Optimization of Signal Versus Background in Liquid Xe Detectors
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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. -
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. -
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]. -
A Statistical Framework for the Characterisation of WIMP Dark Matter with the LUX-ZEPLIN Experiment
A statistical framework for the characterisation of WIMP dark matter with the LUX-ZEPLIN experiment Ibles Olcina Samblas Department of Physics A thesis submitted for the degree of Doctor of Philosophy November 2019 Abstract Several pieces of astrophysical evidence, from galactic to cosmological scales, indicate that most of the mass in the universe is composed of an invisible and essentially collisionless substance known as dark matter. A leading particle candidate that could provide the role of dark matter is the Weakly Interacting Massive Particle (WIMP), which can be searched for directly on Earth via its scattering off atomic nuclei. The LUX-ZEPLIN (LZ) experiment, currently under construction, employs a multi-tonne dual-phase xenon time projection chamber to search for WIMPs in the low background environment of the Davis Campus at the Sanford Underground Research Facility (South Dakota, USA). LZ will probe WIMP interactions with unprecedented sensitivity, starting to explore regions of the WIMP parameter space where new backgrounds are expected to arise from the elastic scattering of neutrinos off xenon nuclei. In this work the theoretical and computational framework underlying the calculation of the sensitivity of the LZ experiment to WIMP-nucleus scattering interactions is presented. After its planned 1000 live days of exposure, LZ will be able to achieve a 3σ discovery for spin independent cross sections above 3.0 10 48 cm2 at 40 GeV/c2 WIMP mass or exclude at × − 90% CL a cross section of 1.3 10 48 cm2 in the absence of signal. The sensitivity of LZ × − to spin-dependent WIMP-neutron and WIMP-proton interactions is also presented. -
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. -
Book of Abstracts Ii Contents
DMSS: A Dark Matter Summer School Monday, 16 July 2018 - Friday, 20 July 2018 Other Institute Book of Abstracts ii Contents Introduction to Dark Matter .................................. 1 Supersymmetry ......................................... 1 Large Scale Structure Formation ................................ 1 Roundtable Discussions ..................................... 1 Dark Matter in the Milky Way ................................. 1 Neutrinos ............................................ 1 Direct Detection of Dark Matter ................................ 1 Roundtable Discussions ..................................... 1 Indirect Dark Matter Searches ................................. 2 Statistical Methods used in Dark Matter ............................ 2 Axions .............................................. 2 Cosmic Microwave Background ................................ 2 Non-SUSY Dark Matter ..................................... 2 Roundtable Discussions ..................................... 2 Dark Matter at the LHC ..................................... 2 Dark Energy ........................................... 2 Roundtable Discussions ..................................... 3 Roundtable Discussions ..................................... 3 Dark Matter search activity at the University of Montreal .................. 3 Extra Dimensions in High-Mass Diphoton Spectrum at 13 TeV ............... 3 The XENONnT Time Projection Chamber .......................... 4 Calibration of the XENON1T experiment at low energies using a Kr83m source . 4 Gravitational-wave -
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 -
LUX Detector
LUX results and LZ sensitivity to dark matter WIMPs Vitaly A. Kudryavtsev University of Sheffield for the LUX and LZ Collaborations Outline n Dark matter direct detection with two-phase noble element instruments. n LUX detector. n LUX results: o WIMPs – spin-independent interactions; o WIMPs – spin-dependent interactions; o Axions and axion-like particles (ALPs). o Modulation search. n LZ detector. n Backgrounds n Sensitivity to WIMPs. n Conclusions. ICNFP2018, 6 July 2018 Vitaly Kudryavtsev 2 Principle of WIMP detection in LXe TPC n Liquid xenon time projection chamber – LXe TPC. n S1 – primary scintillation. n S2 –secondary scintillation, proportional to ionisation. n Position reconstruction based on the light pattern in the PMTs and delay between S2 and S1. ICNFP2018, 6 July 2018 Vitaly Kudryavtsev 3 Advantages of LXe n Good scintillator. n Two-phase -> TPC with good position resolution. n Self-shielding. n Good discrimination between electron recoils (ERs) and nuclear recoils (NRs). n High atomic mass: spin-independent cross- section ∝ A2 n Presence of even-odd isotopes (odd number of neutrons) for spin-dependent studies. n Other physics: o Axion search, o Neutrinoless double-beta decay. LZ Collaboration, LZ TDR, 1703.09144v1 [physics.ins-det] ICNFP2018, 6 July 2018 Vitaly Kudryavtsev 4 LUX Collaboration ² Brown University ² University at Albany, SUNY ² Imperial College London ² University College London ² LIP Coimbra, Portugal ² University of California, Berkeley ² Lawrence Berkley National Laboratory ² University of California, Davis -
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 . -
Dark Matter Vienna University of Technology V2.1
Dark Matter Vienna University of Technology V2.1 Jochen Schieck and Holger Kluck Institut f¨urHochenergiephysik Nikolsdorfer Gasse 18 1050 Wien Atominstitut derTechnischen Universit¨atWien Stadionallee 2 1020 Wien Wintersemester 2017/18 18.12.2017 2 Contents 1 Introduction 7 1.1 What is "Dark Matter" . .7 1.1.1 Dark . .7 1.1.2 Matter . .7 1.1.3 Cosmology . .7 1.1.4 Massive particles as origin of "Dark Matter" . .7 1.1.5 "Dark Matter" as contribution to the energy density of the universe in Cosmology . .7 1.2 First Indication of observing "Dark Matter" . 13 1.3 Brief Introduction to Cosmology . 15 1.3.1 Special Relativity . 16 1.3.2 Differential geometry . 16 1.3.3 General Relativity . 16 1.3.4 Cosmology . 17 1.3.5 Decoupling of matter and radiation . 18 1.4 The Standard Model of Particle Physics . 19 1.4.1 The matter content of the Standard Model . 19 1.4.2 Forces within the Standard Model . 19 1.4.3 Shortcoming of the Standard Model . 20 1.4.4 Microscopic Behaviour of Gravity . 21 2 Evidence 23 2.1 Dynamics of Galaxies . 23 2.2 Gravitational Lensing . 24 2.2.1 Bullet Cluster . 31 2.3 Cosmic Microwave Background . 33 2.4 Primordial Nucleosynthesis (Big Bang Nucleosynthesis - BBN) . 35 3 Structure Evolution 39 3.1 Structure Formation . 39 3.1.1 The Classic Picture . 39 3.1.2 Structure Formation and Cosmology . 41 3.2 Model of the Dark Matter Halo in our Galaxy . 45 3 4 Unsolved Questions and Open Issues 49 4.1 Core-Cusp Problem . -
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. -
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.