Particle Astrophysics and Cosmology: Cosmic Laboratories for New Physics (Summary of the Snowmass 2001 P4 Working Group)
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Explain Inertial and Noninertial Frame of Reference
Explain Inertial And Noninertial Frame Of Reference Nathanial crows unsmilingly. Grooved Sibyl harlequin, his meadow-brown add-on deletes mutely. Nacred or deputy, Sterne never soot any degeneration! In inertial frames of the air, hastening their fundamental forces on two forces must be frame and share information section i am throwing the car, there is not a severe bottleneck in What city the greatest value in flesh-seconds for this deviation. The definition of key facet having a small, polished surface have a force gem about a pretend or aspect of something. Fictitious Forces and Non-inertial Frames The Coriolis Force. Indeed, for death two particles moving anyhow, a coordinate system may be found among which saturated their trajectories are rectilinear. Inertial reference frame of inertial frames of angular momentum and explain why? This is illustrated below. Use tow of reference in as sentence Sentences YourDictionary. What working the difference between inertial frame and non inertial fr. Frames of Reference Isaac Physics. In forward though some time and explain inertial and noninertial of frame to prove your measurement problem you. This circumstance undermines a defining characteristic of inertial frames: that with respect to shame given inertial frame, the other inertial frame home in uniform rectilinear motion. The redirect does not rub at any valid page. That according to whether the thaw is inertial or non-inertial In the. This follows from what Einstein formulated as his equivalence principlewhich, in an, is inspired by the consequences of fire fall. Frame of reference synonyms Best 16 synonyms for was of. How read you govern a bleed of reference? Name we will balance in noninertial frame at its axis from another hamiltonian with each printed as explained at all. -
Relativity with a Preferred Frame. Astrophysical and Cosmological Implications Monday, 21 August 2017 15:30 (30 Minutes)
6th International Conference on New Frontiers in Physics (ICNFP2017) Contribution ID: 1095 Type: Talk Relativity with a preferred frame. Astrophysical and cosmological implications Monday, 21 August 2017 15:30 (30 minutes) The present analysis is motivated by the fact that, although the local Lorentz invariance is one of thecorner- stones of modern physics, cosmologically a preferred system of reference does exist. Modern cosmological models are based on the assumption that there exists a typical (privileged) Lorentz frame, in which the universe appear isotropic to “typical” freely falling observers. The discovery of the cosmic microwave background provided a stronger support to that assumption (it is tacitly assumed that the privileged frame, in which the universe appears isotropic, coincides with the CMB frame). The view, that there exists a preferred frame of reference, seems to unambiguously lead to the abolishmentof the basic principles of the special relativity theory: the principle of relativity and the principle of universality of the speed of light. Correspondingly, the modern versions of experimental tests of special relativity and the “test theories” of special relativity reject those principles and presume that a preferred inertial reference frame, identified with the CMB frame, is the only frame in which the two-way speed of light (the average speed from source to observer and back) is isotropic while it is anisotropic in relatively moving frames. In the present study, the existence of a preferred frame is incorporated into the framework of the special relativity, based on the relativity principle and universality of the (two-way) speed of light, at the expense of the freedom in assigning the one-way speeds of light that exists in special relativity. -
The Sagnac Effect: Does It Contradict Relativity?
The Sagnac Effect: Does it Contradict Relativity? By Doug Marett 2012 A number of authors have suggested that the Sagnac effect contradicts the original postulates of Special Relativity, since the postulate of the constancy of the speed of light is violated in rotating systems. [1,2,3] Sagnac himself designed the experiment of 1913 to prove the existence of the aether [4]. Other authors have attempted to explain the effect within the theoretical framework of relativity, even going as far as calling the effect “relativistic”.[5] However, we seek in this paper to show how the Sagnac effect contravenes in principle the concept of the relativity of time and motion. To understand how this happens and its wider implications, it is necessary to look first at the concept of absolute vs. relative motion, what the Sagnac effect implies about these motions, and what follows logically about the broader notions of space and time. Early Ideas Regarding Rotation and Absolute Motion: The fundamental distinction between translational and rotational motion was first pointed out by Sir Isaac Newton, and emphasized later by the work of Ernest Mach and Heinrich Hertz. One of the first experiments on the subject was Newton’s bucket experiment of 1689. It was an experiment to demonstrate that true rotational motion cannot be defined as relative rotation of a body with respect to surrounding bodies – that true motion and rest should be defined relative to absolute space instead. In Newton’s experiment, a bucket is filled with water and hung by a rope. If the rope is twisted around and around until it is tight and then released, the bucket begins to spin rapidly, not only with respect to the observers watching it, but also with respect to the water in the bucket, which at first doesn’t move and remains flat on its surface. -
THE NONLINEAR MATTER POWER SPECTRUM1 Online Material
The Astrophysical Journal, 665:887– 898, 2007 August 20 A # 2007. The American Astronomical Society. All rights reserved. Printed in U.S.A. THE NONLINEAR MATTER POWER SPECTRUM1 Zhaoming Ma Department of Astronomy and Astrophysics and Kavli Institute for Cosmological Physics, University of Chicago, Chicago, IL 60637; [email protected] Received 2006 October 6; accepted 2007 April 30 ABSTRACT We modify the public PM code developed by Anatoly Klypin and Jon Holtzman to simulate cosmologies with arbitrary initial power spectra and the equation of state of dark energy. With this tool in hand, we perform the follow- ing studies on the matter power spectrum. With an artificial sharp peak at k 0:2 h MpcÀ1 in the initial power spec- trum, we find that the position of the peak is not shifted by nonlinear evolution. An upper limit of the shift at the level of 0.02% is achieved by fitting the power spectrum local to the peak using a power law plus a Gaussian. We also find that the existence of a peak in the linear power spectrum would boost the nonlinear power at all scales evenly. This is contrary to what the HKLM scaling relation predicts, but roughly consistent with that of the halo model. We construct dark energy models with the same linear power spectra today but different linear growth histories. We demonstrate that their nonlinear power spectra differ at the level of the maximum deviation of the corresponding linear power spectra in the past. Similarly, two constructed dark energy models with the same growth histories result in consistent nonlinear power spectra. -
Planck Early Results. XVIII. the Power Spectrum of Cosmic Infrared Background Anisotropies
A&A 536, A18 (2011) Astronomy DOI: 10.1051/0004-6361/201116461 & c ESO 2011 Astrophysics Planck early results Special feature Planck early results. XVIII. The power spectrum of cosmic infrared background anisotropies Planck Collaboration: P. A. R. Ade74, N. Aghanim48,M.Arnaud60, M. Ashdown58,4, J. Aumont48, C. Baccigalupi72,A.Balbi30, A. J. Banday78,8,65,R.B.Barreiro55, J. G. Bartlett3,56,E.Battaner80, K. Benabed49, A. Benoît47,J.-P.Bernard78,8, M. Bersanelli27,42,R.Bhatia5,K.Blagrave7,J.J.Bock56,9, A. Bonaldi38, L. Bonavera72,6,J.R.Bond7,J.Borrill64,76, F. R. Bouchet49, M. Bucher3,C.Burigana41, P. Cabella30, J.-F. Cardoso61,3,49, A. Catalano3,59, L. Cayón20, A. Challinor52,58,11, A. Chamballu45,L.-YChiang51,C.Chiang19,P.R.Christensen69,31,D.L.Clements45, S. Colombi49, F. Couchot63, A. Coulais59, B. P. Crill56,70, F. Cuttaia41,L.Danese72,R.D.Davies57,R.J.Davis57,P.deBernardis26,G.deGasperis30,A.deRosa41, G. de Zotti38,72, J. Delabrouille3, J.-M. Delouis49, F.-X. Désert44,H.Dole48, S. Donzelli42,53,O.Doré56,9,U.Dörl65, M. Douspis48, X. Dupac34, G. Efstathiou52,T.A.Enßlin65,H.K.Eriksen53, F. Finelli41, O. Forni78,8, P. Fosalba50, M. Frailis40, E. Franceschi41, S. Galeotta40, K. Ganga3,46,M.Giard78,8, G. Giardino35, Y. Giraud-Héraud3, J. González-Nuevo72,K.M.Górski56,82,J.Grain48, S. Gratton58,52, A. Gregorio28, A. Gruppuso41,F.K.Hansen53, D. Harrison52,58,G.Helou9, S. Henrot-Versillé63, D. Herranz55, S. R. Hildebrandt9,62,54,E.Hivon49, M. Hobson4,W.A.Holmes56, W. Hovest65,R.J.Hoyland54,K.M.Huffenberger81, A. -
General Relativity Requires Absolute Space and Time 1 Space
CORE Metadata, citation and similar papers at core.ac.uk Provided by CERN Document Server General Relativity Requires Amp`ere’s theory of magnetism [10]. Maxwell uni- Absolute Space and Time fied Faraday’s theory with Huyghens’ wave the- ory of light, where in Maxwell’s theory light is Rainer W. K¨uhne considered as an oscillating electromagnetic wave Lechstr. 63, 38120 Braunschweig, Germany which propagates through the luminiferous aether of Huyghens. We all know that the classical kinematics was re- placed by Einstein’s Special Relativity [11]. Less We examine two far-reaching and somewhat known is that Special Relativity is not able to an- heretic consequences of General Relativity. swer several problems that were explained by clas- (i) It requires a cosmology which includes sical mechanics. a preferred rest frame, absolute space and According to the relativity principle of Special time. (ii) A rotating universe and time travel Relativity, all inertial frames are equivalent, there are strict solutions of General Relativity. is no preferred frame. Absolute motion is not re- quired, only the relative motion between the iner- tial frames is needed. The postulated absence of an absolute frame prohibits the existence of an aether [11]. 1 Space and Time Before Gen- According to Special Relativity, each inertial eral Relativity frame has its own relative time. One can infer via the Lorentz transformations [12] on the time of the According to Aristotle, the Earth was resting in the other inertial frames. Absolute space and time do centre of the universe. He considered the terrestrial not exist. Furthermore, space is homogeneous and frame as a preferred frame and all motion relative isotropic, there does not exist any rotational axis of to the Earth as absolute motion. -
Clusters, Cosmology and Reionization from the SZ Power Spectrum
Clusters, Cosmology and Reionization from the SZ Power Spectrum Shaw et al. (10,11) Reichardt, LS, Zahn + (11) Zahn, Reichardt, LS + (11) Collaborators: D. Nagai, D. Rudd (Yale), G. Holder (McGill), Suman Bhattacharya (LANL), O. Zahn (Berkeley), O. Dore (Caltech), the SPT team. Tremendous recent progress measuring the CMB damping tail Small scales provide additional constraints Keisler+ on ★ Helium abundance ★ ns & running ★ neutrinos ..and beyond thermal & kinetic SZ CMB lensing CIB (dusty galaxies) Radio sources Reichardt+ 11 ..and beyond thermal & kinetic SZ CMB lensing CIB (dusty galaxies) Radio sources Reichardt+ 11 primordial signal secondaries & E.G. foregrounds Statistical detection of the SZE by searching for anisotropy power at small angular scales primary cmb thermal SZ kinetic SZ Amplitude of SZ power spectrum is particularly sensitive to matter power spectrum normalization simulated tsz map (Shaw+, 09) 10deg Sensitive to both the abundance of collapsed structures and the thermal pressure of the intra-cluster medium Halo model approach to calculating the tSZ power spectrum Calculate SZ power spectrum by integrating the mass function over M and z, weighted by cluster signal at a given angular scale. zmax dV Mmax dn(M, z) C = g2 dz dM y (M, z) 2 l ν dz dM | l | 0 0 volume integral cluster mass function Fourier transform of projected gas thermal pressure profiles Where does tSZ power come from? distribution of power at ell = 3000 (~3.6’) 10% 50% 90% Shaw+ (10) Low mass, high redshift contribution significant. Modelling the tSZ Power Spectrum Simple parameterized model, calibrated to observations and including cosmological scaling [Shaw+ (10), Ostriker+ (05)] ★ Gas resides in hydrostatic equilibrium in NFW dark matter halos with polytropic EoS ★ Assume some gas has radiatively cooled + formed stars. -
Cosmological Structure Formation with Modified Gravity
Cosmological Structure Formation with Modified Gravity A THESIS SUBMITTED TO THE UNIVERSITY OF MANCHESTER FOR THE DEGREE OF DOCTOR OF PHILOSOPHY IN THE FACULTY OF ENGINEERING AND PHYSICAL SCIENCES 2015 Samuel J. Cusworth School of Physics and Astronomy 2 Simulations with Modified Gravity Contents Abstract . 10 Declarations . 11 Acknowledgements . 12 The Author . 14 Supporting Publications . 15 1 Introduction 17 1.1 Introduction to Modern Cosmology . 17 1.1.1 Cosmological Principle . 17 1.1.2 Introduction to General Relativity . 18 1.1.3 Einstein’s Equations from an Action Principle . 20 1.2 Concordance Cosmology . 21 1.2.1 Background Cosmology . 21 1.2.2 The Perturbed ΛCDM universe . 23 1.2.3 Non-linear Structure Formation . 27 1.3 Observational Cosmology . 30 1.3.1 SN1a . 30 1.3.2 CMB . 30 1.3.3 Galaxy Clusters . 33 1.4 f(R) as Dark Energy . 34 1.4.1 Gravitational Field Equations . 35 1.4.2 Einstein Frame . 36 Samuel Cusworth 3 CONTENTS 1.4.3 Screening Mechanism . 37 1.4.4 Viable Models . 39 2 Simulations of Structure Formation 43 2.1 Initial Condition Generation . 44 2.2 N-body Solvers . 45 2.2.1 Tree-Based Methods . 46 2.2.2 Particle Mesh Methods . 47 2.2.3 Adaptive Grid Methods . 49 2.3 Hydrodynamics . 50 2.3.1 Smoothed Particle Hydrodynamics . 51 2.4 Measuring Large Scale Structure Statistics . 54 2.4.1 Matter Power Spectrum . 54 2.4.2 Cluster Mass Function . 55 2.5 Known Limitations . 59 2.5.1 Choice of Initial Conditions . -
The Effects of the Small-Scale Behaviour of Dark Matter Power Spectrum on CMB Spectral Distortion
Prepared for submission to JCAP The effects of the small-scale behaviour of dark matter power spectrum on CMB spectral distortion Abir Sarkar,1,2 Shiv.K.Sethi,1 Subinoy Das3 1Raman Research Institute, CV Raman Ave Sadashivnagar, Bengaluru, Karnataka 560080, India 2Indian Institute of Science,CV Raman Ave, Devasandra Layout, Bengaluru, Karnataka 560012, India 3Indian Institute of Astrophysics,100 Feet Rd, Madiwala, 2nd Block, Koramangala, Bengaluru, Karnataka 560034, India E-mail: [email protected], [email protected], [email protected] Abstract. After numerous astronomical and experimental searches, the precise particle nature of dark matter is still unknown. The standard Weakly Interacting Massive Particle(WIMP) dark mat- ter, despite successfully explaining the large-scale features of the universe, has long-standing small- scale issues. The spectral distortion in the Cosmic Microwave Background(CMB) caused by Silk damping in the pre-recombination era allows one to access information on a range of small scales 0.3Mpc <k< 104 Mpc−1, whose dynamics can be precisely described using linear theory. In this paper, we investigate the possibility of using the Silk damping induced CMB spectral distortion as a probe of the small-scale power. We consider four suggested alternative dark matter candidates— Warm Dark Matter (WDM), Late Forming Dark Matter (LFDM), Ultra Light Axion (ULA) dark matter and Charged Decaying Dark Matter (CHDM); the matter power in all these models deviate significantly from the ΛCDM model at small scales. We compute the spectral distortion of CMB for these alternative models and compare our results with the ΛCDM model. We show that the main arXiv:1701.07273v3 [astro-ph.CO] 7 Jul 2017 impact of alternative models is to alter the sub-horizon evolution of the Newtonian potential which affects the late-time behaviour of spectral distortion of CMB. -
Year 1 Cosmology Results from the Dark Energy Survey
Year 1 Cosmology Results from the Dark Energy Survey Elisabeth Krause on behalf of the Dark Energy Survey collaboration TeVPA 2017, Columbus OH Our Simple Universe On large scales, the Universe can be modeled with remarkably few parameters age of the Universe geometry of space density of atoms density of matter amplitude of fluctuations scale dependence of fluctuations [of course, details often not quite as simple] Our Puzzling Universe Ordinary Matter “Dark Energy” accelerates the expansion 5% dominates the total energy density smoothly distributed 25% acceleration first measured by SN 1998 “Dark Matter” 70% Our Puzzling Universe Ordinary Matter “Dark Energy” accelerates the expansion 5% dominates the total energy density smoothly distributed 25% acceleration first measured by SN 1998 “Dark Matter” next frontier: understand cosmological constant Λ: w ≡P/ϱ=-1? 70% magnitude of Λ very surprising dynamic dark energy varying in time and space, w(a)? breakdown of GR? Theoretical Alternatives to Dark Energy Many new DE/modified gravity theories developed over last decades Most can be categorized based on how they break GR: The only local, second-order gravitational field equations that can be derived from a four-dimensional action that is constructed solely from the metric tensor, and admitting Bianchi identities, are GR + Λ. Lovelock’s theorem (1969) [subject to viability conditions] Theoretical Alternatives to Dark Energy Many new DE/modified gravity theories developed over last decades Most can be categorized based on how they break GR: The only local, second-order gravitational field equations that can be derived from a four-dimensional action that is constructed solely from the metric tensor, and admitting Bianchi identities, are GR + Λ. -
Special Relativity: a Centenary Perspective
S´eminaire Poincar´e 1 (2005) 79 { 98 S´eminaire Poincar´e Special Relativity: A Centenary Perspective Clifford M. Will McDonnell Center for the Space Sciences and Department of Physics Washington University St. Louis MO 63130 USA Contents 1 Introduction 79 2 Fundamentals of special relativity 80 2.1 Einstein's postulates and insights . 80 2.2 Time out of joint . 81 2.3 Spacetime and Lorentz invariance . 83 2.4 Special relativistic dynamics . 84 3 Classic tests of special relativity 85 3.1 The Michelson-Morley experiment . 85 3.2 Invariance of c . 86 3.3 Time dilation . 86 3.4 Lorentz invariance and quantum mechanics . 87 3.5 Consistency tests of special relativity . 87 4 Special relativity and curved spacetime 89 4.1 Einstein's equivalence principle . 90 4.2 Metric theories of gravity . 90 4.3 Effective violations of local Lorentz invariance . 91 5 Is gravity Lorentz invariant? 92 6 Tests of local Lorentz invariance at the centenary 93 6.1 Frameworks for Lorentz symmetry violations . 93 6.2 Modern searches for Lorentz symmetry violation . 95 7 Concluding remarks 96 References . 96 1 Introduction A hundred years ago, Einstein laid the foundation for a revolution in our conception of time and space, matter and energy. In his remarkable 1905 paper \On the Electrodynamics of Moving Bodies" [1], and the follow-up note \Does the Inertia of a Body Depend upon its Energy-Content?" [2], he established what we now call special relativity as one of the two pillars on which virtually all of physics of the 20th century would be built (the other pillar being quantum mechanics). -
Cosmology from Cosmic Shear and Robustness to Data Calibration
DES-2019-0479 FERMILAB-PUB-21-250-AE Dark Energy Survey Year 3 Results: Cosmology from Cosmic Shear and Robustness to Data Calibration A. Amon,1, ∗ D. Gruen,2, 1, 3 M. A. Troxel,4 N. MacCrann,5 S. Dodelson,6 A. Choi,7 C. Doux,8 L. F. Secco,8, 9 S. Samuroff,6 E. Krause,10 J. Cordero,11 J. Myles,2, 1, 3 J. DeRose,12 R. H. Wechsler,1, 2, 3 M. Gatti,8 A. Navarro-Alsina,13, 14 G. M. Bernstein,8 B. Jain,8 J. Blazek,7, 15 A. Alarcon,16 A. Ferté,17 P. Lemos,18, 19 M. Raveri,8 A. Campos,6 J. Prat,20 C. Sánchez,8 M. Jarvis,8 O. Alves,21, 22, 14 F. Andrade-Oliveira,22, 14 E. Baxter,23 K. Bechtol,24 M. R. Becker,16 S. L. Bridle,11 H. Camacho,22, 14 A. Carnero Rosell,25, 14, 26 M. Carrasco Kind,27, 28 R. Cawthon,24 C. Chang,20, 9 R. Chen,4 P. Chintalapati,29 M. Crocce,30, 31 C. Davis,1 H. T. Diehl,29 A. Drlica-Wagner,20, 29, 9 K. Eckert,8 T. F. Eifler,10, 17 J. Elvin-Poole,7, 32 S. Everett,33 X. Fang,10 P. Fosalba,30, 31 O. Friedrich,34 E. Gaztanaga,30, 31 G. Giannini,35 R. A. Gruendl,27, 28 I. Harrison,36, 11 W. G. Hartley,37 K. Herner,29 H. Huang,38 E. M. Huff,17 D. Huterer,21 N. Kuropatkin,29 P. Leget,1 A. R. Liddle,39, 40, 41 J.