The University of Chicago Dark Matter

Total Page:16

File Type:pdf, Size:1020Kb

The University of Chicago Dark Matter THE UNIVERSITY OF CHICAGO DARK MATTER HALOS AND THEIR ENVIRONMENTS A DISSERTATION SUBMITTED TO THE FACULTY OF THE DIVISION OF THE PHYSICAL SCIENCES IN CANDIDACY FOR THE DEGREE OF DOCTOR OF PHILOSOPHY DEPARTMENT OF ASTRONOMY & ASTROPHYSICS BY PHILIP MANSFIELD CHICAGO, ILLINOIS AUGUST 2020 Copyright c 2020 by Philip Mansfield All Rights Reserved Dedicated to the 2016-2017 students of the KICP Space Explorers program: the greatest scientists I have ever met. \To turn around that close to the summit...," Hall mused with a shake of his head on May 6 as Kropp plodded past Camp Two on his way down the mountain. \That showed incredibly good judgment on young G¨oran's part. I'm impressed - considerably more impressed than if he'd continued climbing and made the top." | Jon Krakauer, Into Thin Air, pp. 190 TABLE OF CONTENTS LIST OF FIGURES . viii LIST OF TABLES . ix ACKNOWLEDGMENTS . x ABSTRACT . xii 1 PROLOGUE . 1 2 AN INTERGALACTIC MURDER MYSTERY: WHY DO DARK MATTER HALOS DIE TOGETHER? . 7 2.1 The Setting: Galaxies and Dark Matter Halos . 7 2.1.1 Galaxies, Satellite Galaxies, and Distances . 7 2.1.2 Dark Matter . 10 2.1.3 Dark Matter Halos and Dark Matter Subhalos . 14 2.1.4 The Cosmic Web and Large Scale Structure . 19 2.2 The Crime: Assembly Bias . 22 2.3 The Suspects: Tides, Heating, and Misadventure . 25 2.4 The Plan: The Structure of This Thesis . 28 3 TECHNICAL BACKGROUND . 31 3.1 Simulations . 31 3.1.1 Force Softening . 34 3.2 Halo Finding and Halo Properties . 36 4 SPLASHBACK SHELLS OF COLD DARK MATTER HALOS . 43 4.1 Introduction . 43 4.2 Methods . 47 4.2.1 Simulations . 47 4.2.2 Algorithm Description . 48 4.2.3 Definitions of Basic Splashback Shell Properties . 55 4.2.4 Summary of the Algorithm Parameters . 56 4.3 Tests . 58 4.3.1 Comparison to Particle Trajectories . 62 4.4 Results . 63 4.4.1 Sample Selection . 63 4.4.2 Comparison With Stacked Radial Density Profiles . 65 4.4.3 Angular Median Density Profiles of Halos . 68 4.4.4 The Relationship Between Mass, Accretion Rate, and Splashback Radius 73 4.4.5 Splashback Shell Masses . 77 4.4.6 Splashback Shell Overdensities . 79 4.4.7 Splashback Shell Shapes . 79 v 4.5 Summary and Conclusions . 82 4.6 Appendices . 85 4.6.1 An Algorithm for Fast Line of Sight Density Estimates . 85 4.6.2 Splashback Candidate Filtering Algorithm . 88 4.6.3 Parameter-Specific Convergence Tests . 90 4.6.4 Setting Rkernel .............................. 91 4.6.5 Setting Nplanes .............................. 92 4.6.6 Computing Moment of Inertia-Equivalent Ellipsoidal Shell Axes . 94 5 HOW BIASED ARE COSMOLOGICAL SIMULATIONS? . 96 5.1 Introduction . 96 5.2 Methods . 99 5.2.1 Simulations and Halo Finding . 99 5.2.2 Halo Properties . 102 5.2.3 Finding Empirical \Convergence Limits" . 102 5.3 The Empirical Nvir Convergence Limits of Simulations . 111 5.3.1 Typical Convergence Limits . 111 5.3.2 Variation in Limits Between Simulations . 115 5.3.3 Differences Between Multidark and Illustris-TNG . 117 5.4 The Dependence of Halo Properties on Force Softening Scale . 119 5.4.1 Dependence of the Subhalo Mass Function on . 122 5.5 Estimating the Impact of Large on Vmax . 124 5.6 Discussion . 129 5.6.1 Timestepping as an Additional Source of Biases . 129 5.6.2 What is the \Optimal" ? . 135 5.7 Conclusion . 136 5.8 Appendices . 138 5.8.1 Recalibrating the Plummer-Equivalence Scale . 138 5.8.2 Fitting Parameters For Mean Halo Property Relations . 143 6 THE THREE CAUSES OF LOW-MASS ASSEMBLY BIAS . 145 6.1 Introduction . 145 6.2 Methods . 151 6.2.1 Simulations and codes . 151 6.2.2 Basic halo properties . 151 6.2.3 Definition of Halo Boundaries and Subhalos . 153 6.2.4 Halo Sample . 157 6.2.5 Measuring Tidal Force Strength . 158 6.2.6 Measuring Gravitational Heating . 161 6.2.7 Assembly Bias Statistics . 162 6.2.8 Measuring the Connection Between Assembly Bias and Other Variables163 6.3 Analysis . 167 6.3.1 Splashback Subhalos and Assembly Bias . 167 6.3.2 Contribution of Tidal Truncation and Gravitational Heating to As- sembly Bias . 169 vi 6.3.3 The Spatial and Concentration Distributions of the Halos Responsible for Assembly Bias . 173 6.3.4 Time and Mass Dependence of Assembly Bias . 178 6.3.5 Sensitivity to Splashback Subhalo Identification Method . 179 6.3.6 Comparison of the Bolshoi and BolshoiP Simulations . 180 6.4 Discussion . 181 6.4.1 Issues Associated with Proxy Definitions . 181 6.4.2 Sensitivity of Results to Definitional Choices . 181 6.4.3 Comparison with Previous Work . 184 6.4.4 Directions for Future Work . 188 6.5 Summary and Conclusions . 189 6.6 Appendices . 191 6.6.1 Effects of Halo Definition on Concentration in the Rockstar Halo Finder191 6.6.2 Fast Halo Containment Checks . 194 6.6.3 Tidal Force Errors . 195 6.6.4 Identifying Bound Particles in Halo Outskirts . 200 vii LIST OF FIGURES 2.1 Simulated image of a dark matter halo . 16 2.2 Simulated image of the cosmic web . 20 2.3 Qualitative illustration of assembly bias . 23 4.1 Overview of the Shellfish algorithm . 49 4.2 Shellfish surfaces compared against the density fields of several halos . 57 4.3 Convergence tests for various splashback surface properties . 59 4.4 A rare example of the Shellfish algorithm failing catastrophically . 61 4.5 Comparison between Shellfish surfaces and particle trajectories . 64 4.6 Disparity between Rsp measured by Shellfish and by stacked density profiles . 66 4.7 Demonstrations that spherically averaged profiles lead to biased Rsp: . 69 4.8 Agreement between Rsp measured by Shellfish and the median profile method 72 4.9 Fit to the Rsp(ΓDK14; ν200m; z) distribution . 74 4.10 Fit to the Msp(ΓDK14; ν200m; z) distribution . 75 4.11 Illustration of the scatter in the Msp fit. 75 4.12 Fit to the ∆sp(ΓDK14; ν200m; z) distribution . 80 4.13 The asphericity and ellipticity of splashback surfaces . 81 4.14 The alignment between the major axes of halos and their splashback surfaces . 81 4.15 Illustration of the Shellfish ray-tracing algorithm . 84 4.16 Convergence tests for Shellfish nuisance parameters . 93 5.1 Illustration of procedure for finding convergence limits . 103 5.2 The variation in Vmax convergence limits between simulations . 112 5.3 The convergence behavior of Vmax=Vvir and c=a as functions of Mvir . 113 5.4 Disagreement between Multidarkh and IllustrisTNG-Darki h i . 117 5.5 The dependence of various halo properties on force softening scale . 121 5.6 The dependence of subhalo abundances on force softening scale . 122 5.7 Analytic estimates of halo bias due to large . 130 5.8 Impact of analytic bias estimates on the full simulation suite. 131 5.9 Impact of force softening on gravitational fields and rotation curves . 139 6.1 Age-dependent clustering with and without splashback subhalos . 149 6.2 The impact of removing different halo populations on assembly bias . 167 6.3 How efficiently different cuts remove assembly bias from the entire halo population168 6.4 The distribution of different halo groups throughout the entire simulation box . 174 6.5 The distribution of different halo groups around a single dense filament . 175 6.6 The distribution of concentrations for different halo groups . 176 6.7 The mass and redshift dependence of assembly bias for different halo groups . 177 6.8 The impact of tracing age with a1=2 on assembly bias measurements . 182 6.9 The influence of Rockstar parameters on concentration measurements . 193 6.10 Tests of the errors associated with approximations of the tidal field around halos 196 viii LIST OF TABLES 3.1 Simulation parameters . ..
Recommended publications
  • Wimps and Machos ENCYCLOPEDIA of ASTRONOMY and ASTROPHYSICS
    WIMPs and MACHOs ENCYCLOPEDIA OF ASTRONOMY AND ASTROPHYSICS WIMPs and MACHOs objects that could be the dark matter and still escape detection. For example, if the Galactic halo were filled –3 . WIMP is an acronym for weakly interacting massive par- with Jupiter mass objects (10 Mo) they would not have ticle and MACHO is an acronym for massive (astrophys- been detected by emission or absorption of light. Brown . ical) compact halo object. WIMPs and MACHOs are two dwarf stars with masses below 0.08Mo or the black hole of the most popular DARK MATTER candidates. They repre- remnants of an early generation of stars would be simi- sent two very different but reasonable possibilities of larly invisible. Thus these objects are examples of what the dominant component of the universe may be. MACHOs. Other examples of this class of dark matter It is well established that somewhere between 90% candidates include primordial black holes created during and 99% of the material in the universe is in some as yet the big bang, neutron stars, white dwarf stars and vari- undiscovered form. This material is the gravitational ous exotic stable configurations of quantum fields, such glue that holds together galaxies and clusters of galaxies as non-topological solitons. and plays an important role in the history and fate of the An important difference between WIMPs and universe. Yet this material has not been directly detected. MACHOs is that WIMPs are non-baryonic and Since extensive searches have been done, this means that MACHOS are typically (but not always) formed from this mysterious material must not emit or absorb appre- baryonic material.
    [Show full text]
  • A Unifying Theory of Dark Energy and Dark Matter: Negative Masses and Matter Creation Within a Modified ΛCDM Framework J
    Astronomy & Astrophysics manuscript no. theory_dark_universe_arxiv c ESO 2018 November 5, 2018 A unifying theory of dark energy and dark matter: Negative masses and matter creation within a modified ΛCDM framework J. S. Farnes1; 2 1 Oxford e-Research Centre (OeRC), Department of Engineering Science, University of Oxford, Oxford, OX1 3QG, UK. e-mail: [email protected]? 2 Department of Astrophysics/IMAPP, Radboud University, PO Box 9010, NL-6500 GL Nijmegen, the Netherlands. Received February 23, 2018 ABSTRACT Dark energy and dark matter constitute 95% of the observable Universe. Yet the physical nature of these two phenomena remains a mystery. Einstein suggested a long-forgotten solution: gravitationally repulsive negative masses, which drive cosmic expansion and cannot coalesce into light-emitting structures. However, contemporary cosmological results are derived upon the reasonable assumption that the Universe only contains positive masses. By reconsidering this assumption, I have constructed a toy model which suggests that both dark phenomena can be unified into a single negative mass fluid. The model is a modified ΛCDM cosmology, and indicates that continuously-created negative masses can resemble the cosmological constant and can flatten the rotation curves of galaxies. The model leads to a cyclic universe with a time-variable Hubble parameter, potentially providing compatibility with the current tension that is emerging in cosmological measurements. In the first three-dimensional N-body simulations of negative mass matter in the scientific literature, this exotic material naturally forms haloes around galaxies that extend to several galactic radii. These haloes are not cuspy. The proposed cosmological model is therefore able to predict the observed distribution of dark matter in galaxies from first principles.
    [Show full text]
  • Dark Energy and Dark Matter
    Dark Energy and Dark Matter Jeevan Regmi Department of Physics, Prithvi Narayan Campus, Pokhara [email protected] Abstract: The new discoveries and evidences in the field of astrophysics have explored new area of discussion each day. It provides an inspiration for the search of new laws and symmetries in nature. One of the interesting issues of the decade is the accelerating universe. Though much is known about universe, still a lot of mysteries are present about it. The new concepts of dark energy and dark matter are being explained to answer the mysterious facts. However it unfolds the rays of hope for solving the various properties and dimensions of space. Keywords: dark energy, dark matter, accelerating universe, space-time curvature, cosmological constant, gravitational lensing. 1. INTRODUCTION observations. Precision measurements of the cosmic It was Albert Einstein first to realize that empty microwave background (CMB) have shown that the space is not 'nothing'. Space has amazing properties. total energy density of the universe is very near the Many of which are just beginning to be understood. critical density needed to make the universe flat The first property that Einstein discovered is that it is (i.e. the curvature of space-time, defined in General possible for more space to come into existence. And Relativity, goes to zero on large scales). Since energy his cosmological constant makes a prediction that is equivalent to mass (Special Relativity: E = mc2), empty space can possess its own energy. Theorists this is usually expressed in terms of a critical mass still don't have correct explanation for this but they density needed to make the universe flat.
    [Show full text]
  • Self-Interacting Inelastic Dark Matter: a Viable Solution to the Small Scale Structure Problems
    Prepared for submission to JCAP ADP-16-48/T1004 Self-interacting inelastic dark matter: A viable solution to the small scale structure problems Mattias Blennow,a Stefan Clementz,a Juan Herrero-Garciaa; b aDepartment of physics, School of Engineering Sciences, KTH Royal Institute of Tech- nology, AlbaNova University Center, 106 91 Stockholm, Sweden bARC Center of Excellence for Particle Physics at the Terascale (CoEPP), University of Adelaide, Adelaide, SA 5005, Australia Abstract. Self-interacting dark matter has been proposed as a solution to the small- scale structure problems, such as the observed flat cores in dwarf and low surface brightness galaxies. If scattering takes place through light mediators, the scattering cross section relevant to solve these problems may fall into the non-perturbative regime leading to a non-trivial velocity dependence, which allows compatibility with limits stemming from cluster-size objects. However, these models are strongly constrained by different observations, in particular from the requirements that the decay of the light mediator is sufficiently rapid (before Big Bang Nucleosynthesis) and from direct detection. A natural solution to reconcile both requirements are inelastic endothermic interactions, such that scatterings in direct detection experiments are suppressed or even kinematically forbidden if the mass splitting between the two-states is sufficiently large. Using an exact solution when numerically solving the Schr¨odingerequation, we study such scenarios and find regions in the parameter space of dark matter and mediator masses, and the mass splitting of the states, where the small scale structure problems can be solved, the dark matter has the correct relic abundance and direct detection limits can be evaded.
    [Show full text]
  • Throughout the Universe, Galaxies Are Rushing Away from Us – and from Each Other – at Tremendously High Speeds
    Our Universe Began with a Bang Throughout the Universe, galaxies are rushing away from us – and from each other – at tremendously high speeds. This fact tells us that the Universe is expanding over time. Edwin Hubble (after whom the Hubble Space Telescope was named) first measured the expansion in 1929. Observatories of the Carnegie Institution of Washington Edwin Hubble This posed a big question. If we could run the cosmic movie backward in time, would everything in the Universe be crammed together in a blazing fireball – the starting point of Edwin Hubble & Proceedings of The National Academy of Sciences Hubble’s famous diagram showing the the Big Bang? A lot of scientific distance versus velocity of the galaxies he debate and many new theories observed. The farther away the galaxies, the faster they are moving, showing that the followed Hubble’s discovery. Universe is expanding. Among those in the front lines of the debate were physicists Ralph Alpher and Robert Herman. In 1948 they predicted that an afterglow of this fireball should still exist, though at a much lower temperature than at the time of the Big Bang. Here’s why: As the Universe Fun Fact: expands, the waves of heat About radiation from the Big Bang are 1% of the stretched out, and cool from “snow” you see visible energy to infrared and on broadcast TV then to microwave wavelengths. is caused by the Microwaves are just short- cosmic microwave wavelength radio waves, the same background. form of energy used in microwave ovens. The prediction of an afterglow could be tested! Scientists began building instruments to detect this “cosmic microwave background”, or CMB.
    [Show full text]
  • Probing the Nature of Dark Matter in the Universe
    PROBING THE NATURE OF DARK MATTER IN THE UNIVERSE A Thesis Submitted For The Degree Of Doctor Of Philosophy In The Faculty Of Science by Abir Sarkar Under the supervision of Prof. Shiv K Sethi Raman Research Institute Joint Astronomy Programme (JAP) Department of Physics Indian Institute of Science BANGALORE - 560012 JULY, 2017 c Abir Sarkar JULY 2017 All rights reserved Declaration I, Abir Sarkar, hereby declare that the work presented in this doctoral thesis titled `Probing The Nature of Dark Matter in the Universe', is entirely original. This work has been carried out by me under the supervision of Prof. Shiv K Sethi at the Department of Astronomy and Astrophysics, Raman Research Institute under the Joint Astronomy Programme (JAP) of the Department of Physics, Indian Institute of Science. I further declare that this has not formed the basis for the award of any degree, diploma, membership, associateship or similar title of any university or institution. Department of Physics Abir Sarkar Indian Institute of Science Date : Bangalore, 560012 INDIA TO My family, without whose support this work could not be done Acknowledgements First and foremost I would like to thank my supervisor Prof. Shiv K Sethi in Raman Research Institute(RRI). He has always spent substantial time whenever I have needed for any academic discussions. I am thankful for his inspirations and ideas to make my Ph.D. experience produc- tive and stimulating. I am also grateful to our collaborator Prof. Subinoy Das of Indian Institute of Astrophysics, Bangalore, India. I am thankful to him for his insightful comments not only for our publica- tions but also for the thesis.
    [Show full text]
  • A New Universe to Discover: a Guide to Careers in Astronomy
    A New Universe to Discover A Guide to Careers in Astronomy Published by The American Astronomical Society What are Astronomy and Astrophysics? Ever since Galileo first turned his new-fangled one-inch “spyglass” on the moon in 1609, the popular image of the astronomer has been someone who peers through a telescope at the night sky. But astronomers virtually never put eye to lens these days. The main source of astronomical data is still photons (particles of light) from space, but the tools used to gather and analyze them are now so sophisticated that it’s no longer necessary (or even possible, in most cases) for a human eye to look through them. But for all the high-tech gadgetry, the 21st-Century astronomer is still trying to answer the same fundamental questions that puzzled Galileo: How does the universe work, and where did it come from? Webster’s dictionary defines “astronomy” as “the science that deals with the material universe beyond the earth’s atmosphere.” This definition is broad enough to include great theoretical physicists like Isaac Newton, Albert Einstein, and Stephen Hawking as well as astronomers like Copernicus, Johanes Kepler, Fred Hoyle, Edwin Hubble, Carl Sagan, Vera Rubin, and Margaret Burbidge. In fact, the words “astronomy” and “astrophysics” are pretty much interchangeable these days. Whatever you call them, astronomers seek the answers to many fascinating and fundamental questions. Among them: *Is there life beyond earth? *How did the sun and the planets form? *How old are the stars? *What exactly are dark matter and dark energy? *How did the Universe begin, and how will it end? Astronomy is a physical (non-biological) science, like physics and chemistry.
    [Show full text]
  • Dark Radiation from the Axino Solution of the Gravitino Problem
    21st of July 2011 Dark radiation from the axino solution of the gravitino problem Jasper Hasenkamp II. Institute for Theoretical Physics, University of Hamburg, Hamburg, Germany [email protected] Abstract Current observations of the cosmic microwave background could confirm an in- crease in the radiation energy density after primordial nucleosynthesis but before photon decoupling. We show that, if the gravitino problem is solved by a light axino, dark (decoupled) radiation emerges naturally in this period leading to a new upper 11 bound on the reheating temperature TR . 10 GeV. In turn, successful thermal leptogenesis might predict such an increase. The Large Hadron Collider could en- dorse this opportunity. At the same time, axion and axino can naturally form the observed dark matter. arXiv:1107.4319v2 [hep-ph] 13 Dec 2011 1 Introduction It is a new opportunity to determine the amount of radiation in the Universe from obser- vations of the cosmic microwave background (CMB) alone with precision comparable to that from big bang nucleosynthesis (BBN). Recent measurements by the Wilkinson Mi- crowave Anisotropy Probe (WMAP) [1], the Atacama Cosmology Telescope (ACT) [2] and the South Pole Telescope (SPT) [3] indicate|statistically not significant|the radi- ation energy density at the time of photon decoupling to be higher than inferred from primordial nucleosynthesis in standard cosmology making use of the Standard Model of particle physics, cf. [4,5]. This could be taken as another hint for physics beyond the two standard models. The Planck satellite, which is already taking data, could turn the hint into a discovery. We should search for explanations from particle physics for such an increase in ra- diation [6,7], especially, because other explanations are missing, if the current mean values are accurate.
    [Show full text]
  • Collider Signatures of Axino and Gravitino Dark Matter
    2005 International Linear Collider Workshop - Stanford, U.S.A. Collider Signatures of Axino and Gravitino Dark Matter Frank Daniel Steffen DESY Theory Group, Notkestrasse 85, 22603 Hamburg, Germany The axino and the gravitino are extremely weakly interacting candidates for the lightest supersymmetric particle (LSP). We demonstrate that either of them could provide the right amount of cold dark matter. Assuming that a charged slepton is the next-to-lightest supersymmetric particle (NLSP), we discuss how NLSP decays into the axino/gravitino LSP can provide evidence for axino/gravitino dark matter at future colliders. We show that these NLSP decays will allow us to estimate the value of the Peccei–Quinn scale and the axino mass if the axino is the LSP. In the case of the gravitino LSP, we illustrate that the gravitino mass can be determined. This is crucial for insights into the mechanism of supersymmetry breaking and can lead to a microscopic measurement of the Planck scale. 1. INTRODUCTION A key problem in cosmology is the understanding of the nature of cold dark matter. In supersymmetric extensions of the Standard Model, the lightest supersymmetric particle (LSP) is stable if R-parity is conserved [1]. An electrically and color neutral LSP thus appears as a compelling solution to the dark matter problem. The lightest neutralino is such an LSP candidate from the minimal supersymmetric standard model (MSSM). Here we consider two well- motivated alternative LSP candidates beyond the MSSM: the axino and the gravitino. In the following we introduce the axino and the gravitino. We review that axinos/gravitinos from thermal pro- duction in the early Universe can provide the right amount of cold dark matter depending on the value of the reheating temperature after inflation and the axino/gravitino mass.
    [Show full text]
  • Axion Dark Matter from Higgs Inflation with an Intermediate H∗
    Axion dark matter from Higgs inflation with an intermediate H∗ Tommi Tenkanena and Luca Visinellib;c;d aDepartment of Physics and Astronomy, Johns Hopkins University, 3400 N. Charles Street, Baltimore, MD 21218, USA bDepartment of Physics and Astronomy, Uppsala University, L¨agerhyddsv¨agen1, 75120 Uppsala, Sweden cNordita, KTH Royal Institute of Technology and Stockholm University, Roslagstullsbacken 23, 10691 Stockholm, Sweden dGravitation Astroparticle Physics Amsterdam (GRAPPA), Institute for Theoretical Physics Amsterdam and Delta Institute for Theoretical Physics, University of Amsterdam, Science Park 904, 1098 XH Amsterdam, The Netherlands E-mail: [email protected], [email protected], [email protected] Abstract. In order to accommodate the QCD axion as the dark matter (DM) in a model in which the Peccei-Quinn (PQ) symmetry is broken before the end of inflation, a relatively low scale of inflation has to be invoked in order to avoid bounds from DM isocurvature 9 fluctuations, H∗ . O(10 ) GeV. We construct a simple model in which the Standard Model Higgs field is non-minimally coupled to Palatini gravity and acts as the inflaton, leading to a 8 scale of inflation H∗ ∼ 10 GeV. When the energy scale at which the PQ symmetry breaks is much larger than the scale of inflation, we find that in this scenario the required axion mass for which the axion constitutes all DM is m0 . 0:05 µeV for a quartic Higgs self-coupling 14 λφ = 0:1, which correspond to the PQ breaking scale vσ & 10 GeV and tensor-to-scalar ratio r ∼ 10−12. Future experiments sensitive to the relevant QCD axion mass scale can therefore shed light on the physics of the Universe before the end of inflation.
    [Show full text]
  • Edwin Hubble (1889-1953) Measured Distance to Andromeda Galaxy (M31) • Noticed Individual Bright Stars in Andromeda
    The Resolution: Edwin Hubble (1889-1953) Measured Distance to Andromeda Galaxy (M31) • Noticed individual bright stars in Andromeda • Calculated the distance using the Period-Luminosity Relation for Cepheid Variable Stars The Resolution: Edwin Hubble (1889-1953) Measured Distance to Andromeda Galaxy (M31) • Noticed individual bright stars in Andromeda • Calculated the distance using the Period-Luminosity Relation for Cepheid Variable Stars 1. MEASURED magnitude & Period The Resolution: Edwin Hubble (1889-1953) Measured Distance to Andromeda Galaxy (M31) • Noticed individual bright stars in Andromeda • Calculated the distance using the Period-Luminosity Relation for Cepheid Variable Stars 1. MEASURED magnitude & Period 2. CALCULATED Luminosity The Resolution: Edwin Hubble (1889-1953) Measured Distance to Andromeda Galaxy (M31) • Noticed individual bright stars in Andromeda • Calculated the distance using the Period-Luminosity Relation for Cepheid Variable Stars 1. MEASURED magnitude & Period 2. CALCULATED Luminosity 3. CALCULATED Distance The Resolution: Edwin Hubble (1889-1953) Measured Distance to Andromeda Galaxy (M31) • Noticed individual bright stars in Andromeda • Calculated the distance using the Period-Luminosity Relation for Cepheid Variable Stars 1. MEASURED magnitude & Period 2. CALCULATED Luminosity 3. CALCULATED Distance • Result was MUCH farther than expected... • (2.3 Million Ly - well beyond Milky Way) Henrietta Leavitt & Period-Luminosity Relation Cepheid Variables: Bright stars whose Luminosity (energy output) varies every
    [Show full text]
  • Modified Newtonian Dynamics
    Faculty of Mathematics and Natural Sciences Bachelor Thesis University of Groningen Modified Newtonian Dynamics (MOND) and a Possible Microscopic Description Author: Supervisor: L.M. Mooiweer prof. dr. E. Pallante Abstract Nowadays, the mass discrepancy in the universe is often interpreted within the paradigm of Cold Dark Matter (CDM) while other possibilities are not excluded. The main idea of this thesis is to develop a better theoretical understanding of the hidden mass problem within the paradigm of Modified Newtonian Dynamics (MOND). Several phenomenological aspects of MOND will be discussed and we will consider a possible microscopic description based on quantum statistics on the holographic screen which can reproduce the MOND phenomenology. July 10, 2015 Contents 1 Introduction 3 1.1 The Problem of the Hidden Mass . .3 2 Modified Newtonian Dynamics6 2.1 The Acceleration Constant a0 .................................7 2.2 MOND Phenomenology . .8 2.2.1 The Tully-Fischer and Jackson-Faber relation . .9 2.2.2 The external field effect . 10 2.3 The Non-Relativistic Field Formulation . 11 2.3.1 Conservation of energy . 11 2.3.2 A quadratic Lagrangian formalism (AQUAL) . 12 2.4 The Relativistic Field Formulation . 13 2.5 MOND Difficulties . 13 3 A Possible Microscopic Description of MOND 16 3.1 The Holographic Principle . 16 3.2 Emergent Gravity as an Entropic Force . 16 3.2.1 The connection between the bulk and the surface . 18 3.3 Quantum Statistical Description on the Holographic Screen . 19 3.3.1 Two dimensional quantum gases . 19 3.3.2 The connection with the deep MOND limit .
    [Show full text]