IC/80/100 (Limited Distribution) International Atomic Energy Agency

Total Page:16

File Type:pdf, Size:1020Kb

IC/80/100 (Limited Distribution) International Atomic Energy Agency 1) 2) IC/80/100 Dirac's cosmology ia baaed on his large number hypothesis ' (L.N.K.) IT.^JRNAL REPORT which ia the assumption that if two large numbers are comparable there is some (Limited distribution) deep underlying physical reason and not a mere accident. It turns-out that the International Atomic Energy Agency ratio of the estimated age of the Universe, t , to e /me (m,e being the mass •'•• and and charge of the electron, and c the speed of light) Is 7 x ic^ . Also, the fJ '• 1% ^ United Nations educational Scientific and Cultural Organization ratio of the electric to gravitational force between an electron and a proton, e /G Ma (M being the proton mass and G the gravitational "constant") is 2 * 10^. INTERN AT! C'JAl CENTRE FOR THEORETICAL PHYSICS Further, the estimated number of nucleons in the Universe, N, is of order 10 . On the basis of his L.B.H. Dirac takes G to vary inversely with time and K to vary as the square of tiae. For total conservation of energy he invokes a "negative energy *ea" vhich is not observable. (Incidentally, this problem of matter creation does not arise in Diraq's revised theory .) DIrac then DO NEUTRON STARS DISPROVE MULTIPLICATIVE CREATION constructs tvo models depending on whether matter is created uniformly through all space (additive creation) or more where more matter is present (multiplicative III DIRAC'S LARGE NUMBER HYPOTHESIS? * creation). In the one case astronomical distances scale up while in the other 1) 2) case they scale dovn, with time " '. This fact provides a test of the theory Asghar Qadir " In principle by observing 3olar system distances over sufficient periods of time. International Centre for Theoretical Physics, Trieste, Italy, Unfortunately, the test Is not very "clean" as there could be many other factors and responsible for such effects at the type of accuracy required of 10 every two years. Asif A. Mufti Before going on to consider a "clean" test of multiplicative creation Jfattamatics Department, QviaId-I-Asa»,University, Islamabad, Pakistan. in L.M.H. let us consider the conclusions of the hypothesis. It can be argued 2 that e /G Mm ia fundamental as matter is composed of atoms vhose structure ABSTRACT depends on the forces between protons and electrons. However, there aeeras Dirac's cosmologyf based on his large number hypothesis, took the to be no reason to prefer t (me /e }~ to t (Me /e2) vhich is I * 10 or gravitational coupling to be decreasing vith time and matter to be created P giP , 2 -1 as the square of time- Since the effects predicted by Dirac's theory are the ratio of t to the Planck, time ^-10 , or (me /e ) to Planck time p very small, it is difficult to find a "clean" test for it. Here we show 21 that the observed radiation fron pulsars is inconsistent with Dirac's "^lO , etc. Considering the number of dimensionless quantities that can be multiplicative creation model, in vhich the matter created is proportional constructed in this way it Is Inevitable that two or three of them are to the density of matter already present. Of course, this discussion makes comparable to an order of magnitude. Whereas an exact agreement of two no comment on the "additive creation" model, or on the revised version of forty digit numbers i£ unlikely, an order of magnitude agreement has a Dirac's theory. probability of one in forty only. If more than forty such dimensionless constants can be found then there is a certainty that at least two will agree to an order of magnitude? For this reason one may have difficulties in MIRAMARE - TRIESTE accepting the L.H.H. as such, but this does not in any way disprove Dirac's July I960 cosmology with varying <J and creation of matter. To obtain a "clean" teat of the theory we need some phenomenon in a critical state where very small effects vould make a very big difference. • To be submitted for publication. For multiplicative creation such a critical situation Is provided by neutron •• Permanent address: Mathematics Department, Quaid-i-Azam University, ster*. They radiate away a small fraction of their mass, and the effect of Islamabad, Pakistan. -Z- t.hij nsaLis luiij can be ota^rved. If they wore also "secretJng" .a'.'.er due to Now, for the observed slowing down of pulsars to be consistent with Fc,(6), multiplicative creation, the xass la»s would be drastically altered. Relying i.e. the left-hand side to be negative we must have on the observed data ve can see what limits would be imposed on the neutron 2 star Bass. Let us ccr.sider this point in more quantitative detail. dE /dt| >, 2rcc /t . (7) rad " p Since multiplicative creation requires an increase of mass proportional This equation gives a limit of the mass of the pulsars to the mass and trie square of the time, ve must have M = (8) (1) for a given amount of radiated energy. Thus the mass at time t can be expressed in terms of the mass at the present time by Using the standard method of deducing the radiated energy from the observed energy flux 5' "o n '•'•the- '-''-data "~fo r ™2 0 "•—neutro* n ~*-™ we find that 2 2 t /t ) . (2) 18 of them are entirely incompatable with multiplicative creation, as we would require them to have masses less than ICf K& , and even down to 2 x 10" M^I Thus the ratio of change of the mass of a neutron star due to multiplicative Ofthe'Other two one has a mass less than 0.06 Mfi,while the other is only creation at the present time is limited by the Ruffini limit . We conclude that apart from other considerations multiplicative creation of matter is ruled out by the existence of neutron stars. (3) According to the "traditional" neutron star model of pulsars 6) their energy loss was due to dipole radiation. It.is well known now that there are also other mechanisms responsible for energy loss ACKNOWLEDGMENTS dE ,/dt » dE ,/dt + 4E/dt , (it) One of the authors (A.Q.) would like to thank Professor Abdus Salam, rad rot the International Atomic Energy Agency and UNESCO for hospitality at the where dE /it is the total energy radiated, dE ,/dt i3 the rotational rad rot International Centre for Theoretical Physics, Trieste. energy loss given by ^/ dErot (5) (I being the moment of inertia of the neutron star, u its frequency and to the rate of decrease of frequency) and AE/dt is the non-rotational energy that could be radiated. Putting multiplicative creation into the picture we get the total energy loss dE /dt being given by dE_/dT t = -dEra d./d t + 2mc /tp (6) 1) P.A.M. Dirae, Proc. Roy. Soc. (London) A 333. l*03-ln8 (1973). Diatue*.*'.. M/M Serial Pul&ar Observed energy M 21 2T 6 2) P.A.M. Dlrac, Proc. Rcy. Soc. (London) A 338, I|39-W (X9T3). Ho. P S R * 10 cats. flux x 10 egTH./sec, * 1O gnw. * 10" 3) P.A.M. Dirac, "The large number of hypothesis ana the Einstein theory 1 0328 3.1 2.0 3.3 1.6 of gravitation", preprint of the Physics Department, Florida State University, Tallahassee, Florida. 2 0527 5.0 0-3 0.5 0.25 H. Rufflnl, Physics and Contemporary Heeds, Vol.1, Ed. Hiazuddin 3 0532» 6.1 5 » 106 a.3 " 106 U.I * 106 (Plenum Publishers, 1977). k 0628 0.6 0.5 0.83 0.U E.J. Groth, Weatron Stara. Black Holea and Binary X-Ray Sources, 5 0808 O.lt 0.03 0.05 0.02 Eds. H. Gursty and R. Ruffini (D. Riedel Publishing Co., 19T9). 6 0323 2.8 0.3 0.5 0.2 6) A. Qadir, R. Huffini and L. Violini, Lettere al Huovo Cimento 27_, 7 0833* 5 5 381-381* (1980). 1.5 7 * 10 1.2 x 10 0.6 x 10 8 083^ 1.2 1.0 1.7 0.8 7) D. ter Haar, Phys. Rep. 57-125 (1972). 9 0950 0.2 10.0 17.0 0.08 10 1133 0.* 1.0 1.7 0.8 11 1237 1.5 0.2 0.33 0.16 12 1506 1.2 5.0 8.3 k.i 13 1642 0.5 3-0 5.0 2.5 ill 17^9 3.3 1.0 1.6 0.8 15 1919 0.8 0.2 0.33 0.16 16 1929 0.5 3.0 5.0 2.5 1? 1933 6.1 u.o 6.7 3.8 US 2015 3.0 0.02 0.03 0.016 19 201*5 1.2 0.05 0.0S • 0.01*1 20 2213 1*.3 ta.O 6.6 3.3 The distance and the observed energy flux of 20 pulsars is given. On the t>a*iB of Eq.(8) and this data, the calculated upper mass limit, M, Is given in grans and solar masses. The pulsars marked with a • are not In- consistent with multiplicative creation, but the others are—even if ve alloir neutron stars with mass as little as 10~5 M« : -5- -6- CURREHT ICTP PREPRINTS ASD IHTERHAL REPORTS IC/T9/163 0. GELMIHI: The s-vave Qc5c states. ic/80/16 AHfiD OSKAlf: Tour-body problem for four bound alpha particles in 0. IC/79/165 S. MARCULBSCU and L.
Recommended publications
  • Arxiv:1904.10313V3 [Gr-Qc] 22 Oct 2020 PACS Numbers: Keywords: Entropy, Holographic Principle and CCDM Models
    Thermodynamic constraints on matter creation models R. Valentim∗ Departamento de F´ısica, Instituto de Ci^enciasAmbientais, Qu´ımicas e Farmac^euticas - ICAQF, Universidade Federal de S~aoPaulo (UNIFESP) Unidade Jos´eAlencar, Rua S~aoNicolau No. 210, 09913-030 { Diadema, SP, Brazil J. F. Jesusy Universidade Estadual Paulista (UNESP), C^ampusExperimental de Itapeva Rua Geraldo Alckmin 519, 18409-010, Vila N. Sra. de F´atima,Itapeva, SP, Brazil and Universidade Estadual Paulista (UNESP), Faculdade de Engenharia de Guaratinguet´a Departamento de F´ısica e Qu´ımica, Av. Dr. Ariberto Pereira da Cunha 333, 12516-410 - Guaratinguet´a,SP, Brazil Abstract Entropy is a fundamental concept from Thermodynamics and it can be used to study models on context of Creation Cold Dark Matter (CCDM). From conditions on the first (S_ 0)1 and ≥ second order (S¨ < 0) time derivatives of total entropy in the initial expansion of Sitter through the radiation and matter eras until the end of Sitter expansion, it is possible to estimate the intervals of parameters. The total entropy (St) is calculated as sum of the entropy at all eras (Sγ and Sm) plus the entropy of the event horizon (Sh). This term derives from the Holographic Principle where it suggests that all information is contained on the observable horizon. The main feature of this method for these models are that thermodynamic equilibrium is reached in a final de Sitter era. Total entropy of the universe is calculated with three terms: apparent horizon (Sh), entropy of matter (Sm) and entropy of radiation (Sγ). This analysis allows to estimate intervals of parameters of CCDM models.
    [Show full text]
  • European Astroparticle Physics Strategy 2017-2026 Astroparticle Physics European Consortium
    European Astroparticle Physics Strategy 2017-2026 Astroparticle Physics European Consortium August 2017 European Astroparticle Physics Strategy 2017-2026 www.appec.org Executive Summary Astroparticle physics is the fascinating field of research long-standing mysteries such as the true nature of Dark at the intersection of astronomy, particle physics and Matter and Dark Energy, the intricacies of neutrinos cosmology. It simultaneously addresses challenging and the occurrence (or non-occurrence) of proton questions relating to the micro-cosmos (the world decay. of elementary particles and their fundamental interactions) and the macro-cosmos (the world of The field of astroparticle physics has quickly celestial objects and their evolution) and, as a result, established itself as an extremely successful endeavour. is well-placed to advance our understanding of the Since 2001 four Nobel Prizes (2002, 2006, 2011 and Universe beyond the Standard Model of particle physics 2015) have been awarded to astroparticle physics and and the Big Bang Model of cosmology. the recent – revolutionary – first direct detections of gravitational waves is literally opening an entirely new One of its paths is targeted at a better understanding and exhilarating window onto our Universe. We look of cataclysmic events such as: supernovas – the titanic forward to an equally exciting and productive future. explosions marking the final evolutionary stage of massive stars; mergers of multi-solar-mass black-hole Many of the next generation of astroparticle physics or neutron-star binaries; and, most compelling of all, research infrastructures require substantial capital the violent birth and subsequent evolution of our infant investment and, for Europe to remain competitive Universe.
    [Show full text]
  • FRW Type Cosmologies with Adiabatic Matter Creation
    Brown-HET-991 March 1995 FRW Type Cosmologies with Adiabatic Matter Creation J. A. S. Lima1,2, A. S. M. Germano2 and L. R. W. Abramo1 1 Physics Department, Brown University, Providence, RI 02912,USA. 2 Departamento de F´ısica Te´orica e Experimental, Universidade Federal do Rio Grande do Norte, 59072 - 970, Natal, RN, Brazil. Abstract Some properties of cosmological models with matter creation are inves- tigated in the framework of the Friedman-Robertson-Walker (FRW) line element. For adiabatic matter creation, as developed by Prigogine arXiv:gr-qc/9511006v1 2 Nov 1995 and coworkers, we derive a simple expression relating the particle num- ber density n and energy density ρ which holds regardless of the mat- ter creation rate. The conditions to generate inflation are discussed and by considering the natural phenomenological matter creation rate ψ = 3βnH, where β is a pure number of the order of unity and H is the Hubble parameter, a minimally modified hot big-bang model is proposed. The dynamic properties of such models can be deduced from the standard ones simply by replacing the adiabatic index γ of the equation of state by an effective parameter γ∗ = γ(1 β). The − thermodynamic behavior is determined and it is also shown that ages large enough to agree with observations are obtained even given the high values of H suggested by recent measurements. 1 Introduction The origin of the material content (matter plus radiation) filling the presently observed universe remains one of the most fascinating unsolved mysteries in cosmology even though many authors worked out to understand the matter creation process and its effects on the evolution of the universe [1-27].
    [Show full text]
  • Universe Model Multicomponent
    We can’t solve problems by using the same kind of thinking we used when we created them. Albert Einstein WORLD – UNIVERSE MODEL MULTICOMPONENT DARK MATTER COSMIC GAMMA-RAY BACKGROUND Vladimir S. Netchitailo Biolase Inc., 4 Cromwell, Irvine CA 92618, USA. [email protected] ABSTRACT World – Universe Model is based on two fundamental parameters in various rational exponents: Fine-structure constant α, and dimensionless quantity Q. While α is constant, Q increases with time, and is in fact a measure of the size and the age of the World. The Model makes predictions pertaining to masses of dark matter (DM) particles and explains the diffuse cosmic gamma-ray background radiation as the sum of contributions of multicomponent self-interacting dark matter annihilation. The signatures of DM particles annihilation with predicted masses of 1.3 TeV, 9.6 GeV, 70 MeV, 340 keV, and 3.7 keV, which are calculated independently of astrophysical uncertainties, are found in spectra of the diffuse gamma-ray background and the emission of various macroobjects in the World. The correlation between different emission lines in spectra of macroobjects is connected to their structure, which depends on the composition of the core and surrounding shells made up of DM particles. Thus the diversity of Very High Energy (VHE) gamma-ray sources in the World has a clear explanation. 1 1. INTRODUCTION In 1937, Paul Dirac proposed a new basis for cosmology: the hypothesis of a time varying gravitational “constant” [1]. In 1974, Dirac added a mechanism of continuous creation of matter in the World [2]: One might assume that nucleons are created uniformly throughout space, and thus mainly in intergalactic space.
    [Show full text]
  • Searches for Leptophilic Dark Matter with Astrophysical Experiments
    . Searches for leptophilic dark matter with astrophysical experiments . Von der Fakult¨atf¨urMathematik, Informatik und Naturwissenschaften der RWTH Aachen University zur Erlangung des akademischen Grades einer Doktorin der Naturwissenschaften genehmigte Dissertation vorgelegt von M. Sc. Leila Ali Cavasonza aus Finale Ligure, Savona, Italien Berichter: Universit¨atsprofessorDr. rer. nat. Michael Kr¨amer Universit¨atsprofessorDr. rer. nat. Stefan Schael Tag der m¨undlichen Pr¨ufung: 13.05.16 Diese Dissertation ist auf den Internetseiten der Universit¨atsbibliothekonline verf¨ugbar RWTH Aachen University Leila Ali Cavasonza Institut f¨urTheoretische Teilchenphysik und Kosmologie Searches for leptophilic dark matter with astrophysical experiments PhD Thesis February 2016 Supervisors: Prof. Dr. Michael Kr¨amer Prof. Dr. Stefan Schael Zusammenfassung Suche nach leptophilischer dunkler Materie mit astrophysikalischen Experimenten Die Natur der dunklen Materie (DM) zu verstehen ist eines der wichtigsten Ziele der Teilchen- und Astroteilchenphysik. Große experimentelle Anstrengungen werden un- ternommen, um die dunkle Materie nachzuweisen, in der Annahme, dass sie neben der Gravitationswechselwirkung eine weitere Wechselwirkung mit gew¨ohnlicher Materie hat. Die dunkle Materie in unserer Galaxie k¨onnte gew¨ohnliche Teilchen durch An- nihilationsprozesse erzeugen und der kosmischen Strahlung einen zus¨atzlichen Beitrag hinzuf¨ugen.Deswegen sind pr¨aziseMessungen der Fl¨ussekosmischer Strahlung ¨außerst wichtig. Das AMS-02 Experiment misst die
    [Show full text]
  • AST4220: Cosmology I
    AST4220: Cosmology I Øystein Elgarøy 2 Contents 1 Cosmological models 1 1.1 Special relativity: space and time as a unity . 1 1.2 Curvedspacetime......................... 3 1.3 Curved spaces: the surface of a sphere . 4 1.4 The Robertson-Walker line element . 6 1.5 Redshifts and cosmological distances . 9 1.5.1 Thecosmicredshift . 9 1.5.2 Properdistance. 11 1.5.3 The luminosity distance . 13 1.5.4 The angular diameter distance . 14 1.5.5 The comoving coordinate r ............... 15 1.6 TheFriedmannequations . 15 1.6.1 Timetomemorize! . 20 1.7 Equationsofstate ........................ 21 1.7.1 Dust: non-relativistic matter . 21 1.7.2 Radiation: relativistic matter . 22 1.8 The evolution of the energy density . 22 1.9 The cosmological constant . 24 1.10 Some classic cosmological models . 26 1.10.1 Spatially flat, dust- or radiation-only models . 27 1.10.2 Spatially flat, empty universe with a cosmological con- stant............................ 29 1.10.3 Open and closed dust models with no cosmological constant.......................... 31 1.10.4 Models with more than one component . 34 1.10.5 Models with matter and radiation . 35 1.10.6 TheflatΛCDMmodel. 37 1.10.7 Models with matter, curvature and a cosmological con- stant............................ 40 1.11Horizons.............................. 42 1.11.1 Theeventhorizon . 44 1.11.2 Theparticlehorizon . 45 1.11.3 Examples ......................... 46 I II CONTENTS 1.12 The Steady State model . 48 1.13 Some observable quantities and how to calculate them . 50 1.14 Closingcomments . 52 1.15Exercises ............................. 53 2 The early, hot universe 61 2.1 Radiation temperature in the early universe .
    [Show full text]
  • Thermodynamics of Cosmological Matter Creation I
    Proc. Nati. Acad. Sci. USA Vol. 85, pp. 7428-7432, October 1988 Physics Thermodynamics of cosmological matter creation I. PRIGOGINE*t, J. GEHENIAUt, E. GUNZIGt, AND P. NARDONEt *Center for Statistical Mechanics, University of Texas, Austin, TX 78712; and tFree University of Brussels, Brussels, Belgium Contributed by I. Prigogine, June 3, 1988 ABSTRACT A type of cosmological history that includes ergy of these produced particles is then extracted from that large-scale entropy production is proposed. These cosmologies of the (classical) gravitational field (1-4). But these semiclas- are based on reinterpretation of the matter-energy stress ten- sical Einstein equations are adiabatic and reversible as well, sor in Einstein's equations. This modifies the usual adiabatic and consequently they are unable to provide the entropy energy conservation laws, thereby including irreversible mat- burst accompanying the production of matter. Moreover, the ter creation. This creation corresponds to an irreversible ener- quantum nature of these equations renders the various re- gy flow from the gravitational field to the created matter con- sults highly sensitive to quantum subtleties in curved space- stituents. This point of view results from consideration of the times such as the inevitable subtraction procedures. thermodynamics ofopen systems in the framework ofcosmolo- The aim of the present work is to overcome these prob- gy. It is shown that the second law of thermodynamics requires lems and present a phenomenological model of the origin of that space-time transforms into matter, while the inverse the instability leading from the Minkowskian vacuum to the transformation is forbidden. It appears that the usual initial present universe.
    [Show full text]
  • The Matter-Antimatter Asymmetry Problem
    Journal of High Energy Physics, Gravitation and Cosmology, 2018, 4, 166-178 http://www.scirp.org/journal/jhepgc ISSN Online: 2380-4335 ISSN Print: 2380-4327 The Matter-Antimatter Asymmetry Problem Brian Albert Robson Department of Theoretical Physics, Research School of Physics and Engineering, The Australian National University, Canberra, Australia How to cite this paper: Robson, B.A. Abstract (2018) The Matter-Antimatter Asymmetry Problem. Journal of High Energy Physics, The matter-antimatter asymmetry problem, corresponding to the virtual non- Gravitation and Cosmology, 4, 166-178. existence of antimatter in the universe, is one of the greatest mysteries of cos- https://doi.org/10.4236/jhepgc.2018.41015 mology. According to the prevailing cosmological model, the universe was created Received: December 21, 2017 in the so-called “Big Bang” from pure energy and it is generally considered Accepted: January 28, 2018 that the Big Bang and its aftermath produced equal numbers of particles and Published: January 31, 2018 antiparticles, although the universe today appears to consist almost entirely of matter rather than antimatter. This constitutes the matter-antimatter asym- Copyright © 2018 by author and Scientific Research Publishing Inc. metry problem: where have all the antiparticles gone? Within the framework This work is licensed under the Creative of the Generation Model (GM) of particle physics, it is demonstrated that the Commons Attribution International asymmetry problem may be understood in terms of the composite leptons and License (CC BY 4.0). quarks of the GM. It is concluded that there is essentially no matter-antimatter http://creativecommons.org/licenses/by/4.0/ asymmetry in the present universe and that the observed hydrogen-antihydrogen Open Access asymmetry may be understood in terms of statistical fluctuations associated with the complex many-body processes involved in the formation of either a hydrogen atom or an antihydrogen atom.
    [Show full text]
  • Unification of Electromagnetic Force and Gravity Through the Composite Photon
    Preprints (www.preprints.org) | NOT PEER-REVIEWED | Posted: 11 January 2021 doi:10.20944/preprints202101.0076.v3 Unification of Electromagnetic Force and Gravity through the Composite Photon Ian Clague M.A. Hons. (Cantab.) Abstract A deep relationship is identified between the Coulomb Force and Gravity. A gravitational constant for strong gravity is calculated from the relationship. The equivalence between mass and charge is explored. Implications are given for the expansion of Einstein’s Field Equations to include vector gravity. Keywords: Unification, Composite Photon, Negative Mass, Antimatter, Grand Unification Theory Contact: [email protected] Current Affiliation: Independent Introduction The question of whether the photon is an elementary particle or composite has been a matter of debate for almost 100 years since Louis De Broglie published his paper, A Tentative Theory of Light Quanta in 19241. De Broglie wrote “Naturally, the light quantum must have an internal binary symmetry”. The composite theory is more descriptive of reality than the elementary theory. Perkins (2014)2 finds that the composite theory predicts the Maxwell equations, while the elementary photon has been created to reflect them. He continues “In the elementary theory, it is difficult to describe the electromagnetic field with the four-component vector potential. This is because the photon has only two polarisation states. This problem does not exist with the composite photon theory.” Gauthier (2019)3 has done extensive work in this area and elaborates a composite model consisting of an electron-positron pair spinning around each other in helical motion. He finds that the parameters of energy, frequency, wavelength and helical radius of each spin-1/2, half- photon composing the double-helix photon remain the same in the transformation of the half- photons into the relativistic electron and positron quantum vortex models.
    [Show full text]
  • Majorana Neutrinos: What, Why, Where?
    Majorana Neutrinos: What, Why, Where? Francesco Vissani GSSI & LNGS WIN 2019 Conference, Bari, June 7, 2019 why known neutrinos could well be Majorana particles; the minimal formalism; relevance of the issue for the direct search of big-bang neutrinos MAJORANA’S HYPOTHESIS ON NEUTRINOS June 07, 2019 Francesco Vissani, GSSI & LNGS 2 direction of the momentum direction of the momentum 0 0 helicity distinguishes neutrinos from antineutrinos June 07, 2019 Francesco Vissani, GSSI & LNGS 3 direction of the momentum direction of the momentum 0 0 but in the rest frame there is only the spin! June 07, 2019 Francesco Vissani, GSSI & LNGS 4 direction of the momentum direction of the momentum 0 0 Majorana: in the rest frame the two states are the same June 07, 2019 Francesco Vissani, GSSI & LNGS 5 June 07, 2019 Francesco Vissani, GSSI & LNGS 6 June 07, 2019 Francesco Vissani, GSSI & LNGS 7 June 07, 2019 Francesco Vissani, GSSI & LNGS 8 June 07, 2019 Francesco Vissani, GSSI & LNGS 9 Francesco Vissani, GSSI & LNGS June 07, 2019 comments o recall: neutrino masses are necessary to explain oscillations o neutrino mass + V-A nature makes Majorana hypothesis plausible o “unusual appearance” means just “we are used to Dirac” next, one manifestation of Majorana mass – see M. Messina’s talk 10 direct search of big-bang neutrinos big-bang neutrinos produce 3 neutrino-capture lines for a radioactive target their positions depend on mi ; their 2 intensity on |Uei | 1 +βi Dirac 2 lightest neutrino gives the most R ∝U × νi C ei intense line for normal hierarchy
    [Show full text]
  • Relativistic Plasma Physics in Supercritical Fields
    Relativistic plasma physics in supercritical fields Cite as: Phys. Plasmas 27, 050601 (2020); https://doi.org/10.1063/1.5144449 Submitted: 27 December 2019 . Accepted: 23 April 2020 . Published Online: 26 May 2020 P. Zhang , S. S. Bulanov, D. Seipt , A. V. Arefiev , and A. G. R. Thomas COLLECTIONS Note: Invited Perspective Article. This paper was selected as Featured Phys. Plasmas 27, 050601 (2020); https://doi.org/10.1063/1.5144449 27, 050601 © 2020 Author(s). Physics of Plasmas PERSPECTIVE scitation.org/journal/php Relativistic plasma physics in supercritical fields Cite as: Phys. Plasmas 27, 050601 (2020); doi: 10.1063/1.5144449 Submitted: 27 December 2019 . Accepted: 23 April 2020 . Published Online: 26 May 2020 P. Zhang,1,a) S. S. Bulanov,2,b) D. Seipt,3,c) A. V. Arefiev,4,d) and A. G. R. Thomas3,e) AFFILIATIONS 1Department of Electrical and Computer Engineering, Michigan State University, East Lansing, Michigan 48824-1226, USA 2Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA 3Center for Ultrafast Optical Science, University of Michigan, Ann Arbor, Michigan 48109-2099, USA 4Department of Mechanical and Aerospace Engineering, University of California at San Diego, La Jolla, California 92093, USA Note: Invited Perspective Article. a)Electronic mail: [email protected] b)Electronic mail: [email protected] c)Electronic mail: [email protected] d)Electronic mail: aarefi[email protected] e)Electronic mail: [email protected] ABSTRACT Since the invention of chirped pulse amplification, which was recognized by a Nobel Prize in physics in 2018, there has been a continuing increase in available laser intensity. Combined with advances in our understanding of the kinetics of relativistic plasma, studies of laser–plasma interactions are entering a new regime where the physics of relativistic plasmas is strongly affected by strong-field quantum electrodynamics (QED) processes, including hard photon emission and electron–positron (eÀ–eþ) pair production.
    [Show full text]
  • Dark Matter Cosmology and Astrophysics
    Journal of High Energy Physics, Gravitation and Cosmology, 2019, 5, 999-1050 https://www.scirp.org/journal/jhepgc ISSN Online: 2380-4335 ISSN Print: 2380-4327 Dark Matter Cosmology and Astrophysics Vladimir S. Netchitailo Biolase Inc., Irvine, CA, USA How to cite this paper: Netchitailo, V.S. Abstract (2019) Dark Matter Cosmology and As- trophysics. Journal of High Energy Physics, Hypersphere World-Universe Model (WUM) envisions Matter carried from Gravitation and Cosmology, 5, 999-1050. Universe into World from fourth spatial dimension by Dark Matter Particles https://doi.org/10.4236/jhepgc.2019.54056 (DMPs). Luminous Matter is byproduct of Dark Matter (DM) annihilation. WUM introduces Dark Epoch (spanning from Beginning of World for 0.4 Received: June 27, 2019 Accepted: September 9, 2019 billion years) when only DMPs existed, and Luminous Epoch (ever since for Published: September 12, 2019 13.8 billion years). Big Bang discussed in standard cosmological model is, in our view, transition from Dark Epoch to Luminous Epoch due to Rotational Copyright © 2019 by author(s) and Fission of Overspinning DM Supercluster’s Cores and annihilation of DMPs. Scientific Research Publishing Inc. This work is licensed under the Creative WUM solves a number of physical problems in contemporary Cosmology Commons Attribution International and Astrophysics through DMPs and their interactions: Angular Momen- License (CC BY 4.0). tum problem in birth and subsequent evolution of Galaxies and Extrasolar http://creativecommons.org/licenses/by/4.0/ systems—how
    [Show full text]