Modified Teleparallel Theories of Gravity

Total Page:16

File Type:pdf, Size:1020Kb

Modified Teleparallel Theories of Gravity Modified Teleparallel theories of gravity Author: Supervisor: Sebasti´anBahamonde Dr. Christian G. B¨ohmer A thesis submitted in conformity with the requirements for the degree of PhD in Applied Mathematics Department of Mathematics Faculty of Mathematical & Physical Sciences University College London September 06, 2018 i Abstract Teleparallel gravity is an alternative formulation of gravity which has the same field equations as General Relativity (GR), therefore, it also known as the Teleparallel equivalent of General Relativity (TEGR). This theory is a gauge theory of the trans- lations with the torsion tensor being non-zero but with a vanishing curvature tensor, hence, the manifold is globally flat. An interesting approach for understanding the late-time accelerating behaviour of the Universe is called modified gravity where GR is extended or modified. In the same spirit, since TEGR is equivalent to GR, one can consider its modifications and study if they can describe the current cosmological observations. This thesis is devoted to studying several modified Teleparallel theories of gravity with emphasis on late-time cosmology. Those Teleparallel theories are in general different to the modified theories based on GR, but one can relate and clas- sify them accordingly. Various Teleparallel theories are presented and studied such as Teleparallel scalar-tensor theories, quintom models, Teleparallel non-local gravity, and f(T;B) gravity and its extensions (coupled with matter, extensions of new GR and Gauss-Bonnet) where T is the scalar torsion and B is the boundary term which ◦ is related with the Ricci scalar via R = −T + B. This thesis was completed under the supervision of Christian Bohmer¨ . ii Impact statement The new results showed in this thesis are based on eleven different published scientific papers. Basically, this thesis aimed at two directions, establishing new research into some questions within modified gravity and cosmology, in particular, for theories based on Teleparallel gravity. There is no foreseen impact outside of academia at this stage. One impact of this thesis was the possibility of determining a certain relationship between standard modified theories of gravity based on General Relativity (GR) and other modifications based on TEGR. Many of these theories were considered in isolation in the past and their relationship with other similarly looking theories was only made implicitly. Further, in this thesis, it was showed how two very popular ◦ modified theories coming from these two different approaches, f(R) (based on GR) and f(T ) gravity (based on TEGR), are related and could construct the fundamental theory underlying them both. Another impact of this thesis is related to constructing a viable modified Telepar- allel theory which could describe the evolution of the Universe without evoking any cosmological constant. This tells us that modifications of Teleparallel gravity could be good potential candidates for describing the dark energy problem. An additional impact related to a quantum gravity approach was also shown in iii this thesis. There was proposed a new non-local Teleparallel theory of gravity which is the first attempt to integrate this fundamental physical concept from quantum gravity into Teleparallel gravity. Moreover, in different studies related to non-locality (based on GR), researchers found that exponential type of couplings were able to achieve a renormalisable theory of gravity. In all of those studies, researchers put those terms by hand. In one work presented in this thesis, it was shown that these exponential couplings appear naturally by using first physical principles with the symmetries of the Lagrangian. Therefore, this study had an impact in resolving this aspect about non-locality. Preface Acknowledgments I would like to thank all the people who influenced and helped me throughout my PhD studies. Firstly, I would like to thank my supervisor Christian B¨ohmerfor his fantastic su- pervision over these four years. He has been an inspiration to me, not only as an excellent researcher but also as a person. It was very easy to be his student due to his supporting and easy going way of thinking. He has given me much good advice to become a better researcher and always been very objective and helpful. I also thank him for giving me the opportunity of doing independent research in other subjects and with other researchers. Secondly, I would like to thank all my international collaborators who have helped me to learn many different subjects and gave me the opportunity to publish different papers. Explicitly, I would like to thank in alphabetical order, the following collabo- rators: Salvatore Capozziello, Mir Faizal, Eduardo I. Guendelman, Mubasher Jamil, Francisco Lobo, Sergei D. Odintsov and Muhammad Zubair. Thirdly, I would like to thank Angela Cooper who has helped me a lot proofreading my thesis and for giving me very good feedback. I hope that she can be recover soon. I would also like to thank my friends who have supported me in this journey. Special thanks to my friends: Konstantinos F. Dialektopoulos, Manuela Irarr´azabal,Martin Krˇsˇs´ak,Catalina Maturana, Mihai Marciu, Victor Montenegro, Gabriel Saavedra, iv v Pietro Servini and Belgin Seymenoglu. I would also like to thank all my family for supporting me not only in my PhD, but in all my studies, specially my parents Hern´anand Pilar, my brothers Crist´obaland Joaqu´ınand my grandparents Fridia, Ester and Mois´es.Without them, I would not have been able to follow my dreams to study the subject that I love in a foreign country. I would also like to thank the love of my life, Maria-Jos´eVera who has been the most important person throughout this PhD. Without her love, support and caring, it would not have been possible to finish this PhD and also my life would not been so complete as it is. All the experiences shared with her gave me the power to continue and also to live the best years of my life. Finally, I would like to acknowledge financial support from the Chilean government for supporting me through my doctoral scholarship Becas Chile (CONICYT). To my family. vii List of Publications during my PhD 1. S. Bahamonde, C. G. Boehmer, S. Carloni, E. J. Copeland, W. Fang and N. Tamanini, \Dynamical systems applied to cosmology: dark energy and mod- ified gravity," [arXiv:1712.03107 [gr-qc]] (to appear in Physics Reports). 2. A. Dutta, S. Gangopadhyay, S. Bahamonde and M. Faizal, \The Effect of Modified Dispersion Relation on Dumb Holes," Int. J. Mod. Phys. D 27 (2018) 1850113, [arXiv:1805.01294 [gr-qc]]. 3. S. Bahamonde, \Generalised nonminimally gravity-matter coupled theory," Eur. Phys. J. C 78 (2018) no.4, 326, [arXiv:1709.05319 [gr-qc]]. 4. S. Bahamonde, M. Marciu and P. Rudra, \Generalised teleparallel quintom dark energy non-minimally coupled with the scalar torsion and a boundary term," JCAP 1804 (2018) no.04, 056, [arXiv:1802.09155 [gr-qc]]. 5. S. Bahamonde, M. Zubair and G. Abbas, \Thermodynamics and cosmolog- ical reconstruction in f(T;B) gravity," Phys.Dark Univ. 19 (2018) 78-90, [arXiv:1609.08373 [gr-qc]]. 6. A. Banerjee, K. Jusufi and S. Bahamonde, \Stability of a d-dimensional thin- shell wormhole surrounded by quintessence," Grav.Cosmol. 24 (2018) 1, [arXiv:1612.06892 [gr-qc]]. 7. S. Bahamonde, C. G. Boehmer and M. Krˇsˇs´ak, \New classes of modified teleparallel gravity models," Phys. Lett. B 775 (2017) 37, [arXiv:1706.04920 [gr-qc]]. 8. S. Bahamonde, S. Capozziello and K. F. Dialektopoulos, \Constraining Gen- eralized Non-local Cosmology from Noether Symmetries," Eur. Phys. J. C 77 (2017) no.11, 722, [arXiv:1708.06310 [gr-qc]]. viii 9. S. Bahamonde, C. G. Boehmer and P. Neff. \Geometrically nonlinear Cosserat elasticity in the plane: applications to chirality", Journal of Mechanics of Ma- terials and Structures 12 (2017) 689-710 [arXiv:1705.04868 [math-ph]] 10. S. Bahamonde, S. Capozziello, M. Faizal and R. C. Nunes, \Nonlocal Teleparal- lel Cosmology," Eur. Phys. J. C 77 (2017) no.9, 628, [arXiv:1709.02692 [gr-qc]]. 11. M. Zubair, S. Bahamonde and M. Jamil, \Generalized Second Law of Ther- modynamic in Modified Teleparallel Theory," Eur. Phys. J. C 77 (2017) no.7, 472, [arXiv:1604.02996 [gr-qc]]. 12. M. Azreg-A¨ınou, S. Bahamonde and M. Jamil, \Strong Gravitational Lens- ing by a Charged Kiselev Black Hole," Eur. Phys. J. C 77 (2017) no.6, 414, [arXiv:1701.02239 [gr-qc]]. 13. D. Momeni, M. Faizal, A. Myrzakul, S. Bahamonde and R. Myrzakulov, \A Holographic Bound for D3-Brane," Eur. Phys. J. C 77 (2017) no.6, 391, [arXiv:1608.08819 [hep-th]]. 14. S. Bahamonde, S. D. Odintsov, V. K. Oikonomou and P. V. Tretyakov, \De- celeration versus Acceleration Universe in Different Frames of F (R) Gravity,", Phys. Lett. B 766 (2017) 225-230, [arXiv:1701.02381 [gr-qc]]. 15. S. Bahamonde and S. Capozziello, \Noether Symmetry Approach in f(T;B) teleparallel cosmology," Eur. Phys. J. C 77 (2017) no.2, 107, [arXiv:1612.01299 [gr-qc]]. 16. N. S. Mazhari, D. Momeni, S. Bahamonde, M. Faizal and R. Myrzakulov, \Holographic Complexity and Fidelity Susceptibility as Holographic Informa- tion Dual to Different Volumes in AdS," Phys. Lett. B 766 (2017) 94, [arXiv:1609.00250 [hep-th]]. ix αβ 17. M. Zubair, F. Kousar and S. Bahamonde, \Thermodynamics in f(R; RαβR ; φ) theory of gravity," Phys. Dark Univ. 14 (2016) 116, [arXiv:1604.07213 [gr-qc]]. 18. S. Bahamonde and C. G. B¨ohmer,\Modified teleparallel theories of gravity: Gauss{Bonnet and trace extensions," Eur. Phys. J. C 76 (2016) no.10, 578, [arXiv:1606.05557 [gr-qc]]. 19. S. Bahamonde, U. Camci, S. Capozziello and M. Jamil, \Scalar-Tensor Telepar- allel Wormholes by Noether Symmetries," Phys. Rev. D 94 (2016) 084042 [arXiv:1608.03918 [gr-qc]].
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 State of the Multiverse: the String Landscape, the Cosmological Constant, and the Arrow of Time
    The State of the Multiverse: The String Landscape, the Cosmological Constant, and the Arrow of Time Raphael Bousso Center for Theoretical Physics University of California, Berkeley Stephen Hawking: 70th Birthday Conference Cambridge, 6 January 2011 RB & Polchinski, hep-th/0004134; RB, arXiv:1112.3341 The Cosmological Constant Problem The Landscape of String Theory Cosmology: Eternal inflation and the Multiverse The Observed Arrow of Time The Arrow of Time in Monovacuous Theories A Landscape with Two Vacua A Landscape with Four Vacua The String Landscape Magnitude of contributions to the vacuum energy graviton (a) (b) I Vacuum fluctuations: SUSY cutoff: ! 10−64; Planck scale cutoff: ! 1 I Effective potentials for scalars: Electroweak symmetry breaking lowers Λ by approximately (200 GeV)4 ≈ 10−67. The cosmological constant problem −121 I Each known contribution is much larger than 10 (the observational upper bound on jΛj known for decades) I Different contributions can cancel against each other or against ΛEinstein. I But why would they do so to a precision better than 10−121? Why is the vacuum energy so small? 6= 0 Why is the energy of the vacuum so small, and why is it comparable to the matter density in the present era? Recent observations Supernovae/CMB/ Large Scale Structure: Λ ≈ 0:4 × 10−121 Recent observations Supernovae/CMB/ Large Scale Structure: Λ ≈ 0:4 × 10−121 6= 0 Why is the energy of the vacuum so small, and why is it comparable to the matter density in the present era? The Cosmological Constant Problem The Landscape of String Theory Cosmology: Eternal inflation and the Multiverse The Observed Arrow of Time The Arrow of Time in Monovacuous Theories A Landscape with Two Vacua A Landscape with Four Vacua The String Landscape Many ways to make empty space Topology and combinatorics RB & Polchinski (2000) I A six-dimensional manifold contains hundreds of topological cycles.
    [Show full text]
  • Weyl Gauge-Vector and Complex Dilaton Scalar for Conformal Symmetry and Its Breaking
    1 Weyl gauge-vector and complex dilaton scalar for conformal symmetry and its breaking Hans C. Ohanian1 Abstract Instead of the scalar “dilaton” field that is usually adopted to construct conformally invariant Lagrangians for gravitation, we here propose a hybrid construction, involving both a complex dilaton scalar and a Weyl gauge- vector, in accord with Weyl’s original concept of a non-Riemannian conformal geometry with a transport law for length and time intervals, for which this gauge vector is required. Such a hybrid construction permits us to avoid the wrong sign of the dilaton kinetic term (the ghost problem) that afflicts the usual construction. The introduction of a Weyl gauge-vector and its interaction with the dilaton also has the collateral benefit of providing an explicit mechanism for spontaneous breaking of the conformal symmetry, whereby the dilaton and the Weyl gauge-vector acquire masses somewhat smaller than mP by the Coleman-Weinberg mechanism. Conformal symmetry breaking is assumed to precede inflation, which occurs later by a separate GUT or electroweak symmetry breaking, as in inflationary models based on the Higgs boson. Keywords Quantum gravity • Conformal invariance • Spontaneous symmetry breaking •Weyl length transport Publication history First arXiv publication [v1] 30 January 2015. The final publication is available at Springer via http://dx.doi.org/10.1007/s10714-016-2023-8 and in General Relativity and Gravitation, March 2016, 48:25. 1 Introduction Modifications of Einstein’s gravitational theory that incorporate local conformal symmetry—that is, invariance 2 (x ) under the transformation g( x ) e g ( x ) , where ()x is an arbitrary real function—have been exploited in attempts at the solution of various of theoretical problems, such as renormalization of the stress tensor, renormalization of quantum gravity, quantum mechanics of black holes, analytic solutions and geodesic completeness in the early universe, and the dynamics that lead to inflation by symmetry breaking.
    [Show full text]
  • Conformally Invariant Equations for Graviton 50 5.1 the Conformally Invariant System of Conformal Degree 1
    Conformally Invariant Equations for Graviton Mohsen Fathi Department of Physics, Tehran Central Branch Islamic Azad Univeristy arXiv:1210.3436v3 [physics.gen-ph] 12 Nov 2012 A thesis submitted for the Master degree Master of Science in Physics Tehran, Winter 2010 I am grateful to my supervisor Dr. Mohammad Reza Tanhayi for the helps, supports and scientific training, during this work and thereafter. Abstract Recent astrophysical data indicate that our universe might currently be in a de Sitter (dS) phase. The importance of dS space has been primarily ignited by the study of the inflationary model of the universe and the quantum gravity. As we know Einstein’s theory of gravitation (with a nonzero cosmological constant) can be interpreted as a theory of a metric field; that is, a symmetric tensor field of rank-2 on a fixed de Sitter back- ground. It has been shown the massless spin-2 Fierz-Pauli wave equation (or the linearized Einstein equation) is not conformally invariant. This result is in contrary with what we used to expect for massless theories. In this thesis we obtain conformally invariant wave equation for the massless spin-2 in the dS space. This study is motivated by the belief that confor- mal invariance may be the key to a future theory of quantum gravity. Contents Introduction 1 1 The Lorentz and the conformal groups, and the concept of invari- ance 3 1.1 Grouptheory ............................... 3 1.1.1 Orthogonalgroups ........................ 4 1.1.2 Rotationgroups.......................... 5 1.2 Invarianceunderagroupaction . 7 1.2.1 Invarianceofthelawsofphysics. 7 1.3 TheLorentzgroup ............................ 8 1.4 Theconformalgroup ..........................
    [Show full text]
  • Conformal Gravity Holography in Four Dimensions
    Loyola University Chicago Loyola eCommons Physics: Faculty Publications and Other Works Faculty Publications 2014 Conformal Gravity Holography in Four Dimensions Daniel Grumiller Maria Irakleidou Iva Lovrekovic, Robert McNees Loyola University Chicago, [email protected] Follow this and additional works at: https://ecommons.luc.edu/physics_facpubs Part of the Physics Commons Recommended Citation Grumiller, D, M Irakleidou, I Lovrekovic, and R McNees. "Conformal Gravity Holography in Four Dimensions." Physical Review Letters 112, 2014. This Article is brought to you for free and open access by the Faculty Publications at Loyola eCommons. It has been accepted for inclusion in Physics: Faculty Publications and Other Works by an authorized administrator of Loyola eCommons. For more information, please contact [email protected]. This work is licensed under a Creative Commons Attribution-Noncommercial-No Derivative Works 3.0 License. © 2014 American Physical Society. week ending PRL 112, 111102 (2014) PHYSICAL REVIEW LETTERS 21 MARCH 2014 Conformal Gravity Holography in Four Dimensions † ‡ Daniel Grumiller,1,* Maria Irakleidou,1, Iva Lovrekovic,1, and Robert McNees2,§ 1Institute for Theoretical Physics, Vienna University of Technology, Wiedner Hauptstrasse 8–10/136, A-1040 Vienna, Austria 2Department of Physics, Loyola University Chicago, Chicago, Illinois 60660, USA (Received 8 October 2013; published 18 March 2014) We formulate four-dimensional conformal gravity with (anti–)de Sitter boundary conditions that are weaker than Starobinsky boundary conditions, allowing for an asymptotically subleading Rindler term concurrent with a recent model for gravity at large distances. We prove the consistency of the variational principle and derive the holographic response functions. One of them is the conformal gravity version of the Brown–York stress tensor, the other is a “partially massless response”.
    [Show full text]
  • Rotating Black Holes in Conformal Gravity
    European Online Journal of Natural and Social Sciences 2014; www.european-science.com Vol.3, No.4 pp. 892-896 ISSN 1805-3602 Rotating black holes in conformal gravity Sara Dastan1*, Ali Farokhtabar1, Mohammad Ali Ganjali1,2, Bahare Hosseini1 1Department of Science, Faculty of Physics, Kharazmi University, Tehran, Iran 2Institute for Research in Fundamental Sciences(IPM), P.O. Box 19395-5531, Tehran, Iran *E-mail: [email protected] Received for publication: 02 June 2014. Accepted for publication: 30 September 2014. Abstract It is a long time since the motion of astronomical objects has been explained in the framework of Newtonian gravity. The great success of Newton’s law of universal gravitation in planetary motion persuaded astronomers to use this regime as a viable framework in the larger scales. Meanwhile, whenever a deviation of observed motions from expected ones were observed, the immediate question came up: should such anomalies be considered as incompleteness of laws of gravitation or as indication of the existence of unseen objects? In following we explain rotating black holes and solving this metric’s black hole with conformal gravity. Firstly explaining problem with DM then introducing conformal transformation and conformal gravity, in the last step we solve a metric for rotating black hole in the presence and absence of matter. Keywords: Rotation, Gravity, Black Holes, Conformal Gravity Introduction During the last century Einstein gravity (EG) was one the corner of theoretical physics. Despite of the success in explanation of various gravitational phenomena in nature, there are some unsolved basic problems such as singularity problem, black hole physics,… and most importantly quantum theory of gravity.
    [Show full text]
  • The Multiverse: Conjecture, Proof, and Science
    The multiverse: conjecture, proof, and science George Ellis Talk at Nicolai Fest Golm 2012 Does the Multiverse Really Exist ? Scientific American: July 2011 1 The idea The idea of a multiverse -- an ensemble of universes or of universe domains – has received increasing attention in cosmology - separate places [Vilenkin, Linde, Guth] - separate times [Smolin, cyclic universes] - the Everett quantum multi-universe: other branches of the wavefunction [Deutsch] - the cosmic landscape of string theory, imbedded in a chaotic cosmology [Susskind] - totally disjoint [Sciama, Tegmark] 2 Our Cosmic Habitat Martin Rees Rees explores the notion that our universe is just a part of a vast ''multiverse,'' or ensemble of universes, in which most of the other universes are lifeless. What we call the laws of nature would then be no more than local bylaws, imposed in the aftermath of our own Big Bang. In this scenario, our cosmic habitat would be a special, possibly unique universe where the prevailing laws of physics allowed life to emerge. 3 Scientific American May 2003 issue COSMOLOGY “Parallel Universes: Not just a staple of science fiction, other universes are a direct implication of cosmological observations” By Max Tegmark 4 Brian Greene: The Hidden Reality Parallel Universes and The Deep Laws of the Cosmos 5 Varieties of Multiverse Brian Greene (The Hidden Reality) advocates nine different types of multiverse: 1. Invisible parts of our universe 2. Chaotic inflation 3. Brane worlds 4. Cyclic universes 5. Landscape of string theory 6. Branches of the Quantum mechanics wave function 7. Holographic projections 8. Computer simulations 9. All that can exist must exist – “grandest of all multiverses” They can’t all be true! – they conflict with each other.
    [Show full text]
  • Conformally Coupled General Relativity
    universe Article Conformally Coupled General Relativity Andrej Arbuzov 1,* and Boris Latosh 2 ID 1 Bogoliubov Laboratory for Theoretical Physics, JINR, Dubna 141980, Russia 2 Dubna State University, Department of Fundamental Problems of Microworld Physics, Universitetskaya str. 19, Dubna 141982, Russia; [email protected] * Correspondence: [email protected] Received: 28 December 2017; Accepted: 7 February 2018; Published: 14 February 2018 Abstract: The gravity model developed in the series of papers (Arbuzov et al. 2009; 2010), (Pervushin et al. 2012) is revisited. The model is based on the Ogievetsky theorem, which specifies the structure of the general coordinate transformation group. The theorem is implemented in the context of the Noether theorem with the use of the nonlinear representation technique. The canonical quantization is performed with the use of reparametrization-invariant time and Arnowitt– Deser–Misner foliation techniques. Basic quantum features of the models are discussed. Mistakes appearing in the previous papers are corrected. Keywords: models of quantum gravity; spacetime symmetries; higher spin symmetry 1. Introduction General relativity forms our understanding of spacetime. It is verified by the Solar System and cosmological tests [1,2]. The recent discovery of gravitational waves provided further evidence supporting the theory’s viability in the classical regime [3–6]. Despite these successes, there are reasons to believe that general relativity is unable to provide an adequate description of gravitational phenomena in the high energy regime and should be either modified or replaced by a new theory of gravity [7–11]. One of the main issues is the phenomenon of inflation. It appears that an inflationary phase of expansion is necessary for a self-consistent cosmological model [12–14].
    [Show full text]
  • Modified Standard Einstein's Field Equations and the Cosmological
    Issue 1 (January) PROGRESS IN PHYSICS Volume 14 (2018) Modified Standard Einstein’s Field Equations and the Cosmological Constant Faisal A. Y. Abdelmohssin IMAM, University of Gezira, P.O. BOX: 526, Wad-Medani, Gezira State, Sudan Sudan Institute for Natural Sciences, P.O. BOX: 3045, Khartoum, Sudan E-mail: [email protected] The standard Einstein’s field equations have been modified by introducing a general function that depends on Ricci’s scalar without a prior assumption of the mathemat- ical form of the function. By demanding that the covariant derivative of the energy- momentum tensor should vanish and with application of Bianchi’s identity a first order ordinary differential equation in the Ricci scalar has emerged. A constant resulting from integrating the differential equation is interpreted as the cosmological constant introduced by Einstein. The form of the function on Ricci’s scalar and the cosmologi- cal constant corresponds to the form of Einstein-Hilbert’s Lagrangian appearing in the gravitational action. On the other hand, when energy-momentum is not conserved, a new modified field equations emerged, one type of these field equations are Rastall’s gravity equations. 1 Introduction term in his standard field equations to represent a kind of “anti ff In the early development of the general theory of relativity, gravity” to balance the e ect of gravitational attractions of Einstein proposed a tensor equation to mathematically de- matter in it. scribe the mutual interaction between matter-energy and Einstein modified his standard equations by introducing spacetime as [13] a term to his standard field equations including a constant which is called the cosmological constant Λ, [7] to become Rab = κTab (1.1) where κ is the Einstein constant, Tab is the energy-momen- 1 Rab − gabR + gabΛ = κTab (1.6) tum, and Rab is the Ricci curvature tensor which represents 2 geometry of the spacetime in presence of energy-momentum.
    [Show full text]
  • Gravitational Waves in Massive Conformal Gravity Arxiv:2007.03637V2 [Gr-Qc] 23 Jul 2020
    Gravitational waves in massive conformal gravity F. F. Faria ∗ Centro de Ci^enciasda Natureza, Universidade Estadual do Piau´ı, 64002-150 Teresina, PI, Brazil Abstract First, we obtain the plane wave solution of the linearized massive conformal gravity field equations. It is shown that the theory has seven physical plane waves. In addition, we investigate the gravitational radiation from binary systems in massive conformal gravity. We find that the theory with large graviton mass can reproduce the orbit of binaries by the emission of gravitational waves. arXiv:2007.03637v2 [gr-qc] 23 Jul 2020 PACS numbers: 04.50.Kd, 04.30.-w * [email protected] 1 Introduction Over the years several alternative theories of gravity have emerged in the attempt to solve some of the problems presented by the general theory of rel- ativity, such as the dark matter and dark energy problems. Besides solving these problems, for an alternative theory of gravity to be considered consis- tent, it must also reproduce the successful predictions of general relativity. One of these recently confirmed predictions is the existence of gravitational waves [1, 2, 3, 4]. Among the many alternative theories of gravity that have already studied the gravitational waves phenomenology is conformal gravity (CG). It was shown that the plane wave of this theory is composed of the usual plane wave of general relativity plus a plane wave that grows linearly in time [5], which causes the energy carried by the CG plane wave to diverges in momentum space [6]. In this paper, we intend to study the behavior of gravitational waves in another alternative theory of gravity with conformal symmetry called massive conformal gravity (MCG) [7].
    [Show full text]
  • Copyrighted Material
    ftoc.qrk 5/24/04 1:46 PM Page iii Contents Timeline v de Sitter,Willem 72 Dukas, Helen 74 Introduction 1 E = mc2 76 Eddington, Sir Arthur 79 Absentmindedness 3 Education 82 Anti-Semitism 4 Ehrenfest, Paul 85 Arms Race 8 Einstein, Elsa Löwenthal 88 Atomic Bomb 9 Einstein, Mileva Maric 93 Awards 16 Einstein Field Equations 100 Beauty and Equations 17 Einstein-Podolsky-Rosen Besso, Michele 18 Argument 101 Black Holes 21 Einstein Ring 106 Bohr, Niels Henrik David 25 Einstein Tower 107 Books about Einstein 30 Einsteinium 108 Born, Max 33 Electrodynamics 108 Bose-Einstein Condensate 34 Ether 110 Brain 36 FBI 113 Brownian Motion 39 Freud, Sigmund 116 Career 41 Friedmann, Alexander 117 Causality 44 Germany 119 Childhood 46 God 124 Children 49 Gravitation 126 Clothes 58 Gravitational Waves 128 CommunismCOPYRIGHTED 59 Grossmann, MATERIAL Marcel 129 Correspondence 62 Hair 131 Cosmological Constant 63 Heisenberg, Werner Karl 132 Cosmology 65 Hidden Variables 137 Curie, Marie 68 Hilbert, David 138 Death 70 Hitler, Adolf 141 iii ftoc.qrk 5/24/04 1:46 PM Page iv iv Contents Inventions 142 Poincaré, Henri 220 Israel 144 Popular Works 222 Japan 146 Positivism 223 Jokes about Einstein 148 Princeton 226 Judaism 149 Quantum Mechanics 230 Kaluza-Klein Theory 151 Reference Frames 237 League of Nations 153 Relativity, General Lemaître, Georges 154 Theory of 239 Lenard, Philipp 156 Relativity, Special Lorentz, Hendrik 158 Theory of 247 Mach, Ernst 161 Religion 255 Mathematics 164 Roosevelt, Franklin D. 258 McCarthyism 166 Russell-Einstein Manifesto 260 Michelson-Morley Experiment 167 Schroedinger, Erwin 261 Millikan, Robert 171 Solvay Conferences 265 Miracle Year 174 Space-Time 267 Monroe, Marilyn 179 Spinoza, Baruch (Benedictus) 268 Mysticism 179 Stark, Johannes 270 Myths and Switzerland 272 Misconceptions 181 Thought Experiments 274 Nazism 184 Time Travel 276 Newton, Isaac 188 Twin Paradox 279 Nobel Prize in Physics 190 Uncertainty Principle 280 Olympia Academy 195 Unified Theory 282 Oppenheimer, J.
    [Show full text]
  • Cosmic Microwave Background
    1 29. Cosmic Microwave Background 29. Cosmic Microwave Background Revised August 2019 by D. Scott (U. of British Columbia) and G.F. Smoot (HKUST; Paris U.; UC Berkeley; LBNL). 29.1 Introduction The energy content in electromagnetic radiation from beyond our Galaxy is dominated by the cosmic microwave background (CMB), discovered in 1965 [1]. The spectrum of the CMB is well described by a blackbody function with T = 2.7255 K. This spectral form is a main supporting pillar of the hot Big Bang model for the Universe. The lack of any observed deviations from a 7 blackbody spectrum constrains physical processes over cosmic history at redshifts z ∼< 10 (see earlier versions of this review). Currently the key CMB observable is the angular variation in temperature (or intensity) corre- lations, and to a growing extent polarization [2–4]. Since the first detection of these anisotropies by the Cosmic Background Explorer (COBE) satellite [5], there has been intense activity to map the sky at increasing levels of sensitivity and angular resolution by ground-based and balloon-borne measurements. These were joined in 2003 by the first results from NASA’s Wilkinson Microwave Anisotropy Probe (WMAP)[6], which were improved upon by analyses of data added every 2 years, culminating in the 9-year results [7]. In 2013 we had the first results [8] from the third generation CMB satellite, ESA’s Planck mission [9,10], which were enhanced by results from the 2015 Planck data release [11, 12], and then the final 2018 Planck data release [13, 14]. Additionally, CMB an- isotropies have been extended to smaller angular scales by ground-based experiments, particularly the Atacama Cosmology Telescope (ACT) [15] and the South Pole Telescope (SPT) [16].
    [Show full text]