Cosmology of Brane Universes and Brane Gases
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Symmetries of String Theory and Early Universe Cosmology
String Cosmology R. Branden- berger Introduction Symmetries of String Theory and Early T-Duality: Key Symmetry of Universe Cosmology String Theory String Gas Cosmology Structure Robert Brandenberger Perturbations Overview Physics Department, McGill University Analysis DFT Conclusions Yukawa Institute, Kyoto University, Feb. 26, 2018 1 / 61 Outline String Cosmology 1 Introduction R. Branden- berger 2 T-Duality: Key Symmetry of String Theory Introduction T-Duality: Key 3 String Gas Cosmology Symmetry of String Theory String Gas 4 String Gas Cosmology and Structure Formation Cosmology Review of the Theory of Cosmological Perturbations Structure Perturbations Overview Overview Analysis Analysis DFT 5 Double Field Theory as a Background for String Gas Conclusions Cosmology 6 Conclusions 2 / 61 Plan String Cosmology 1 Introduction R. Branden- berger 2 T-Duality: Key Symmetry of String Theory Introduction T-Duality: Key 3 String Gas Cosmology Symmetry of String Theory String Gas 4 String Gas Cosmology and Structure Formation Cosmology Review of the Theory of Cosmological Perturbations Structure Perturbations Overview Overview Analysis Analysis DFT 5 Double Field Theory as a Background for String Gas Conclusions Cosmology 6 Conclusions 3 / 61 Inflation: the Standard Model of Early Universe Cosmology String Cosmology R. Branden- berger Introduction Inflation is the standard paradigm of early universe T-Duality: Key cosmology. Symmetry of String Theory Inflation solves conceptual problems of Standard Big String Gas Bang Cosmology. Cosmology Structure Inflation predicts an almost scale-invariant spectrum of Perturbations Overview primordial cosmological perturbations with a small red Analysis tilt (Chibisov & Mukhanov, 1981). DFT Conclusions Fluctuations are nearly Gaussian and nearly adiabatic. 4 / 61 Map of the Cosmic Microwave Background (CMB) String Cosmology R. -
Off-Shell Interactions for Closed-String Tachyons
Preprint typeset in JHEP style - PAPER VERSION hep-th/0403238 KIAS-P04017 SLAC-PUB-10384 SU-ITP-04-11 TIFR-04-04 Off-Shell Interactions for Closed-String Tachyons Atish Dabholkarb,c,d, Ashik Iqubald and Joris Raeymaekersa aSchool of Physics, Korea Institute for Advanced Study, 207-43, Cheongryangri-Dong, Dongdaemun-Gu, Seoul 130-722, Korea bStanford Linear Accelerator Center, Stanford University, Stanford, CA 94025, USA cInstitute for Theoretical Physics, Department of Physics, Stanford University, Stanford, CA 94305, USA dDepartment of Theoretical Physics, Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai 400005, India E-mail:[email protected], [email protected], [email protected] Abstract: Off-shell interactions for localized closed-string tachyons in C/ZN super- string backgrounds are analyzed and a conjecture for the effective height of the tachyon potential is elaborated. At large N, some of the relevant tachyons are nearly massless and their interactions can be deduced from the S-matrix. The cubic interactions be- tween these tachyons and the massless fields are computed in a closed form using orbifold CFT techniques. The cubic interaction between nearly-massless tachyons with different charges is shown to vanish and thus condensation of one tachyon does not source the others. It is shown that to leading order in N, the quartic contact in- teraction vanishes and the massless exchanges completely account for the four point scattering amplitude. This indicates that it is necessary to go beyond quartic inter- actions or to include other fields to test the conjecture for the height of the tachyon potential. Keywords: closed-string tachyons, orbifolds. -
Arxiv:Astro-Ph/0402129V2 21 Sep 2004 Abstract
Cosmological Perturbation Theory Ruth Durrer Universit´ede Gen`eve, D´epartement de Physique Th´eorique, 24 Quai E. Ansermet, CH–1211 Gen`eve, Switzerland [email protected] Abstract. This is a review on cosmological perturbation theory. After an intro- duction, it presents the problem of gauge transformation. Gauge invariant variables are introduced and the Einstein and conservation equations are written in terms of these variables. Some examples, especially perfect fluids and scalar fields are pre- sented in detail. The generation of perturbations during inflation is studied. Lightlike geodesics and their relevance for CMB anisotropies are briefly discussed. Perturba- tion theory in braneworlds is also introduced. February 5, 2004 arXiv:astro-ph/0402129v2 21 Sep 2004 2 Ruth Durrer 1 Introduction The idea that the large scale structure of our Universe might have grown our of small initial fluctuations via gravitational instability goes back to Newton (letter to Bentley, 1692[1]). The first relativistic treatment of linear perturbations in a Friedmann- Lemaˆıtre universe was given by Lifshitz (1946)[2]. There He found that the gravitational potential cannot grow within linear perturbation theory and he concluded that galaxies have not formed by gravitational instability. Today we know that it is sufficient that matter density fluctuations can grow. Nevertheless, considerable initial fluctuations with amplitudes of the 5 order of 10− are needed in order to reproduce the cosmic structures observed today. These are much larger than typical statistical fluctuations on scales of galaxies and we have to propose a mechanism to generate them. Furthermore, the measurements of anisotropies in the cosmic microwave background show that the amplitude of fluctuations is constant over a wide range of scales, the spectrum is scale independent. -
String-Inspired Running Vacuum—The ``Vacuumon''—And the Swampland Criteria
universe Article String-Inspired Running Vacuum—The “Vacuumon”—And the Swampland Criteria Nick E. Mavromatos 1 , Joan Solà Peracaula 2,* and Spyros Basilakos 3,4 1 Theoretical Particle Physics and Cosmology Group, Physics Department, King’s College London, Strand, London WC2R 2LS, UK; [email protected] 2 Departament de Física Quàntica i Astrofísica, and Institute of Cosmos Sciences (ICCUB), Universitat de Barcelona, Av. Diagonal 647, E-08028 Barcelona, Catalonia, Spain 3 Academy of Athens, Research Center for Astronomy and Applied Mathematics, Soranou Efessiou 4, 11527 Athens, Greece; [email protected] 4 National Observatory of Athens, Lofos Nymfon, 11852 Athens, Greece * Correspondence: [email protected] Received: 15 October 2020; Accepted: 17 November 2020; Published: 20 November 2020 Abstract: We elaborate further on the compatibility of the “vacuumon potential” that characterises the inflationary phase of the running vacuum model (RVM) with the swampland criteria. The work is motivated by the fact that, as demonstrated recently by the authors, the RVM framework can be derived as an effective gravitational field theory stemming from underlying microscopic (critical) string theory models with gravitational anomalies, involving condensation of primordial gravitational waves. Although believed to be a classical scalar field description, not representing a fully fledged quantum field, we show here that the vacuumon potential satisfies certain swampland criteria for the relevant regime of parameters and field range. We link the criteria to the Gibbons–Hawking entropy that has been argued to characterise the RVM during the de Sitter phase. These results imply that the vacuumon may, after all, admit under certain conditions, a rôle as a quantum field during the inflationary (almost de Sitter) phase of the running vacuum. -
String Theory and Pre-Big Bang Cosmology
IL NUOVO CIMENTO 38 C (2015) 160 DOI 10.1393/ncc/i2015-15160-8 Colloquia: VILASIFEST String theory and pre-big bang cosmology M. Gasperini(1)andG. Veneziano(2) (1) Dipartimento di Fisica, Universit`a di Bari - Via G. Amendola 173, 70126 Bari, Italy and INFN, Sezione di Bari - Bari, Italy (2) CERN, Theory Unit, Physics Department - CH-1211 Geneva 23, Switzerland and Coll`ege de France - 11 Place M. Berthelot, 75005 Paris, France received 11 January 2016 Summary. — In string theory, the traditional picture of a Universe that emerges from the inflation of a very small and highly curved space-time patch is a possibility, not a necessity: quite different initial conditions are possible, and not necessarily unlikely. In particular, the duality symmetries of string theory suggest scenarios in which the Universe starts inflating from an initial state characterized by very small curvature and interactions. Such a state, being gravitationally unstable, will evolve towards higher curvature and coupling, until string-size effects and loop corrections make the Universe “bounce” into a standard, decreasing-curvature regime. In such a context, the hot big bang of conventional cosmology is replaced by a “hot big bounce” in which the bouncing and heating mechanisms originate from the quan- tum production of particles in the high-curvature, large-coupling pre-bounce phase. Here we briefly summarize the main features of this inflationary scenario, proposed a quarter century ago. In its simplest version (where it represents an alternative and not a complement to standard slow-roll inflation) it can produce a viable spectrum of density perturbations, together with a tensor component characterized by a “blue” spectral index with a peak in the GHz frequency range. -
The Cosmic Microwave Background: the History of Its Experimental Investigation and Its Significance for Cosmology
REVIEW ARTICLE The Cosmic Microwave Background: The history of its experimental investigation and its significance for cosmology Ruth Durrer Universit´ede Gen`eve, D´epartement de Physique Th´eorique,1211 Gen`eve, Switzerland E-mail: [email protected] Abstract. This review describes the discovery of the cosmic microwave background radiation in 1965 and its impact on cosmology in the 50 years that followed. This discovery has established the Big Bang model of the Universe and the analysis of its fluctuations has confirmed the idea of inflation and led to the present era of precision cosmology. I discuss the evolution of cosmological perturbations and their imprint on the CMB as temperature fluctuations and polarization. I also show how a phase of inflationary expansion generates fluctuations in the spacetime curvature and primordial gravitational waves. In addition I present findings of CMB experiments, from the earliest to the most recent ones. The accuracy of these experiments has helped us to estimate the parameters of the cosmological model with unprecedented precision so that in the future we shall be able to test not only cosmological models but General Relativity itself on cosmological scales. Submitted to: Class. Quantum Grav. arXiv:1506.01907v1 [astro-ph.CO] 5 Jun 2015 The Cosmic Microwave Background 2 1. Historical Introduction The discovery of the Cosmic Microwave Background (CMB) by Penzias and Wilson, reported in Refs. [1, 2], has been a 'game changer' in cosmology. Before this discovery, despite the observation of the expansion of the Universe, see [3], the steady state model of cosmology still had a respectable group of followers. -
Exploring Cosmic Strings: Observable Effects and Cosmological Constraints
EXPLORING COSMIC STRINGS: OBSERVABLE EFFECTS AND COSMOLOGICAL CONSTRAINTS A dissertation submitted by Eray Sabancilar In partial fulfilment of the requirements for the degree of Doctor of Philosophy in Physics TUFTS UNIVERSITY May 2011 ADVISOR: Prof. Alexander Vilenkin To my parents Afife and Erdal, and to the memory of my grandmother Fadime ii Abstract Observation of cosmic (super)strings can serve as a useful hint to understand the fundamental theories of physics, such as grand unified theories (GUTs) and/or superstring theory. In this regard, I present new mechanisms to pro- duce particles from cosmic (super)strings, and discuss their cosmological and observational effects in this dissertation. The first chapter is devoted to a review of the standard cosmology, cosmic (super)strings and cosmic rays. The second chapter discusses the cosmological effects of moduli. Moduli are relatively light, weakly coupled scalar fields, predicted in supersymmetric particle theories including string theory. They can be emitted from cosmic (super)string loops in the early universe. Abundance of such moduli is con- strained by diffuse gamma ray background, dark matter, and primordial ele- ment abundances. These constraints put an upper bound on the string tension 28 as strong as Gµ . 10− for a wide range of modulus mass m. If the modulus coupling constant is stronger than gravitational strength, modulus radiation can be the dominant energy loss mechanism for the loops. Furthermore, mod- ulus lifetimes become shorter for stronger coupling. Hence, the constraints on string tension Gµ and modulus mass m are significantly relaxed for strongly coupled moduli predicted in superstring theory. Thermal production of these particles and their possible effects are also considered. -
Phenomenological Aspects of Type IIB Flux Compactifications
Phenomenological Aspects of Type IIB Flux Compactifications Enrico Pajer Munchen¨ 2008 Phenomenological Aspects of Type IIB Flux Compactifications Enrico Pajer Dissertation an der Fakult¨at fur¨ Physik der Ludwig–Maximilians–Universit¨at Munchen¨ vorgelegt von Enrico Pajer aus Venedig, Italien Munchen,¨ den 01. Juni 2008 Erstgutachter: Dr. Michael Haack Zweitgutachter: Prof. Dr. Dieter Lust¨ Tag der mundlichen¨ Prufung:¨ 18.07.2008 Contents 1 Introduction and conclusions 1 2 Type IIB flux compactifications 9 2.1 Superstring theory in a nutshell . 10 2.2 How many string theories are there? . 13 2.3 Type IIB . 15 2.4 D-branes . 17 2.5 Flux compactifications . 18 2.5.1 The GKP setup . 19 2.6 Towards de Sitter vacua in string theory . 21 3 Inflation in string theory 27 3.1 Observations . 27 3.2 Inflation . 29 3.2.1 Slow-roll models . 32 3.3 String theory models of inflation . 35 3.3.1 Open string models . 35 3.3.2 Closed string models . 36 3.4 Discussion . 37 4 Radial brane inflation 39 4.1 Preliminaries . 40 4.2 The superpotential . 42 4.3 Warped Brane inflation . 44 4.3.1 The η-problem from volume stabilization . 44 4.3.2 F-term potential for the conifold . 46 4.4 Critical points of the potential . 47 4.4.1 Axion stabilization . 48 4.4.2 Volume stabilization . 48 4.4.3 Angular moduli stabilization . 50 4.4.4 Potential with fixed moduli . 51 4.5 Explicit examples: Ouyang vs Kuperstein embedding . 52 4.5.1 Ouyang embedding . 52 4.5.2 Kuperstein embedding . -
Generalised Velocity-Dependent One-Scale Model for Current-Carrying Strings
Generalised velocity-dependent one-scale model for current-carrying strings C. J. A. P. Martins,1, 2, ∗ Patrick Peter,3, 4, y I. Yu. Rybak,1, 2, z and E. P. S. Shellard4, x 1Centro de Astrofísica da Universidade do Porto, Rua das Estrelas, 4150-762 Porto, Portugal 2Instituto de Astrofísica e Ciências do Espaço, CAUP, Rua das Estrelas, 4150-762 Porto, Portugal 3 GR"CO – Institut d’Astrophysique de Paris, CNRS & Sorbonne Université, UMR 7095 98 bis boulevard Arago, 75014 Paris, France 4Centre for Theoretical Cosmology, Department of Applied Mathematics and Theoretical Physics, University of Cambridge, Wilberforce Road, Cambridge CB3 0WA, United Kingdom (Dated: November 20, 2020) We develop an analytic model to quantitatively describe the evolution of superconducting cosmic string networks. Specifically, we extend the velocity-dependent one-scale (VOS) model to incorpo- rate arbitrary currents and charges on cosmic string worldsheets under two main assumptions, the validity of which we also discuss. We derive equations that describe the string network evolution in terms of four macroscopic parameters: the mean string separation (or alternatively the string correlation length) and the root mean square (RMS) velocity which are the cornerstones of the VOS model, together with parameters describing the averaged timelike and spacelike current contribu- tions. We show that our extended description reproduces the particular cases of wiggly and chiral cosmic strings, previously studied in the literature. This VOS model enables investigation of the evolution and possible observational signatures of superconducting cosmic string networks for more general equations of state, and these opportunities will be exploited in a companion paper. -
Loop Quantum Gravity: the First 25 Years Carlo Rovelli
Loop quantum gravity: the first 25 years Carlo Rovelli To cite this version: Carlo Rovelli. Loop quantum gravity: the first 25 years. Classical and Quantum Gravity, IOP Publishing, 2011, 28 (15), pp.153002. 10.1088/0264-9381/28/15/153002. hal-00723006 HAL Id: hal-00723006 https://hal.archives-ouvertes.fr/hal-00723006 Submitted on 7 Aug 2012 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Loop quantum gravity: the first twenty five years Carlo Rovelli Centre de Physique Th´eorique de Luminy∗, Case 907, F-13288 Marseille, EU (Dated: January 27, 2011) I give a synthetic presentation of loop quantum gravity. I spell-out the aims of the theory and compare the results obtained with the initial hopes that motivated the early interest in this research direction. I give my own perspective on the status of the program and attempt of a critical evaluation of its successes and limits. I. INTRODUCTION The history of quantum gravity is full of great hopes later disappointed. I remember as a young student sitting in a major conference where a world-renowned physicists Loop gravity is not quite twenty-five years old, but announced that the final theory of quantum gravity and is getting close to such a venerable age: several basic everything had finally been found. -
Dilaton and Off-Shell (Non-Critical String) Effects in Boltzmann Equation for Species Abundances AB Lahanas1, NE Mavromatos2 and DV Nanopoulos3,4,5
Research article Open Access Dilaton and off-shell (non-critical string) effects in Boltzmann equation for species abundances AB Lahanas1, NE Mavromatos2 and DV Nanopoulos3,4,5 Address: 1University of Athens, Physics Department, Nuclear and Particle Physics Section, GR157 71, Athens, Greece., 2King's College London, University of London, Department of Physics, Strand WC2R 2LS, London, UK., 3George P. and Cynthia W. Mitchell Institute for Fundamental Physics, Texas A&M University, College Station, TX 77843, USA., 4Astroparticle Physics Group, Houston Advanced Research Center (HARC), Mitchell Campus, Woodlands, TX 77381, USA. and 5Academy of Athens, Division of Natural Sciences, 28 Panepistimiou Avenue, Athens 10679, Greece. Email: AB Lahanas - [email protected]; NE Mavromatos - [email protected]; DV Nanopoulos - [email protected] Published: 2 October 2007 Received: 3 June 2007 Accepted: 2 October 2007 PMC Physics A 2007, 1:2 doi:10.1186/1754-0410-1-2 This article is available from: http://www.physmathcentral.com/1754-0410/1/2 © 2007 Lahanas et al. This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/ licenses/by/2.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. Abstract In this work we derive the modifications to the Boltzmann equation governing the cosmic evolution of relic abundances induced by dilaton dissipative-source and non-critical-string terms in dilaton-driven non-equilibrium string Cosmologies. We also discuss briefly the most important phenomenological consequences, including modifications of the constraints on the available parameter space of cosmologically appealing particle physics models, imposed by recent precision data of astrophysical measurements. -
Model-Independent Cosmological Constraints from the CMB
Outline Motivations Cosmic Microwave Background (CMB): basic ideas Model-independent analyze of the CMB Conclusion Model-independent cosmological constraints from the CMB. Marc Vonlanthen, Ruth Durrer, Syksy Ras¨anen University of Geneva Ascona, January 20th 2010 Marc Vonlanthen, Ruth Durrer, Syksy Ras¨anen Model-independent cosmological constraints from the CMB. Outline Motivations Cosmic Microwave Background (CMB): basic ideas Model-independent analyze of the CMB Conclusion Motivations Cosmic Microwave Background (CMB): basic ideas The Cosmic Microwave Background CMB anisotropies Model-independent analyze of the CMB Sensitivity of the CMB to the cosmological parameters Methodology Results Conclusion Marc Vonlanthen, Ruth Durrer, Syksy Ras¨anen Model-independent cosmological constraints from the CMB. Outline Motivations Cosmic Microwave Background (CMB): basic ideas Model-independent analyze of the CMB Conclusion What we want to study and why it is interesting... 1. The standard model of cosmology in which Ωm ∼ 0.3and ΩΛ ∼ 0.7seemstofitanimpressivevarietyofdata. Λ ρΛ 2. However, Λin ΩΛ = 2 = faces many problems: 3H0 ρc ! why is ρΛ so much smaller than we expect (120 order of magnitudes) ? ! what is the origin of the small nonzero energy that comprises 70% of the universe today ? ! why is the current value of the vacuum energy of the same order of magnitude as the matter density ΩΛ ∼ a3 ∼O(1) Ωm today ? 3. Answers are model-dependent and uncertain, it is therefore worthwhile to study model-independently our universe. Marc Vonlanthen, Ruth Durrer, Syksy Ras¨anen Model-independent cosmological constraints from the CMB. Outline Motivations The Cosmic Microwave Background Cosmic Microwave Background (CMB): basic ideas CMB anisotropies Model-independent analyze of the CMB Conclusion Dynamics of a Friedmann-Lemaˆıtre universe ln(ρ) radiation matter Cosmological constant ln(a) aeq arec adec aΛ a0 Marc Vonlanthen, Ruth Durrer, Syksy Ras¨anen Model-independent cosmological constraints from the CMB.