The Quantum to Classical Transition in Inflationary Cosmology
|
|
- Jason Lewis
- 5 years ago
- Views:
Transcription
1 The Quantum to Classical Transition in Inflationary Cosmology C. D. McCoy Department of Philosophy University of California San Diego Foundations of Physics Munich, 31 July 2013
2 Questions to Address 1. How does the measurement problem arise in cosmological structure formation? 2. Which proposed solutions of the measurement problem are applicable to structure formation? 3. How does the Everett interpretation fare in explaining this quantum to classical" transition?
3 A History of the Universe
4 The Cosmic Microwave Background Radiation Θ(n ) δt (n ) X = a`m Y`m (n ) T0 `,m
5 The Power Spectrum of the Cosmic Microwave Background C l = 1 2l + 1 alm, a lm = 2 π m k 2 dk P Φ (k) 2 l (k)
6 The Power Spectrum of the Cosmic Microwave Background C l = 1 2l + 1 alm, a lm = 2 π m k 2 dk P Φ (k) 2 l (k)
7 The Power Spectrum of the Cosmic Microwave Background C l = 1 2l + 1 alm, a lm = 2 π m k 2 dk P Φ (k) 2 l (k)
8 The Power Spectrum of the Cosmic Microwave Background C l = 1 2l + 1 alm, a lm = 2 π m k 2 dk P Φ (k) 2 l (k)
9 Primordial Perturbations Assume that the primordial spectrum follows a power law: P(k) = A k ns 1 Then the CMB data suggest that the spectrum is approximately scale invariant (P(k) const); 2. small amplitude (A << 1); 3. and approximately Gaussian (n s 1);
10 Primordial Perturbations Assume that the primordial spectrum follows a power law: P(k) = A k ns 1 Then the CMB data suggest that the spectrum is approximately scale invariant (P(k) const); 2. small amplitude (A << 1); 3. and approximately Gaussian (n s 1);...but a naive retrodiction of this spectrum (classical general relativity and relativistic hydrodynamics) results in all modes being generated beyond the horizon (acausal) at early times/high densities.
11 Origin of the Primordial Spectrum
12 Origin of the Primordial Spectrum Inexplicable acausal correlations Horizon Problem!
13 Origin of the Primordial Spectrum
14 Origin of the Primordial Spectrum Inflation solves horizon problem Inflation implemented by a scalar field with a certain potential
15 Quantum Fluctuations as the Origin of the Primordial Spectrum* Einstein-Hilbert Action and Action of a Scalar Field (Inflaton). S = 1 d 4 x R g + d 4 x [ ] 1 φ φ g gµν 16π 2 x µ x ν V (φ) Linearize metric and scalar field, separating homogeneous part from perturbation. g µν (x, t) = ḡ µν (t) + δg µν (x, t) φ(x, t) = φ(t) + δφ(x, t) ds 2 = a 2 (η) [ (1 + 2Φ) dη 2 + (1 2Ψ) γ ij dx i dx j ] *Mukhanov, Feldman, and Brandenberger, Phys Rep 1992 *Mukhanov, Physical Foundations of Cosmology 2005
16 Quantum Fluctuations as the Origin of the Primordial Spectrum Introduce a gauge-invariant combination of the scalar field and metric perturbations, the Mukhanov-Sasaki variable v: v(η, x) = a(δφ + φ φ Ψ) z = a H H And write the action in terms of v and z: S 2 = Ldη d 3 x = 1 ) (v 2 v,i v,i + z 2 z v 2 dη d 3 x v k + (k 2 z z )v k = 0
17 Quantizing the Inflaton Define the momentum π canonically conjugate to v as π = v. Promote v and π to operators obeying the standard commutation relations. Decompose solutions into adiabatic modes with creation and annihilation operators and define the vacuum as â k 0 = 0. Compute the power spectrum: P Φ (k) = Φ k 2 2π 2 = 1 2π 2 ˆΦ(x, η)ˆφ (y, η)
18 Quantizing the Inflaton Define the momentum π canonically conjugate to v as π = v. Promote v and π to operators obeying the standard commutation relations. Decompose solutions into adiabatic modes with creation and annihilation operators and define the vacuum as â k 0 = 0. Compute the power spectrum: P Φ (k) = Φ k 2 2π 2 = 1 2π 2 ˆΦ(x, η)ˆφ (y, η) Quantum correlation function to ensemble average? 0 ˆΦ(x, η)ˆφ(y, η) 0 ˆΦ(x, η)ˆφ (y, η)
19 Quantum Theory without Observers Quantum theory applied to cosmology must be a quantum theory without observers.
20 Quantum Theory without Observers Quantum theory applied to cosmology must be a quantum theory without observers. 1. Collapse Theories Martin, Vennin, and Peter, Phys. Rev. D 2012; Lochan, Das, and Bassi, Phys. Rev. D 2012; Cañate, Pearle, and Sudarsky, Phys, Rev. D 2013
21 Quantum Theory without Observers Quantum theory applied to cosmology must be a quantum theory without observers. 1. Collapse Theories Martin, Vennin, and Peter, Phys. Rev. D 2012; Lochan, Das, and Bassi, Phys. Rev. D 2012; Cañate, Pearle, and Sudarsky, Phys, Rev. D Bohmian Theories Valentini, Phys. Rev. D 2010; Pinto-Neto, Santos, and Struyve, Phys. Rev. D 2012
22 Quantum Theory without Observers Quantum theory applied to cosmology must be a quantum theory without observers. 1. Collapse Theories Martin, Vennin, and Peter, Phys. Rev. D 2012; Lochan, Das, and Bassi, Phys. Rev. D 2012; Cañate, Pearle, and Sudarsky, Phys, Rev. D Bohmian Theories Valentini, Phys. Rev. D 2010; Pinto-Neto, Santos, and Struyve, Phys. Rev. D Everett interpretation???
23 Classicality Condition for Many Worlds (Wallace) A history is a sequence of time-indexed PVMs. The set of such histories generated from some such sequence of PVMs is a history space P. The history operator Ĉα of the history α is Ĉ α = ˆα(n)... ˆα(0). The decoherence functional is a complex function on pairs of histories (relative to a choice of state ψ ) given by D(α, β) = ψ Ĉ αĉβ ψ. A history space is said to satisfy the decoherence condition or to be decoherent if the decoherence functional between any two incompatible histories is zero. If P satisfies the decoherence condition, it is a coarse-graining of a (decoherent) history space which has a branching structure relative to ψ.
24 Decoherence in the Early Universe Decoherence is essentially the suppression of interference with respect to a system s macroscopic degrees of freedom via interactions with microscopic degrees of freedom (internal or external environment").
25 Decoherence in the Early Universe Decoherence is essentially the suppression of interference with respect to a system s macroscopic degrees of freedom via interactions with microscopic degrees of freedom (internal or external environment"). Decoherence does not solve the measurement problem, but does it place a constraint on quantum theories of structure formation?
26 Decoherence in the Early Universe Decoherence is essentially the suppression of interference with respect to a system s macroscopic degrees of freedom via interactions with microscopic degrees of freedom (internal or external environment"). Decoherence does not solve the measurement problem, but does it place a constraint on quantum theories of structure formation? In the literature on the quantum to classical transition during cosmological structure formation, decoherence has been shown to occur in many ways: external scalar fields, short wavelength modes, non-linear coupling between modes, spatial entanglement, thermal fluctuations after reheating...
27 Decoherence in the Early Universe Decoherence is essentially the suppression of interference with respect to a system s macroscopic degrees of freedom via interactions with microscopic degrees of freedom (internal or external environment"). Decoherence does not solve the measurement problem, but does it place a constraint on quantum theories of structure formation? In the literature on the quantum to classical transition during cosmological structure formation, decoherence has been shown to occur in many ways: external scalar fields, short wavelength modes, non-linear coupling between modes, spatial entanglement, thermal fluctuations after reheating... What attitude should one take to these demonstrations?
28 Attitudes Toward Structure Formation and the Everett Interpretation 1. The ease of generating decoherence in the inflationary scenario is further evidence that decoherence is ubiquitous, thus by requiring decoherence the Everett interpretation places a minimal constraint on theories of structure formation. What accounts for the ubiquity of decoherence and therefore the direction of branching?
29 Attitudes Toward Structure Formation and the Everett Interpretation 1. The ease of generating decoherence in the inflationary scenario is further evidence that decoherence is ubiquitous, thus by requiring decoherence the Everett interpretation places a minimal constraint on theories of structure formation. What accounts for the ubiquity of decoherence and therefore the direction of branching? Initial Conditions?
30 Attitudes Toward Structure Formation and the Everett Interpretation 1. The ease of generating decoherence in the inflationary scenario is further evidence that decoherence is ubiquitous, thus by requiring decoherence the Everett interpretation places a minimal constraint on theories of structure formation. What accounts for the ubiquity of decoherence and therefore the direction of branching? Initial Conditions? 2. The variety of ways to decohere fields in the early universe that people have proposed raises theoretical worries about inflation or the Everett interpretation. Too little known about the inflaton and its interactions with other physical fields There is no principled division" of the universe into system and environment.
31 Attitudes Toward Structure Formation and the Everett Interpretation 1. The ease of generating decoherence in the inflationary scenario is further evidence that decoherence is ubiquitous, thus by requiring decoherence the Everett interpretation places a minimal constraint on theories of structure formation. What accounts for the ubiquity of decoherence and therefore the direction of branching? Initial Conditions? 2. The variety of ways to decohere fields in the early universe that people have proposed raises theoretical worries about inflation or the Everett interpretation. Too little known about the inflaton and its interactions with other physical fields. Effective theory? There is no principled division" of the universe into system and environment.
32 Attitudes Toward Structure Formation and the Everett Interpretation 1. The ease of generating decoherence in the inflationary scenario is further evidence that decoherence is ubiquitous, thus by requiring decoherence the Everett interpretation places a minimal constraint on theories of structure formation. What accounts for the ubiquity of decoherence and therefore the direction of branching? Initial Conditions? 2. The variety of ways to decohere fields in the early universe that people have proposed raises theoretical worries about inflation or the Everett interpretation. Too little known about the inflaton and its interactions with other physical fields. Effective theory? There is no principled division" of the universe into system and environment. Need to show consistency!
33 Conclusions 1. The standard theory of structure formation is a quantum theory with the appearance of classical outcomes thus the quantum measurement problem appears in cosmology as it does elsewhere in physics. 2. A solution of the measurement problem must be a quantum theory without observers to be applicable to cosmology. 3. The Everett interpretation (modulo concerns over probability) is applicable to cosmology, but is conservative and unlikely to raise issues in this application still, work is required to demonstrate satisfaction of the decoherence condition. 4. Further work on the quantum measurement problem is of relatively little importance to cosmology; of far more importance is understanding the initial state of the universe and the nature of the inflaton.
34 Structure Formation and the Measurement Problem Mukhanov, Physical Foundations of Cosmology When we look at the sky we see the galaxies in certain positions. If these galaxies originated from initial quantum fluctuations, a natural question arises: how does a galaxy, e.g. Andromeda, find itself at a particular place if the initial vacuum state was translational-invariant with no preferred position in space? Quantum mechanical unitary evolution does not destroy translational invariance and hence the answer to this question must lie in the transition from quantum fluctuations to classical inhomogeneities.
35 Structure Formation and the Measurement Problem Decoherence is a necessary condition for the emergence of classical inhomogeneities and can easily be justified for amplified cosmological perturbations. However, decoherence is not sufficient to explain the breaking of translational invariance. It can be shown that as a result of unitary evolution we obtain a state which is a superposition of many macroscopically different states, each corresponding to a particular realization of galaxy distribution.
36 Structure Formation and the Measurement Problem Most of these realizations have the same statistical properties. Such a state is a close cosmic analog of the Schrödinger cat." Therefore, to pick an observed macroscopic state from the superposition we have to appeal either to Bohr s reduction postulate or to Everett s many-worlds interpretation of quantum mechanics.
37 Quantum Measurement Problem Today The quantum measurement problem is not a psuedo-problem. It is a conceptual stumbling block to the universal application of quantum theory, e.g. in cosmology.
38 Quantum Measurement Problem Today The quantum measurement problem is not a psuedo-problem. It is a conceptual stumbling block to the universal application of quantum theory, e.g. in cosmology. The quantum measurement problem is not solved by decoherence. Decoherence does not destroy superpositions.
39 Quantum Measurement Problem Today The quantum measurement problem is not a psuedo-problem. It is a conceptual stumbling block to the universal application of quantum theory, e.g. in cosmology. The quantum measurement problem is not solved by decoherence. Decoherence does not destroy superpositions. The quantum measurement problem is not solved. Conceptual problems are not solved". There are many approaches, some of which are coherent, of interest, etc. Others are not.
40 Quantum Measurement Problem Today The quantum measurement problem is not a psuedo-problem. It is a conceptual stumbling block to the universal application of quantum theory, e.g. in cosmology. The quantum measurement problem is not solved by decoherence. Decoherence does not destroy superpositions. The quantum measurement problem is not solved. Conceptual problems are not solved". There are many approaches, some of which are coherent, of interest, etc. Others are not. The quantum measurement problem is not a severe difficulty.
Cosmology and the origin of structure
1 Cosmology and the origin of structure ocy I: The universe observed ocy II: Perturbations ocy III: Inflation Primordial perturbations CB: a snapshot of the universe 38, AB correlations on scales 38, light
More informationApplications of Bohmian mechanics in quantum gravity
Applications of Bohmian mechanics in quantum gravity Ward Struyve LMU, Munich, Germany Outline: Why do we need a quantum theory for gravity? What is the quantum theory for gravity? Problems with quantum
More informationThe Theory of Inflationary Perturbations
The Theory of Inflationary Perturbations Jérôme Martin Institut d Astrophysique de Paris (IAP) Indian Institute of Technology, Chennai 03/02/2012 1 Introduction Outline A brief description of inflation
More informationQuantum Fluctuations During Inflation
In any field, find the strangest thing and then explore it. (John Archibald Wheeler) Quantum Fluctuations During Inflation ( ) v k = e ikτ 1 i kτ Contents 1 Getting Started Cosmological Perturbation Theory.1
More informationThe quantum origin of the cosmic structure: an arena for Quantum Gravity Phenomenology
The quantum origin of the cosmic structure: an arena for Quantum Gravity Phenomenology Daniel Sudarsky ICN- UNAM, Mexico Original work in collaboration with: A. Perez ( U. MARSEILLE) H.Sahlmann ( PENN
More informationPAPER 71 COSMOLOGY. Attempt THREE questions There are seven questions in total The questions carry equal weight
MATHEMATICAL TRIPOS Part III Friday 31 May 00 9 to 1 PAPER 71 COSMOLOGY Attempt THREE questions There are seven questions in total The questions carry equal weight You may make free use of the information
More informationInflation and the Primordial Perturbation Spectrum
PORTILLO 1 Inflation and the Primordial Perturbation Spectrum Stephen K N PORTILLO Introduction The theory of cosmic inflation is the leading hypothesis for the origin of structure in the universe. It
More informationarxiv:gr-qc/ v1 20 Aug 1992
BROWN-HET-849 August 1992 The Entropy of the Gravitational Field R. Brandenberger, T. Prokopec arxiv:gr-qc/9208009 v1 20 Aug 1992 Department of Physics, Brown University, Providence, Rhode Island 02912,
More informationInflationary Cosmology and Alternatives
Inflationary Cosmology and Alternatives V.A. Rubakov Institute for Nuclear Research of the Russian Academy of Sciences, Moscow and Department of paricle Physics abd Cosmology Physics Faculty Moscow State
More informationPREHEATING, PARAMETRIC RESONANCE AND THE EINSTEIN FIELD EQUATIONS
PREHEATING, PARAMETRIC RESONANCE AND THE EINSTEIN FIELD EQUATIONS Matthew PARRY and Richard EASTHER Department of Physics, Brown University Box 1843, Providence RI 2912, USA Email: parry@het.brown.edu,
More informationCosmic Bubble Collisions
Outline Background Expanding Universe: Einstein s Eqn with FRW metric Inflationary Cosmology: model with scalar field QFTà Bubble nucleationà Bubble collisions Bubble Collisions in Single Field Theory
More informationPedro 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 informationSignatures of Trans-Planckian Dissipation in Inflationary Spectra
Signatures of Trans-Planckian Dissipation in Inflationary Spectra 3. Kosmologietag Bielefeld Julian Adamek ITPA University Würzburg 8. May 2008 Julian Adamek 1 / 18 Trans-Planckian Dissipation in Inflationary
More informationIntroduction to Inflation
Introduction to Inflation Miguel Campos MPI für Kernphysik & Heidelberg Universität September 23, 2014 Index (Brief) historic background The Cosmological Principle Big-bang puzzles Flatness Horizons Monopoles
More informationBouncing Cosmologies with Dark Matter and Dark Energy
Article Bouncing Cosmologies with Dark Matter and Dark Energy Yi-Fu Cai 1, *, Antonino Marcianò 2, Dong-Gang Wang 1,3,4 and Edward Wilson-Ewing 5 1 CAS Key Laboratory for Research in Galaxies and Cosmology,
More informationComputational Physics and Astrophysics
Cosmological Inflation Kostas Kokkotas University of Tübingen, Germany and Pablo Laguna Georgia Institute of Technology, USA Spring 2012 Our Universe Cosmic Expansion Co-moving coordinates expand at exactly
More informationStructures in the early Universe. Particle Astrophysics chapter 8 Lecture 4
Structures in the early Universe Particle Astrophysics chapter 8 Lecture 4 overview Part 1: problems in Standard Model of Cosmology: horizon and flatness problems presence of structures Part : Need for
More informationAttempts at relativistic QM
Attempts at relativistic QM based on S-1 A proper description of particle physics should incorporate both quantum mechanics and special relativity. However historically combining quantum mechanics and
More informationOn 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 informationAn Estimator for statistical anisotropy from the CMB. CMB bispectrum
An Estimator for statistical anisotropy from the CMB bispectrum 09/29/2012 1 2 3 4 5 6 ...based on: N. Bartolo, E. D., M. Liguori, S. Matarrese, A. Riotto JCAP 1201:029 N. Bartolo, E. D., S. Matarrese,
More informationScale 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 informationNon-singular quantum cosmology and scale invariant perturbations
th AMT Toulouse November 6, 2007 Patrick Peter Non-singular quantum cosmology and scale invariant perturbations Institut d Astrophysique de Paris GRεCO AMT - Toulouse - 6th November 2007 based upon Tensor
More informationInflationary Massive Gravity
New perspectives on cosmology APCTP, 15 Feb., 017 Inflationary Massive Gravity Misao Sasaki Yukawa Institute for Theoretical Physics, Kyoto University C. Lin & MS, PLB 75, 84 (016) [arxiv:1504.01373 ]
More informationprimordial avec les perturbations cosmologiques *
Tests de l Univers primordial avec les perturbations cosmologiques * Filippo Vernizzi Batz-sur-Mer, 16 octobre, 2008 * Soustitré en anglais What is the initial condition? Standard single field inflation
More informationFrom inflation to the CMB to today s universe. I - How it all begins
From inflation to the CMB to today s universe I - How it all begins Raul Abramo Physics Institute - University of São Paulo abramo@fma.if.usp.br redshift Very brief cosmic history 10 9 200 s BBN 1 MeV
More informationSchool Observational Cosmology Angra Terceira Açores 3 rd June Juan García-Bellido Física Teórica UAM Madrid, Spain
School Observational Cosmology Angra Terceira Açores 3 rd June 2014 Juan García-Bellido Física Teórica UAM Madrid, Spain Outline Lecture 1 Shortcomings of the Hot Big Bang The Inflationary Paradigm Homogeneous
More informationBielefeld - 09/23/09. Observing Alternatives to Inflation. Patri Pe r. Institut d Astrophysique de Paris. Bielefeld - 23 rd september 2009
Bielefeld - 09/23/09 Observing Alternatives to Inflation Patri Pe r Institut d Astrophysique de Paris GRεCO Bielefeld - 23 rd september 2009 Problems with standard model: Singularity Horizon Flatness Homogeneity
More informationMASAHIDE YAMAGUCHI. Quantum generation of density perturbations in the early Universe. (Tokyo Institute of Technology)
Quantum generation of density perturbations in the early Universe MASAHIDE YAMAGUCHI (Tokyo Institute of Technology) 03/07/16@Symposium: New Generation Quantum Theory -Particle Physics, Cosmology, and
More informationInflation and the origin of structure in the Universe
Phi in the Sky, Porto 0 th July 004 Inflation and the origin of structure in the Universe David Wands Institute of Cosmology and Gravitation University of Portsmouth outline! motivation! the Primordial
More informationClassical Dynamics of Inflation
Preprint typeset in JHEP style - HYPER VERSION Classical Dynamics of Inflation Daniel Baumann School of Natural Sciences, Institute for Advanced Study, Princeton, NJ 08540 http://www.sns.ias.edu/ dbaumann/
More informationPHY 396 K. Problem set #5. Due October 9, 2008.
PHY 396 K. Problem set #5. Due October 9, 2008.. First, an exercise in bosonic commutation relations [â α, â β = 0, [â α, â β = 0, [â α, â β = δ αβ. ( (a Calculate the commutators [â αâ β, â γ, [â αâ β,
More informationClassical field theory 2012 (NS-364B) Feynman propagator
Classical field theory 212 (NS-364B Feynman propagator 1. Introduction States in quantum mechanics in Schrödinger picture evolve as ( Ψt = Û(t,t Ψt, Û(t,t = T exp ı t dt Ĥ(t, (1 t where Û(t,t denotes the
More informationKey: cosmological perturbations. With the LHC, we hope to be able to go up to temperatures T 100 GeV, age t second
Lecture 3 With Big Bang nucleosynthesis theory and observations we are confident of the theory of the early Universe at temperatures up to T 1 MeV, age t 1 second With the LHC, we hope to be able to go
More informationAstro 507 Lecture 28 April 2, 2014
Astro 507 Lecture 28 April 2, 2014 Announcements: PS 5 due now Preflight 6 posted today last PF! 1 Last time: slow-roll inflation scalar field dynamics in an expanding universe slow roll conditions constrain
More informationSecond-order gauge-invariant cosmological perturbation theory: --- Recent development and problems ---
Second-order gauge-invariant cosmological perturbation theory: --- Recent development and problems --- Kouji Nakamura (NAOJ) with Masa-Katsu Fujimoto (NAOJ) References : K.N. Prog. Theor. Phys., 110 (2003),
More informationGravitation: Cosmology
An Introduction to General Relativity Center for Relativistic Astrophysics School of Physics Georgia Institute of Technology Notes based on textbook: Spacetime and Geometry by S.M. Carroll Spring 2013
More informationObservational signatures of holographic models of inflation
Observational signatures of holographic models of inflation Paul McFadden Universiteit van Amsterdam First String Meeting 5/11/10 This talk I. Cosmological observables & non-gaussianity II. Holographic
More informationarxiv:hep-th/ v1 20 Oct 2002
arxiv:hep-th/0210186v1 20 Oct 2002 TRANS-PLANCKIAN PHYSICS AND INFLATIONARY COSMOLOGY ROBERT H. BRANDENBERGER Physics Dept., Brown University, Providence, R.I. 02912, USA E-mail: rhb@het.brown.edu Due
More informationBenefits of Objective Collapse Models for Cosmology and Quantum Gravity
Benefits of Objective Collapse Models for Cosmology and Quantum Gravity Elias Okon Instituto de Investigaciones Filosóficas, Universidad Nacional Autónoma de México Circuito Maestro Mario de la Cueva s/n,
More informationConnecting Quarks to the Cosmos
Connecting Quarks to the Cosmos Institute for Nuclear Theory 29 June to 10 July 2009 Inflationary Cosmology II Michael S. Turner Kavli Institute for Cosmological Physics The University of Chicago Michael
More informationAstronomy 182: Origin and Evolution of the Universe
Astronomy 182: Origin and Evolution of the Universe Prof. Josh Frieman Lecture 14 Dec. 2, 2015 Today The Inflationary Universe Origin of Density Perturbations Gravitational Waves Origin and Evolution of
More informationLoop Quantum Cosmology holonomy corrections to inflationary models
Michał Artymowski Loop Quantum Cosmology holonomy corrections to inflationary models University of Warsaw With collaboration with L. Szulc and Z. Lalak Pennstate 5 0 008 Michał Artymowski, University of
More informationIntroduction to Quantum fields in Curved Spaces
Introduction to Quantum fields in Curved Spaces Tommi Markkanen Imperial College London t.markkanen@imperial.ac.uk April/June-2018 Solvalla QFT in curved spacetime 1 / 35 Outline 1 Introduction 2 Cosmological
More informationTowards Multi-field Inflation with a Random Potential
Towards Multi-field Inflation with a Random Potential Jiajun Xu LEPP, Cornell Univeristy Based on H. Tye, JX, Y. Zhang, arxiv:0812.1944 and work in progress 1 Outline Motivation from string theory A scenario
More informationGauge 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 information4 Evolution of density perturbations
Spring term 2014: Dark Matter lecture 3/9 Torsten Bringmann (torsten.bringmann@fys.uio.no) reading: Weinberg, chapters 5-8 4 Evolution of density perturbations 4.1 Statistical description The cosmological
More informationIs quantum linear superposition exact on all energy scales? A unique case study with flavour oscillating systems
Is quantum linear superposition exact on all energy scales? A unique case study with flavour oscillating systems Supervisor: Dr. Beatrix C. Hiesmayr Universität Wien, Fakultät für Physik March 17, 2015
More informationPatrick Peter. Institut d Astrophysique de Paris Institut Lagrange de Paris. Evidences for inflation constraints on alternatives
Patrick Peter Institut d Astrophysique de Paris Institut Lagrange de Paris Evidences for inflation constraints on alternatives Thanks to Jérôme Martin For his help Planck 2015 almost scale invariant quantum
More informationPERTURBATIONS IN LOOP QUANTUM COSMOLOGY
PERTURBATIONS IN LOOP QUANTUM COSMOLOGY William Nelson Pennsylvania State University Work with: Abhay Astekar and Ivan Agullo (see Ivan s ILQG talk, 29 th March ) AUTHOR, W. NELSON (PENN. STATE) PERTURBATIONS
More informationOn the quantum origin of the seeds of cosmic structure
arxiv:gr-qc/0508100v3 25 Feb 2006 On the quantum origin of the seeds of cosmic structure Alejandro Perez 1,2, Hanno Sahlmann 1,4, and Daniel Sudarsky 1,3 1. Institute for Gravitational Physics and Geometry,
More informationState of the Universe Address
State of the Universe Address Prof. Scott Watson ( Syracuse University ) This talk is available online at: https://gswatson.expressions.syr.edu This research was supported in part by: Theoretical Cosmology
More informationOddities of the Universe
Oddities of the Universe Koushik Dutta Theory Division, Saha Institute Physics Department, IISER, Kolkata 4th November, 2016 1 Outline - Basics of General Relativity - Expanding FRW Universe - Problems
More informationThe multi-field facets of inflation. David Langlois (APC, Paris)
The multi-field facets of inflation David Langlois (APC, Paris) Introduction After 25 years of existence, inflation has been so far very successful to account for observational data. The nature of the
More informationCHAPTER 4 INFLATIONARY MODEL BUILDING. 4.1 Canonical scalar field dynamics. Non-minimal coupling and f(r) theories
CHAPTER 4 INFLATIONARY MODEL BUILDING Essentially, all models are wrong, but some are useful. George E. P. Box, 1987 As we learnt in the previous chapter, inflation is not a model, but rather a paradigm
More informationConstraints on Inflationary Correlators From Conformal Invariance. Sandip Trivedi Tata Institute of Fundamental Research, Mumbai.
Constraints on Inflationary Correlators From Conformal Invariance Sandip Trivedi Tata Institute of Fundamental Research, Mumbai. Based on: 1) I. Mata, S. Raju and SPT, JHEP 1307 (2013) 015 2) A. Ghosh,
More informationCosmological Signatures of Brane Inflation
March 22, 2008 Milestones in the Evolution of the Universe http://map.gsfc.nasa.gov/m mm.html Information about the Inflationary period The amplitude of the large-scale temperature fluctuations: δ H =
More informationEffects of Entanglement during Inflation on Cosmological Observables
Effects of Entanglement during Inflation on Cosmological Observables Nadia Bolis 1 Andreas Albrecht 1 Rich Holman 2 1 University of California Davis 2 Carnegie Mellon University September 5, 2015 Inflation
More informationWhy 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 informationExamining the Viability of Phantom Dark Energy
Examining the Viability of Phantom Dark Energy Kevin J. Ludwick LaGrange College 12/20/15 (11:00-11:30) Kevin J. Ludwick (LaGrange College) Examining the Viability of Phantom Dark Energy 12/20/15 (11:00-11:30)
More informationQuantum Field Theory
Quantum Field Theory PHYS-P 621 Radovan Dermisek, Indiana University Notes based on: M. Srednicki, Quantum Field Theory 1 Attempts at relativistic QM based on S-1 A proper description of particle physics
More informationExamining the Viability of Phantom Dark Energy
Examining the Viability of Phantom Dark Energy Kevin J. Ludwick LaGrange College 11/12/16 Kevin J. Ludwick (LaGrange College) Examining the Viability of Phantom Dark Energy 11/12/16 1 / 28 Outline 1 Overview
More informationGalaxy Formation Seminar 2: Cosmological Structure Formation as Initial Conditions for Galaxy Formation. Prof. Eric Gawiser
Galaxy Formation Seminar 2: Cosmological Structure Formation as Initial Conditions for Galaxy Formation Prof. Eric Gawiser Cosmic Microwave Background anisotropy and Large-scale structure Cosmic Microwave
More informationBlack holes as open quantum systems
Black holes as open quantum systems Claus Kiefer Institut für Theoretische Physik Universität zu Köln Hawking radiation 1 1 singularity II γ H γ γ H collapsing 111 star 1 1 I - future event horizon + i
More informationPhys/Astro 689: Lecture 3. The Growth of Structure
Phys/Astro 689: Lecture 3 The Growth of Structure Last time Examined the milestones (zeq, zrecomb, zdec) in early Universe Learned about the WIMP miracle and searches for WIMPs Goal of Lecture Understand
More informationZhong-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 informationarxiv: v1 [gr-qc] 30 Dec 2015 Abstract. We investigate the behavior of the entanglement entropy of space in the
Entanglement time in the primordial universe Eugenio Bianchi, 1, Lucas Hackl, 1, and Nelson Yokomizo 1, 1 Institute for Gravitation and the Cosmos, Physics Department, Penn State, University Park, PA 16802,
More informationarxiv:astro-ph/ v4 17 Sep 2004
A TIME VARYING STRONG COUPLING CONSTANT AS A MODEL OF INFLATIONARY UNIVERSE arxiv:astro-ph/000904v4 17 Sep 004 N. Chamoun 1,, S. J. Landau 3,4, H. Vucetich 1,3, 1 Departamento de Física, Universidad Nacional
More informationMaster Projects (EPFL) Philosophical perspectives on the exact sciences and their history
Master Projects (EPFL) Philosophical perspectives on the exact sciences and their history Some remarks on the measurement problem in quantum theory (Davide Romano) 1. An introduction to the quantum formalism
More informationQuantum Geometry and Space-time Singularities
p. Quantum Geometry and Space-time Singularities Abhay Ashtekar Newton Institute, October 27th, 2005 General Relativity: A beautiful encoding of gravity in geometry. But, as a consequence, space-time itself
More informationGaussian States in de Sitter Spacetime and the Evolution of Semiclassical Density Perturbations. 1. Homogeneous Mode
J. Astrophys. Astr. (1989) 10, 391 406 Gaussian States in de Sitter Spacetime and the Evolution of Semiclassical Density Perturbations. 1. Homogeneous Mode T. R. Seshadri & T. Padmanabhan Astrophysics
More informationHiggs field in cosmology
Higgs field in cosmology Christian Friedrich Steinwachs Albert-Ludwigs-Universität Freiburg 678th Wilhelm and Else Heraeus Seminar: Hundred Years of Gauge Theory, Bad Honnef, 02.08.2018 Cosmic history
More informationMulti-disformal invariance of nonlinear primordial perturbations
Multi-disformal invariance of nonlinear primordial perturbations Yuki Watanabe Natl. Inst. Tech., Gunma Coll.) with Atsushi Naruko and Misao Sasaki accepted in EPL [arxiv:1504.00672] 2nd RESCEU-APCosPA
More informationGravitation et Cosmologie: le Modèle Standard Cours 8: 6 fevrier 2009
Particules Élémentaires, Gravitation et Cosmologie Année 2008-09 Gravitation et Cosmologie: le Modèle Standard Cours 8: 6 fevrier 2009 Le paradigme inflationnaire Homogeneity and flatness problems in HBB
More informationA STUDY OF INFLATIONARY PARADIGM
A STUDY OF INFLATIONARY PARADIGM A Project Report By RATHUL NATH R The Institute of Mathematical Sciences, Chennai Under the joint-supervison of Prof. L. Sriramkumar and Prof. Ghanashyam Date June, 014
More informationAsymptotically safe Quantum Gravity. Nonperturbative renormalizability and fractal space-times
p. 1/2 Asymptotically safe Quantum Gravity Nonperturbative renormalizability and fractal space-times Frank Saueressig Institute for Theoretical Physics & Spinoza Institute Utrecht University Rapporteur
More informationBenefits of Objective Collapse Models for Cosmology and Quantum Gravity
DOI 10.1007/s10701-014-9772-6 Benefits of Objective Collapse Models for Cosmology and Quantum Gravity Elias Okon Daniel Sudarsky Received: 24 September 2013 / Accepted: 6 January 2014 Springer Science+Business
More informationCosmic Large-scale Structure Formations
Cosmic Large-scale Structure Formations Bin HU bhu@bnu.edu.cn Astro@BNU Office: 京师 大厦 9907 18 weeks outline Background (1 w) universe geometry and matter components (1 hr) Standard candle (SNIa) (0.5 hr)
More informationInflation. Week 9. ASTR/PHYS 4080: Introduction to Cosmology
Inflation ASTR/PHYS 4080: Intro to Cosmology Week 9 1 Successes of the Hot Big Bang Model Consists of: General relativity Cosmological principle Known atomic/nuclear/particle physics Explains: dark night
More informationCOSMIC INFLATION AND THE REHEATING OF THE UNIVERSE
COSMIC INFLATION AND THE REHEATING OF THE UNIVERSE Francisco Torrentí - IFT/UAM Valencia Students Seminars - December 2014 Contents 1. The Friedmann equations 2. Inflation 2.1. The problems of hot Big
More informationStatistical anisotropy in the inflationary universe
Statistical anisotropy in the inflationary universe Yuri Shtanov Bogolyubov Institute for Theoretical Physics, Kiev, Ukraine Grassmannian Conference, Szczecin (2009) Outline Primordial spectrum after inflation
More informationCosmology and particle physics
Cosmology and particle physics Lecture notes Timm Wrase Lecture 9 Inflation - part I Having discussed the thermal history of our universe and in particular its evolution at times larger than 10 14 seconds
More informationIntro to Inflationary Cosmology
Times are bad. Children no longer obey their parents and everyone is writing a book. Cicero, 43 BC Bruce A. Bassett Intro to Inflationary Cosmology SAAO & UCT Cosmic Problem 1 : Isotropy COBE satellite
More informationArchaeology of Our Universe YIFU CAI ( 蔡一夫 )
Archaeology of Our Universe YIFU CAI ( 蔡一夫 ) 2013-11-05 Thermal History Primordial era 13.8 billion years by WMAP/NASA Large Scale Structure (LSS) by 2MASS Cosmic Microwave Background (CMB) by ESA/Planck
More informationPrimordial Perturbations from Anisotropic Inflation
89 Chapter 4 Primordial Perturbations from Anisotropic Inflation We examine cosmological perturbations in a dynamical theory of inflation in which an abelian gauge field couples directly to the inflaton,
More informationMP463 QUANTUM MECHANICS
MP463 QUANTUM MECHANICS Introduction Quantum theory of angular momentum Quantum theory of a particle in a central potential - Hydrogen atom - Three-dimensional isotropic harmonic oscillator (a model of
More informationSupergravity and inflationary cosmology Ana Achúcarro
Supergravity and inflationary cosmology Ana Achúcarro Supergravity and inflationary cosmology Slow roll inflation with fast turns: Features of heavy physics in the CMB with J-O. Gong, S. Hardeman, G. Palma,
More informationIntroduction to Cosmology
Introduction to Cosmology Subir Sarkar CERN Summer training Programme, 22-28 July 2008 Seeing the edge of the Universe: From speculation to science Constructing the Universe: The history of the Universe:
More informationCosmic Inflation Tutorial
Cosmic Inflation Tutorial Andreas Albrecht Center for Quantum Mathematics and Physics (QMAP) and Department of Physics UC Davis Simons Workshop on Quantum Information in Cosmology Niels Bohr Institute
More informationPrimordial perturbations from inflation. David Langlois (APC, Paris)
Primordial perturbations from inflation David Langlois (APC, Paris) Cosmological evolution Homogeneous and isotropic Universe Einstein s equations Friedmann equations The Universe in the Past The energy
More informationAnisotropic signatures in cosmic structures from primordial tensor perturbations
Anisotropic signatures in cosmic structures from primordial tensor perturbations Emanuela Dimastrogiovanni FTPI, Univ. of Minnesota Cosmo 2014, Chicago based on:!! ED, M. Fasiello, D. Jeong, M. Kamionkowski!
More informationCover Page. The handle holds various files of this Leiden University dissertation.
Cover Page The handle http://hdl.handle.net/1887/28941 holds various files of this Leiden University dissertation. Author: Ortiz, Pablo Title: Effects of heavy fields on inflationary cosmology Issue Date:
More informationLeptogenesis via Higgs Condensate Relaxation
The Motivation Quantum Fluctuations Higgs Relaxation Leptogenesis Summary Leptogenesis via Higgs Condensate Relaxation Louis Yang Department of Physics and Astronomy University of California, Los Angeles
More informationINFLATION. - EARLY EXPONENTIAL PHASE OF GROWTH OF SCALE FACTOR (after T ~ TGUT ~ GeV)
INFLATION - EARLY EXPONENTIAL PHASE OF GROWTH OF SCALE FACTOR (after T ~ TGUT ~ 10 15 GeV) -Phenomenologically similar to Universe with a dominant cosmological constant, however inflation needs to end
More informationA Covariant Natural Ultraviolet Cutoff in Inflationary Cosmology
A Covariant Natural Ultraviolet Cutoff in Inflationary Cosmology by Aidan Chatwin-Davies A thesis presented to the University of Waterloo in fulfillment of the thesis requirement for the degree of Master
More informationQuantum Mechanics in the de Sitter Spacetime and Inflationary Scenario
J. Astrophys. Astr. (1985) 6, 239 246 Quantum Mechanics in the de Sitter Spacetime and Inflationary Scenario Τ. Padmanabhan Tata Institute of Fundamental Research, Homi Bhabha Road, Bombay 400005 Received
More informationMimetic Cosmology. Alexander Vikman. New Perspectives on Cosmology Institute of Physics of the Czech Academy of Sciences
New Perspectives on Cosmology Mimetic Cosmology Alexander Vikman Institute of Physics of the Czech Academy of Sciences 07.01.2016 This talk is mostly based on arxiv: 1512.09118, K. Hammer, A. Vikman arxiv:
More informationHiggs Inflation Mikhail Shaposhnikov SEWM, Montreal, 29 June - 2 July 2010
Higgs Inflation Mikhail Shaposhnikov SEWM, Montreal, 29 June - 2 July 2010 SEWM, June 29 - July 2 2010 p. 1 Original part based on: F. Bezrukov, M. S., Phys. Lett. B 659 (2008) 703 F. Bezrukov, D. Gorbunov,
More informationPOST-INFLATIONARY HIGGS RELAXATION AND THE ORIGIN OF MATTER- ANTIMATTER ASYMMETRY
POST-INFLATIONARY HIGGS RELAXATION AND THE ORIGIN OF MATTER- ANTIMATTER ASYMMETRY LOUIS YANG ( 楊智軒 ) UNIVERSITY OF CALIFORNIA, LOS ANGELES (UCLA) DEC 27, 2016 NATIONAL TSING HUA UNIVERSITY OUTLINE Big
More informationMulti-Field Inflation with a Curved Field-Space Metric
Multi-Field Inflation with a Curved Field-Space Metric A senior thesis submitted in partial fulfillment of the requirement for the degree of Bachelor of Science in Physics from the College of William and
More informationCosmic Variance of the Three-Point Correlation Function of the Cosmic Microwave Background
CfPA 93 th 18 astro-ph/9306012 June 1993 REVISED arxiv:astro-ph/9306012v2 14 Jul 1993 Cosmic Variance of the Three-Point Correlation Function of the Cosmic Microwave Background Mark Srednicki* Center for
More information