completely wrong about the posited microstructure. As a consequence, the recovery of general relativity cannot serve as the ultimate arbiter that decides which theory of quantum gravity that is worthy of pursuit, even though it is of course not irrelevant either qua quantum gravity. Thus, the recovery of general relativity in string theory, for instance, does not guarantee that the stringy account of the world is on the right track; despite sentiments to the contrary among string theorists. Keywords quantum gravity, general relativity, spacetime functionalism, entanglement, emergent gravity, multiple realizability, string theory ∗Department of Philosophy and Religious Studies, NTNU – Norwegian University of Science and Technology, Trondheim, Norway. Email: [email protected] †This is a post-peer-review, pre-copyedit version of an article published in Synthese. -
Cosmology Beyond Einstein Essay
Adam R. Solomon Department of Physics, 5000 Forbes Avenue, Pittsburgh, PA 15213 email: [email protected] web: http://andrew.cmu.edu/~adamsolo/ RESEARCH INTERESTS Theoretical cosmology: dark energy, dark matter, inflation, baryogenesis; field theory; modified gravity; cosmological tests. EMPLOYMENT HISTORY Sep. 2018- Carnegie Mellon University present Postdoctoral Research Associate Department of Physics and McWilliams Center for Cosmology Sep. 2015- University of Pennsylvania Aug. 2018 Postdoctoral Fellow Center for Particle Cosmology Apr. 2015- University of Heidelberg Jul. 2015 DAAD Visiting Fellow Institute for Theoretical Physics Dec. 2014- University of Cambridge Feb. 2015 Research Assistant Department of Applied Mathematics and Theoretical Physics EDUCATION 2011-2015 University of Cambridge – Ph.D. Department of Applied Mathematics and Theoretical Physics Thesis: Cosmology Beyond Einstein Supervisor: Prof. John D. Barrow 2010-2011 University of Cambridge – Master of Advanced Study in Mathematics Part III of the Mathematical Tripos (Distinction) Essay: Probing the Very Early Universe with the Stochastic Gravitational Wave Background Supervisors: Prof. Paul Shellard, Dr. Eugene Lim 2006-2010 Yale University – B.S. in Astronomy and Physics Thesis: The Sunyaev-Zel’dovich Effect in the Wilkinson Microwave Anisotropy Probe Data Supervisors: Prof. Daisuke Nagai, Dr. Suchetana Chatterjee PUBLICATIONS AND CONFERENCE PROCEEDINGS 1. Khoury, J., Sakstein, J., & Solomon, A. R., “Superfluids and the Cosmological Constant Problem.” 2018, JCAP08(2018)024, arXiv:1805.05937 2. Solomon, A. R. & Trodden, M., “Higher-derivative operators and effective field theory for general scalar-tensor theories.” 2017, JCAP02(2018)031, arXiv:1709.09695 3. Sakstein, J. & Solomon, A. R., “Baryogenesis in Lorentz-violating gravity theories.” 2017, Phys. Lett. B 773, 186, arXiv:1705.10695 4. -
Redalyc.Big Extra Dimensions Make a Too Small
Brazilian Journal of Physics ISSN: 0103-9733 [email protected] Sociedade Brasileira de Física Brasil Sorkin, Rafael D. Big extra dimensions make A too Small Brazilian Journal of Physics, vol. 35, núm. 2A, june, 2005, pp. 280-283 Sociedade Brasileira de Física Sâo Paulo, Brasil Available in: http://www.redalyc.org/articulo.oa?id=46435212 How to cite Complete issue Scientific Information System More information about this article Network of Scientific Journals from Latin America, the Caribbean, Spain and Portugal Journal's homepage in redalyc.org Non-profit academic project, developed under the open access initiative 280 Brazilian Journal of Physics, vol. 35, no. 2A, June, 2005 Big Extra Dimensions Make L too Small Rafael D. Sorkin Perimeter Institute, 31 Caroline Street North, Waterloo ON, N2L 2Y5 Canada and Department of Physics, Syracuse University, Syracuse, NY 13244-1130, U.S.A. Received on 23 February, 2005 I argue that the true quantum gravity scale cannot be much larger than the Planck length, because if it were then the quantum gravity-induced fluctuations in L would be insufficient to produce the observed cosmic “dark energy”. If one accepts this argument, it rules out scenarios of the “large extra dimensions” type. I also point out that the relation between the lower and higher dimensional gravitational constants in a Kaluza-Klein theory is precisely what is needed in order that a black hole’s entropy admit a consistent higher dimensional interpretation in terms of an underlying spatio-temporal discreteness. Probably few people anticipate that laboratory experiments in L far too small to be compatible with its observed value. -
Manifoldlike Causal Sets
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by eGrove (Univ. of Mississippi) University of Mississippi eGrove Electronic Theses and Dissertations Graduate School 2019 Manifoldlike Causal Sets Miremad Aghili University of Mississippi Follow this and additional works at: https://egrove.olemiss.edu/etd Part of the Physics Commons Recommended Citation Aghili, Miremad, "Manifoldlike Causal Sets" (2019). Electronic Theses and Dissertations. 1529. https://egrove.olemiss.edu/etd/1529 This Dissertation is brought to you for free and open access by the Graduate School at eGrove. It has been accepted for inclusion in Electronic Theses and Dissertations by an authorized administrator of eGrove. For more information, please contact [email protected]. Manifoldlike Causal Sets A Dissertation presented in partial fulfillment of requirements for the degree of Doctor of Philosophy in the Department of Physics and Astronomy The University of Mississippi by Miremad Aghili May 2019 Copyright Miremad Aghili 2019 ALL RIGHTS RESERVED ABSTRACT The content of this dissertation is written in a way to answer the important question of manifoldlikeness of causal sets. This problem has importance in the sense that in the continuum limit and in the case one finds a formalism for the sum over histories, the result requires to be embeddable in a manifold to be able to reproduce General Relativity. In what follows I will use the distribution of path length in a causal set to assign a measure for manifoldlikeness of causal sets to eliminate the dominance of nonmanifoldlike causal sets. The distribution of interval sizes is also investigated as a way to find the discrete version of scalar curvature in causal sets in order to present a dynamics of gravitational fields. -
Dimension and Dimensional Reduction in Quantum Gravity
March 2019 Dimension and Dimensional Reduction in Quantum Gravity S. Carlip∗ Department of Physics University of California Davis, CA 95616 USA Abstract If gravity is asymptotically safe, operators will exhibit anomalous scaling at the ultraviolet fixed point in a way that makes the theory effectively two- dimensional. A number of independent lines of evidence, based on different approaches to quantization, indicate a similar short-distance dimensional reduction. I will review the evidence for this behavior, emphasizing the physical question of what one means by “dimension” in a quantum spacetime, and will dis- cuss possible mechanisms that could explain the universality of this phenomenon. For proceedings of the conference in honor of Martin Reuter: “Quantum Fields—From Fundamental Concepts to Phenomenological Questions” September 2018 arXiv:1904.04379v1 [gr-qc] 8 Apr 2019 ∗email: [email protected] 1. Introduction The asymptotic safety program offers a fascinating possibility for the quantization of gravity, starkly different from other, more common approaches, such as string theory and loop quantum gravity [1–3]. We don’t know whether quantum gravity can be described by an asymptotically safe (and unitary) field theory, but it might be. For “traditionalists” working on quantum gravity, this raises a fundamental question: What does asymptotic safety tell us about the small-scale structure of spacetime? So far, the most intriguing answer to this question involves the phenomenon of short-distance dimensional reduction. It seems nearly certain that, near a nontrivial ultraviolet fixed point, operators acquire large anomalous dimensions, in such a way that their effective dimensions are those of operators in a two-dimensional spacetime [4–6]. -
Arxiv:Gr-Qc/9510063V1 31 Oct 1995
STRUCTURAL ISSUES IN QUANTUM GRAVITYa C.J. Isham b Blackett Laboratory, Imperial College of Science, Technology and Medicine, South Kensington, London SW7 2BZ A discursive, non-technical, analysis is made of some of the basic issues that arise in almost any approach to quantum gravity, and of how these issues stand in relation to recent developments in the field. Specific topics include the applicability of the conceptual and mathematical structures of both classical general relativity and standard quantum theory. This discussion is preceded by a short history of the last twenty-five years of research in quantum gravity, and concludes with speculations on what a future theory might look like. 1 Introduction 1.1 Some Crucial Questions in Quantum Gravity In this lecture I wish to reflect on certain fundamental issues that can be expected to arise in almost all approaches to quantum gravity. As such, the talk is rather non-mathematical in nature—in particular, it is not meant to be a technical review of the who-has-been-doing-what-since-GR13 type: the subject has developed in too many different ways in recent years to make this option either feasible or desirable. The presentation is focussed around the following prima facie questions: 1. Why are we interested in quantum gravity at all? In the past, different researchers have had significantly different motivations for their work— and this has had a strong influence on the technical developments of the subject. arXiv:gr-qc/9510063v1 31 Oct 1995 2. What are the basic ways of trying to construct a quantum theory of gravity? For example, can general relativity be regarded as ‘just another field theory’ to be quantised in a more-or-less standard way, or does its basic structure demand something quite different? 3.