Getting to the Heart of Matter

Total Page:16

File Type:pdf, Size:1020Kb

Getting to the Heart of Matter Getting to the Heart of Matter: New Ways to Understand the Mass We See and Don't See in the World Around Us Extraordinary progress has been made over the past decade in understanding masses of "elementary" particles, the building blocks that make up all matter we know about in the universe. That progress was accompanied by great surprises: supposedly mass-less neutrinos have been shown to possess mass. Most of the mass in our galaxy and elsewhere in the universe appears to be in the form of "dark matter", particles not yet detected in the laboratory. In the "Standard Model" of particle physics, mass derives from interactions of quarks and leptons -- the constituents of all known matter -- with a new kind of particle or field, called the "Higgs particle". The Higgs particle also remains elusive. New scientific tools -- including the Large Hadron Collider which will be coming online next year -- may be able to shed light on the nature of dark matter and the Higgs particle. If history is any guide, the new tools will also create their own surprises. The talk will cover some of the recent highlights in the historic quest to understand the basic forces and building blocks of all matter and energy and it will preview the new tools and how they plan to carry on this quest. 1 Einstein (1905, ff.) E hc m = E = mm= c2 λ and, the World is made of atoms! Last year, we celebrated the centenary of Einstein’s annus mirabilis: 5 remarkable papers that changed physics. We will use 3 equations of Einstein in our examination of mass In the universe. The first, and to most physicists, the most radical of that year, proposed that light— radiation—was not continuous, but consisted of particles we now call photons which carry a definite quantum of energy depending on their wavelength. This is the work for which he received the Nobel Prize. His formula for representing this idea is the centerpiece of this slide. The formula on the left came from his final paper of 1905 in an addendum to his “relativity” paper; in slightly different form, it is the most famous formula in science. In the present form, however, it achieves its “Einsteinian” significance: “The mass of a body is a measure of its energy content;” He went on to say: “If theory agrees with the facts, then radiation carries inertia between emitting and absorbing bodies.” (Comment: energy from the stars; accelerators.) The third formula is Einstein’s somewhat later postulate, the equivalence principle, stating that the two Newtonian concepts of mass, inertial and gravitational, are equivalent. Taken as icons, these three formulas represent modern physics, the joining of relativity and quantum theory to describe our world of atoms and nuclei in all their diversity and Einstein’s theory of gravity, “General Relativity.” His other two papers that year essentially closed any remaining debate on the atomic picture of the structure of matter. 2 Goals of particle physics to find out: What is the world made of? How does it work? Answer: it depends on where you look. Physics recognizes 4 basic forces in nature: gravity, electromagnetism, a strong force responsible for binding nuclei of atoms and a weak force involved in certain kinds of radioactive decay. At the largest scales we know about, gravity is the dominant force, shaping the universe around us. At our scale, gravity is important, but we begin to sense the importance of the other forces and by the time we examine physics at the scale of atoms and smaller, gravity is completely negligible and the other forces dominate. 20th century physics revealed the nature of these forces at the atomic scale and smaller, the particles that make up all the matter around us, and the theoretical tools needed to understand their interactions down to distances ~1/1000 the size of atomic nuclei, our present horizon of understand of the very small. At much smaller distances—the “Planck scale”—it is expected that gravity will return to be the dominant force. 3 E hc m = E = c2 λ Progress in understanding the structure of atoms and their nuclei during the 2nd half of the 20th century was achieved by remarkable advances in particle accelerators and detectors. The photo above shows Fermilab, outside Chicago, which has operated the world’s highest energy accelerator—the Tevatron—over the past 20 years (along with other, lower-energy machines). In the Tevatron, counter-rotating beams of protons and their antiparticle, antiprotons, collide in the center of large detectors, such as “CDF” shown, which analyze particles produced in the collisions. Physicists use detectors to “see” trails of ionization left by charged particles produced in the collisions as they pass through matter. In these experiments, direct use is made of Einstein’s relationship between mass and energy. New massive particles are created from the energy achieved by the accelerator. The study of the new particles and their interactions reveals details of the underlying physics down to scales of distance related to energy by Einstein’s “photon” relationship. The 50 “golden-years” of accelerator-driven particle physics can be broken into two major periods: 1947-1974 experimental and theoretical discoveries leading to the “Standard Model”, post-1974 testing the SM and searching for physics “beyond the Standard Model” 4 Standard Model ca. Nov. 1974 — today nt t n c n m t u b e m s e d Leptons Quarks + forces unified through hidden Mass of quarks and charged leptons symmetries, all described by acquired through interactions with a relativistic quantum field theory new field filling all space: The Higgs The Standard Model represents the culmination of the 20th Century quest to understand the basic building blocks of all matter and the forces that operate between building blocks. It posits matter as being made from two classes of objects: quarks and leptons. Quarks participate in the strong nuclear force and are the distinguishing constituents of the nuclei of atoms. Leptons do not respond to the strong force, but interact with the other known forces, electromagnetism, weak and gravity, in the same way as do quarks. The Standard Model is based on symmetry principles requiring the quarks and leptons to have exactly zero mass. It accommodates the evident fact that particles carry mass by introducing a new field which fills all space, the “Higgs field”. Quarks and the charged leptons acquire their masses by they way they “attach” to the Higgs field. The precise date I’ve given to the acceptance of the Standard Model corresponds to the start of a revolutionary set of experiments which began on this day in 1974 at the Stanford Linear Accelerator Center. That was a Saturday; by the following Monday the world of particle physics had entered its “November Revolution” which, over the next few weeks and months, joined in a remarkable consensus on the validity of the Standard Model. To date, there are no experimental conflicts with predictions of the SM, but as we shall see, there certainly are important questions not understood within the Standard Model. Review what was so special about the Nov. revolution and the next generation of discoveries to where we stand today. 5 Weighing Nothing E hc m = E = c2 λ How mass is described in the Standard Model: The SM uses elegant symmetry arguments to describe and unify the strong, electromagnetic and weak forces. The symmetries invoked rely on having all particles—quarks and leptons—exactly massless. The symmetry is broken in our world by the introduction of a new field filling all space, the Higgs field. Interactions between the quarks and charged leptons and the Higgs field given them their apparent mass. Nuclei of atoms gain additional mass from the energy content associated with binding quarks in nuclei. The diversity of masses between, say, the electron and the top quark is large, about 1 : 1/3 million The three neutrinos sit outside this picture. They don’t stick to the Higgs field in the way quarks and charged leptons do. They don’t bind together to acquire internal energy and, hence, mass. They were expected to retain their masslessness in the real world. It was known since the early days of nuclear physics that neutrinos must have tiny masses at most, much less than the electron, for example. Starting nearly 40 years ago, there started to appear data indicating something was wrong with neutrinos that travel long distances, first from the sun, then in the upper reaches of the earth’s atmosphere and now in accelerator experiments. 2002 NP, SNO & MINOS @ UT Unavoidable conclusion: neutrinos have definite mass, small but not zero. 6 Weighing Nearly Everything mm= For decades, astronomers have sought to measure the total mass “out there” in our universe. In both Newton’s theory of gravity and Einstein’s, an object in orbit around other things must move with a speed that depends on the total mass inside its orbit. Too slow and it falls in; too fast and it sails off. So, by measuring the speed of stars orbiting on the fringes of galaxies, one can determine the total mass of all the stuff in the galaxy! (Naturally, some simple equations from Einstein tell how to relate shifts in the apparent color of stars to their speed around their galaxy—just like Doppler radar!) Historically big putdown: what we actually see in galaxies—all the stars and other exotic things—represents only a few percent of the mass of the galaxy, itself! Another several percent is probably in non-luminous ordinary matter, like planets and dust clouds and the like.
Recommended publications
  • Conformal Symmetry in Field Theory and in Quantum Gravity
    universe Review Conformal Symmetry in Field Theory and in Quantum Gravity Lesław Rachwał Instituto de Física, Universidade de Brasília, Brasília DF 70910-900, Brazil; [email protected] Received: 29 August 2018; Accepted: 9 November 2018; Published: 15 November 2018 Abstract: Conformal symmetry always played an important role in field theory (both quantum and classical) and in gravity. We present construction of quantum conformal gravity and discuss its features regarding scattering amplitudes and quantum effective action. First, the long and complicated story of UV-divergences is recalled. With the development of UV-finite higher derivative (or non-local) gravitational theory, all problems with infinities and spacetime singularities might be completely solved. Moreover, the non-local quantum conformal theory reveals itself to be ghost-free, so the unitarity of the theory should be safe. After the construction of UV-finite theory, we focused on making it manifestly conformally invariant using the dilaton trick. We also argue that in this class of theories conformal anomaly can be taken to vanish by fine-tuning the couplings. As applications of this theory, the constraints of the conformal symmetry on the form of the effective action and on the scattering amplitudes are shown. We also remark about the preservation of the unitarity bound for scattering. Finally, the old model of conformal supergravity by Fradkin and Tseytlin is briefly presented. Keywords: quantum gravity; conformal gravity; quantum field theory; non-local gravity; super- renormalizable gravity; UV-finite gravity; conformal anomaly; scattering amplitudes; conformal symmetry; conformal supergravity 1. Introduction From the beginning of research on theories enjoying invariance under local spacetime-dependent transformations, conformal symmetry played a pivotal role—first introduced by Weyl related changes of meters to measure distances (and also due to relativity changes of periods of clocks to measure time intervals).
    [Show full text]
  • The Universe, Life and Everything…
    Our current understanding of our world is nearly 350 years old. Durston It stems from the ideas of Descartes and Newton and has brought us many great things, including modern science and & increases in wealth, health and everyday living standards. Baggerman Furthermore, it is so engrained in our daily lives that we have forgotten it is a paradigm, not fact. However, there are some problems with it: first, there is no satisfactory explanation for why we have consciousness and experience meaning in our The lives. Second, modern-day physics tells us that observations Universe, depend on characteristics of the observer at the large, cosmic Dialogues on and small, subatomic scales. Third, the ongoing humanitarian and environmental crises show us that our world is vastly The interconnected. Our understanding of reality is expanding to Universe, incorporate these issues. In The Universe, Life and Everything... our Changing Dialogues on our Changing Understanding of Reality, some of the scholars at the forefront of this change discuss the direction it is taking and its urgency. Life Understanding Life and and Sarah Durston is Professor of Developmental Disorders of the Brain at the University Medical Centre Utrecht, and was at the Everything of Reality Netherlands Institute for Advanced Study in 2016/2017. Ton Baggerman is an economic psychologist and psychotherapist in Tilburg. Everything ISBN978-94-629-8740-1 AUP.nl 9789462 987401 Sarah Durston and Ton Baggerman The Universe, Life and Everything… The Universe, Life and Everything… Dialogues on our Changing Understanding of Reality Sarah Durston and Ton Baggerman AUP Contact information for authors Sarah Durston: [email protected] Ton Baggerman: [email protected] Cover design: Suzan Beijer grafisch ontwerp, Amersfoort Lay-out: Crius Group, Hulshout Amsterdam University Press English-language titles are distributed in the US and Canada by the University of Chicago Press.
    [Show full text]
  • Science in Nasa's Vision for Space Exploration
    SCIENCE IN NASA’S VISION FOR SPACE EXPLORATION SCIENCE IN NASA’S VISION FOR SPACE EXPLORATION Committee on the Scientific Context for Space Exploration Space Studies Board Division on Engineering and Physical Sciences THE NATIONAL ACADEMIES PRESS Washington, D.C. www.nap.edu THE NATIONAL ACADEMIES PRESS 500 Fifth Street, N.W. Washington, DC 20001 NOTICE: The project that is the subject of this report was approved by the Governing Board of the National Research Council, whose members are drawn from the councils of the National Academy of Sciences, the National Academy of Engineering, and the Institute of Medicine. The members of the committee responsible for the report were chosen for their special competences and with regard for appropriate balance. Support for this project was provided by Contract NASW 01001 between the National Academy of Sciences and the National Aeronautics and Space Administration. Any opinions, findings, conclusions, or recommendations expressed in this material are those of the authors and do not necessarily reflect the views of the sponsors. International Standard Book Number 0-309-09593-X (Book) International Standard Book Number 0-309-54880-2 (PDF) Copies of this report are available free of charge from Space Studies Board National Research Council The Keck Center of the National Academies 500 Fifth Street, N.W. Washington, DC 20001 Additional copies of this report are available from the National Academies Press, 500 Fifth Street, N.W., Lockbox 285, Washington, DC 20055; (800) 624-6242 or (202) 334-3313 (in the Washington metropolitan area); Internet, http://www.nap.edu. Copyright 2005 by the National Academy of Sciences.
    [Show full text]
  • Neutrino Mass Models: a Road Map
    Neutrino Mass Models: a road map S.F.King School of Physics and Astronomy, University of Southampton, Southampton SO17 1BJ, UK E-mail: [email protected] Abstract. In this talk we survey some of the recent promising developments in the search for the theory behind neutrino mass and mixing, and indeed all fermion masses and mixing. The talk is organized in terms of a neutrino mass models road map according to which the answers to experimental questions provide sign posts to guide us through the maze of theoretical models eventually towards a complete theory of flavour and uni¯cation. 1. Introduction It has been one of the long standing goals of theories of particle physics beyond the Standard Model (SM) to predict quark and lepton masses and mixings. With the discovery of neutrino mass and mixing, this quest has received a massive impetus. Indeed, perhaps the greatest advance in particle physics over the past decade has been the discovery of neutrino mass and mixing involving two large mixing angles commonly known as the atmospheric angle θ23 and the solar angle θ12, while the remaining mixing angle θ13, although unmeasured, is constrained to be relatively small [1]. The largeness of the two large lepton mixing angles contrasts sharply with the smallness of the quark mixing angles, and this observation, together with the smallness of neutrino masses, provides new and tantalizing clues in the search for the origin of quark and lepton flavour. However, before trying to address such questions, it is worth recalling why neutrino mass forces us to go beyond the SM.
    [Show full text]
  • Quantum Gravity from the QFT Perspective
    Quantum Gravity from the QFT perspective Ilya L. Shapiro Universidade Federal de Juiz de Fora, MG, Brazil Partial support: CNPq, FAPEMIG ICTP-SAIFR/IFT-UNESP – 1-5 April, 2019 Ilya Shapiro, Quantum Gravity from the QFT perspective April - 2019 Lecture 5. Advances topics in QG Induced gravity concept. • Effective QG: general idea. • Effective QG as effective QFT. • Where we are with QG?. • Bibliography S.L. Adler, Rev. Mod. Phys. 54 (1982) 729. S. Weinberg, Effective Field Theory, Past and Future. arXive:0908.1964[hep-th]; J.F. Donoghue, The effective field theory treatment of quantum gravity. arXive:1209.3511[gr-qc]; I.Sh., Polemic notes on IR perturbative quantum gravity. arXiv:0812.3521 [hep-th]. Ilya Shapiro, Quantum Gravity from the QFT perspective April - 2019 I. Induced gravity. The idea of induced gravity is simple, while its realization may be quite non-trivial, depending on the theory. In any case, the induced gravity concept is something absolutely necessary if we consider an interaction of gravity with matter and quantum theory concepts. I. Induced gravity from cut-off Original simplest version. Ya.B. Zeldovich, Sov. Phys. Dokl. 6 (1967) 883. A.D. Sakharov, Sov. Phys. Dokl. 12 (1968) 1040. Strong version of induced gravity is like that: Suppose that the metric has no pre-determined equations of motion. These equations result from the interaction to matter. Main advantage: Since gravity is not fundamental, but induced interaction, there is no need to quantize metric. Ilya Shapiro, Quantum Gravity from the QFT perspective April - 2019 And we already know that the semiclassical approach has no problems with renormalizability! Suppose we have a theory of quantum matter fields Φ = (ϕ, ψ, Aµ) interacting to the metric gµν .
    [Show full text]
  • A Fermi National Accelerator Laboratory
    a Fermi National Accelerator Laboratory FERMILAB-Pub-83/l&THY January, 1983 Composite Model with Confining SU(N) x SU(2)L x SU(2)K Hypercolor Carl H. Albright Fermi National Accelerator Laboratory P.O. Box 500, Batavia, Illinois 60510 and Department of Physics, Northern Illinois University* DeKalb, Illinois 60115 ABSTRACT A model of composite quarks and leptons is constructed with confining SU(N) x SU(2jL x SU(2)R hypercolor interactions such that only standard quark and lepton families appear in global SU(2)L x SU(2)K doublets. Several generations are admitted by the anomaly-matching conditions and labeled by a discrete axial symmetry. The SU(N) interactions are N independent and play the role Of technicolor. Three conserved U(l)" charges identified with Q, B - L and B + L prohibit qqq + Lc transitions. 3 Oparatrd by Unlvsrsitiae Research Association Inc. under contract with the United States Department of Energy -2- FERMILAB-Pub-83/16-THY With little or no support from the experimental realm, an extensive literature fl on the subject of composite quarks and leptons has emerged over the past few years. Many of the papers are based on the pioneering work of 't Hooft who formulated several criteria which composite models should satisfy in order to explain why quarks and leptons are nearly massless on the large energy scale where the hypercolor forces become sufficiently strong to bind the massless preons together. General searches for candidate preon models have been carried out, or specfific models themselves have been proposed, in which the fundamental preons are either all spinors or spinors and scalars and the weak gauge fields are either fundamental or composite.
    [Show full text]
  • Spontaneous Symmetry Breaking and Mass Generation As Built-In Phenomena in Logarithmic Nonlinear Quantum Theory
    Vol. 42 (2011) ACTA PHYSICA POLONICA B No 2 SPONTANEOUS SYMMETRY BREAKING AND MASS GENERATION AS BUILT-IN PHENOMENA IN LOGARITHMIC NONLINEAR QUANTUM THEORY Konstantin G. Zloshchastiev Department of Physics and Center for Theoretical Physics University of the Witwatersrand Johannesburg, 2050, South Africa (Received September 29, 2010; revised version received November 3, 2010; final version received December 7, 2010) Our primary task is to demonstrate that the logarithmic nonlinearity in the quantum wave equation can cause the spontaneous symmetry break- ing and mass generation phenomena on its own, at least in principle. To achieve this goal, we view the physical vacuum as a kind of the funda- mental Bose–Einstein condensate embedded into the fictitious Euclidean space. The relation of such description to that of the physical (relativis- tic) observer is established via the fluid/gravity correspondence map, the related issues, such as the induced gravity and scalar field, relativistic pos- tulates, Mach’s principle and cosmology, are discussed. For estimate the values of the generated masses of the otherwise massless particles such as the photon, we propose few simple models which take into account small vacuum fluctuations. It turns out that the photon’s mass can be naturally expressed in terms of the elementary electrical charge and the extensive length parameter of the nonlinearity. Finally, we outline the topological properties of the logarithmic theory and corresponding solitonic solutions. DOI:10.5506/APhysPolB.42.261 PACS numbers: 11.15.Ex, 11.30.Qc, 04.60.Bc, 03.65.Pm 1. Introduction Current observational data in astrophysics are probing a regime of de- partures from classical relativity with sensitivities that are relevant for the study of the quantum-gravity problem [1,2].
    [Show full text]
  • Magnetic Moment (G-2) and New Physics
    Magnetic moment (g − 2)µ and new physics Dominik Stöckinger Dresden Lepton Moments, July 2010 Dominik Stöckinger Magnetic moment (g − 2)µ and new physics Introduction exp SM A3σ deviation for aµ − aµ has been established! Currently: exp SM −11 aµ − aµ = (255 ± 63 ± 49) × 10 Expected with new Fermilab exp. (and th. progress): exp SM −11 aµ − aµ = (?? ± 16 ± 30) × 10 Which types of physics beyond the SM could explain this? What is the impact of aµ on physics beyond the SM? Dominik Stöckinger Magnetic moment (g − 2)µ and new physics Outline 1 Introduction 2 Different types of new physics 3 aµ, parameter measurements and model discrimination SUSY could explain the deviation Littlest Higgs (T-parity) cannot explain the deviation Randall-Sundrum models could explain the deviation 4 Conclusions Dominik Stöckinger Magnetic moment (g − 2)µ and new physics Introduction Outline 1 Introduction 2 Different types of new physics 3 aµ, parameter measurements and model discrimination SUSY could explain the deviation Littlest Higgs (T-parity) cannot explain the deviation Randall-Sundrum models could explain the deviation 4 Conclusions Dominik Stöckinger Magnetic moment (g − 2)µ and new physics Introduction Muon magnetic moment Quantum field theory: Operator: aµ µ¯ σ qνµ mµ L µν R CP-, Flavour-conserving, chirality-flipping, loop-induced 2 Heavy particles contribute ∝ mµ Mheavy Sensitive to all SM interactions Sensitive to TeV-scale new physics in a unique way Dominik Stöckinger Magnetic moment (g − 2)µ and new physics Introduction Why new physics? Big questions EWSB, Higgs, mass generation? hierarchy MPl/MW ? Naturalness? Unification of the Coupling Constants in the SM and the minimal MSSM i i α 60 α 60 1/α 1/ 1/ 1 MSSM 50 50 40 40 α 1/ 2 30 30 20 20 10 10 α 1/ 3 0 0 0 5 10 15 0 5 10 15 10log Q 10log Q dark matter? Grand Unification? .
    [Show full text]
  • Hep-Ph/9703242
    LMU–02/97 The Symmetry and the Problem of Mass Generation Harald Fritzsch Sektion Physik, Ludwig–Maximilians–Universit¨at Munchen,¨ Theresienstrasse 37, 80333 Munchen,¨ Germany (E–Mail: [email protected]–muenchen.de) Abstract The mass problem in particle physics and its impact for other fields is discussed. While the problem of the nuclear masses has been resolved within the QCD framework, many parameters of the “Standard Model” are related to the fermion sector. The origin of the fermion masses remains unresolved. We discuss attempts to explain the observed hierarchical features of the mass spectrum by a symmetry, relating the mass eigenvalues to the flavor mixing angles. Invited plenary talk given at the XXI International Colloquium on Group Theoretical Methods in Physics (Goslar, Germany, July 1996)” arXiv:hep-ph/9703242v1 5 Mar 1997 Towards the end of the last century the electron was discovered. In retrospect this discovery marked the beginning of a remarkable development, which eventually led to the emergence of the “Standard Model of Fundamental Particles and Forces” in the 70ies. According to the latter all the visible matter in the universe is composed of fundamental objects of two different categories – leptons (among them the electron) and quarks. The latter do not exist as free particles, but are bound among each other to form the protons and neutrons, the building blocks of the atomic nuclei. Symmetries have played a decisive role in this development, especially at the beginning, and group theory became since the sixties an essential tool of the particle physicists. They learned move than any other scientists that symmetry is the poetry of nature, and group theory its language.
    [Show full text]
  • Spontaneous Symmetry Breaking in the Higgs Mechanism
    Spontaneous symmetry breaking in the Higgs mechanism August 2012 Abstract The Higgs mechanism is very powerful: it furnishes a description of the elec- troweak theory in the Standard Model which has a convincing experimental ver- ification. But although the Higgs mechanism had been applied successfully, the conceptual background is not clear. The Higgs mechanism is often presented as spontaneous breaking of a local gauge symmetry. But a local gauge symmetry is rooted in redundancy of description: gauge transformations connect states that cannot be physically distinguished. A gauge symmetry is therefore not a sym- metry of nature, but of our description of nature. The spontaneous breaking of such a symmetry cannot be expected to have physical e↵ects since asymmetries are not reflected in the physics. If spontaneous gauge symmetry breaking cannot have physical e↵ects, this causes conceptual problems for the Higgs mechanism, if taken to be described as spontaneous gauge symmetry breaking. In a gauge invariant theory, gauge fixing is necessary to retrieve the physics from the theory. This means that also in a theory with spontaneous gauge sym- metry breaking, a gauge should be fixed. But gauge fixing itself breaks the gauge symmetry, and thereby obscures the spontaneous breaking of the symmetry. It suggests that spontaneous gauge symmetry breaking is not part of the physics, but an unphysical artifact of the redundancy in description. However, the Higgs mechanism can be formulated in a gauge independent way, without spontaneous symmetry breaking. The same outcome as in the account with spontaneous symmetry breaking is obtained. It is concluded that even though spontaneous gauge symmetry breaking cannot have physical consequences, the Higgs mechanism is not in conceptual danger.
    [Show full text]
  • Resolving Cosmological Singularity Problem in Logarithmic Superfluid Theory of Physical Vacuum
    XXI International Meeting of Physical Interpretations of Relativity Theory IOP Publishing Journal of Physics: Conference Series 1557 (2020) 012038 doi:10.1088/1742-6596/1557/1/012038 Resolving cosmological singularity problem in logarithmic superfluid theory of physical vacuum K G Zloshchastiev Institute of Systems Science, Durban University of Technology, Durban, South Africa E-mail: [email protected] Abstract. A paradigm of the physical vacuum as a non-trivial quantum object, such as superfluid, opens an entirely new prospective upon origins and interpretations of Lorentz symmetry and spacetime, black holes, cosmological evolution and singularities. Using the logarithmic superfluid model, one can formulate a post-relativistic theory of superfluid vacuum, which is not only essentially quantum but also successfully recovers special and general relativity in the \phononic" (low-momenta) limit. Thus, it represents spacetime as an induced observer- dependent phenomenon. We focus on the cosmological aspects of the logarithmic superfluid vacuum theory and show how can the related singularity problem be resolved in this approach. 1. Introduction It is a general consensus now that the physical vacuum, or a non-removable background, is a nontrivial object whose properties' studies are of utmost importance, because it affects the most fundamental notions our physics is based upon, such as space, time, matter, field, and fundamental symmetries. An internal structure of physical vacuum is still a subject of debates based on different views and approaches, which generally agree on the main paradigm, but differ in details; some introduction can be found in monographs by Volovik and Huang [1, 2]. It is probably Dirac who can be regarded as a forerunner of the superfluid vacuum theory (SVT).
    [Show full text]
  • 1 “A Big History of the Universe for Secondary Education” PI
    “A Big History of the Universe for Secondary Education” PI: Tara Firenzi Co-Is: Joel Primack, Ph.D, Nancy Abrams, Darrell Steely, Joel Tarbox Collaborator: Doris B. Ash, Ph.D GSR: Zoe Buck Consultant: Solana Pyne Summary Overview Over the last decade, world history and astrophysics have become more and more similar in the way they examine the origins of the universe. Principally, world historians and social science educators have come to realize that the origin of our universe is the beginning of our human story. Though the incorporation of these ideas into secondary curricula is not yet widespread, well respected efforts such as “World History for Us All,” a project of the National Center for History in Schools at UCLA, have strongly advocated for the incorporation of the history of the universe in world history curricula. As put forth by books like David Christian’s Maps of Time: An Introduction to Big History (2005), these ideas will no doubt become a more significant part of both history and science instruction in secondary schools in the near future, and make instruction in both areas more interdisciplinary. In scientific fields, of course, the importance of the origins of the universe has long been understood. Bringing us to a new level of understanding on the subject of these origins, UCSC Professor Joel Primack and Nancy Abrams have recently introduced a number of new ideas about the connections between advanced scientific theories and the historical importance of the origins of the universe as discussed in their book, The View From the Center of the Universe: Discovering Our Extraordinary Place in the Cosmos (2006).
    [Show full text]