|  Gravitation | 
In General
  > s.a. newtonian gravity and modifications;
  gravitational phenomenology.
  * History, I: The first systematic studies
    were carried out by Galileo (XVI century), or maybe by Riccioli; Hooke suggested that gravity
    plays a role in celestial motions, but the first precise description is Newton's (1665).
  * History, II: 1915, The equivalence principle,
    Einstein's theory of general relativity, gravity as geometry; 1920s, Cartan analyzed the
    geometric structure of Newtonian gravity (in terms of a degenerate non-dynamical metric)
    and general relativity, and introduced the concept of torsion; A general framework
    is Ehler's Frame Theory; Alternative gravity theories.
  * History, III: Various precursors are XX
    century proposals of higher-dimensional gravity, discrete theories, etc; 1990s, Beginning
    of a systematic study of phenomenology of higher-dimensional models; Quantum gravity?
  * Strength: When we jump off a ledge,
    gravity takes over, but what happens when we hit the ground below?
  * Motivation to look for new theories:
    Galactic rotation curves (unless explained by dark matter) and cosmological expansion
    acceleration (unless explained by dark energy); Eötvös-type experiments;
    Search for theory of quantum gravity and quantum corrections to classical gravity;
    (Anomalous spacecraft acceleration is now considered to have other explainations).
  @ Intros and textbooks: Schutz 03 [II];
    Olmo a1112-ch [intro];
    Gasperini 13 [II, and other interactions];
    Girifalco 14 [I];
    Fleury a1902-ln [IIb].
  @ General references: Cartan ENS(23),
    ENS(24), ENS(25);
    Mann gq/98-GR15;
    Aguirre et al CQG(01)hp [and astrophysics];
    Deser IJMPA(02)ht/01 [rev];
    Sotiriou et al IJMPD(08)-a0707 [no-progress report];
    Krasnov MPLA(07)-a0711 [non-metric theories];
    Sotiriou PhD(07)-a0712 [theory and phenomenology];
    Zee IJMPA(08)-a0805-conf [rambling talk];
    Padmanabhan FP(08) [and the equivalence principle];
    Percacci PoS-a0910
      [particle-physics perspective, gauge and renormalization];
    Ananth IJMPD(10) [and Yang-Mills theory];
    Bertolami a1112-talk;
    Starkman PTRS(11)-a1201 [and cosmology];
    Frampton & Karl a1304 [at very short distances];
    Trippe ZfN(14)-a1401 [the missing mass problem and the need for a new theory];
    Papini MPLA(14) [covariance and gauge invariance];
    Capozziello & Lambiase a1409-conf [open problems];
    Lobo JPCS(15)-a1412 [dark matter, dark energy and modified gravity];
    Strominger a1703-ln [infrared structure].
  @ History: Synge et al PRS(62),
    Hoyle et al PRS(62) [status];
    Gondhalekar 01;
    Kumar & Suresh gq/06;
    Graney PT(12)sep [Riccioli];
    Pitts a1907-ch;
    > s.a. history of relativistic physics.
  @ Speculations, origin of gravity: Mazur APPB(96)ht;
    Wootters FP(03) [from simple assumptions];
    Amelino-Camelia et al IJMPD(15)-a1505-GRF [breakdown of conformal invariance];
    Sels & Wouters JPCS(17)-a1602 [from mutual information in many-body quantum systems];
    Altamirano et al NJP(17)-a1605 [from repeated quantum measurements];
    Khosravi PRD(16)-a1606 [from ensenble average of all theoretically consistent models];
    > s.a. emergent gravity; entropic gravity;
      phenomenology of entanglement; dynamical
      wave-function collapse.
  @ Gravity as a universal force: Dieks Syn(87) [Reichenbach and Grünbaum];
    Dadhich gq/04,
    gq/04-proc [universality??].
  @ Gravity as geometry: Giesel et al PRD(12)-a1202 [based tensorial geometries other than Lorentzian geometries];
    Capozziello et al IJGMP(12)-a1202 [physical foundations, Ehlers-Pirani-Schild approach];
    Capozziello et al IJGMP(14)-a1401 [symmetries and affine structure];
    Ximenes & Biezuner a1912 [obstructions].
  > And other areas of physics:
    see modified quantum theory.
  > Online resources: see Internet Encyclopedia of Science
    pages;
    Verlinde, Wilczek and Mersini-Houghton debate.
Types of Theories  s.a. theories of gravity [including higher-spin, vector, vector-tensor, ... theories].
  s.a. theories of gravity [including higher-spin, vector, vector-tensor, ... theories].
  * General idea: The first one in the
    modern sense was Newtonian gravity (originated in the 1660s, formulated in terms
    of action at a distance); The modern  ones are usually geometrically formulated, as
    relativistic field theories; It can be fundamental or derived from other theories
    (induced gravity, AdS-cft, ...); Phenomenologically, the best motivated ones are
    scalar-tensor theories.
  * Frameworks: The main ones in which
    various theories can be included and compared are the Dicke framework [@ in Dicke
    64], and the PPN framework [which only treats
    conservative aspects, and does not include radiation]; There is also a Post-Keplerian
    framework, and Goldberger's & Rothstein's 2004 NRGR ("Non-Relativistic
    General Relativity", an unfortunate name) [this does include radiation].
  * Results: General relativity
    (or another covariant gravity theory) is intrinsically non-linear because it must be
    self-interacting or "charged" if it is to interact consistently with matter
    via its stress tensors; This can be shown by bootstrapping the theory starting from
    any background; Of all the purely metrical theories, i.e., L = L(g,
    ∂g, ∂∂g, φ, ∂φ), only general
    relativity with arbitrary matter, i.e., L = |g|1/2
    R + L(g, φ, ∂φ), gives second-order
    equations in g (and is linear in ∂∂g), and not fourth-order; A
    large class of these theories are "dynamically equivalent" to general relativity.
  * Sources of corrections:
    A graviton mass gives corrections of order \((\lambda/\lambda^{~}_{\rm Compton})^2\),
    spacetime fluctuations corrections of order \((\lambda^{~}_{\rm fundam})^2/\lambda\).
  @ General references:
    Weyl AJM(44) [as a linear field theory];
    Deser GRG(70)gq/04 [need for non-linearity];
    Ferraris & Kijowski GRG(82);
    Ferraris et al in-GR11;
    Ferraris et al CQG(88)
    + comment Brans CQG(88)
    + reply Ferraris et al CQG(90);
    Borowiec et al CQG(98)gq/96 [universality of Ricci-squared theories];
    Knox SHPMP(11)
      [empirically equivalent theories and underdetermination];
    Fabris & Velten a1501-proc [neo-Newtonian theories];
    Licata et al IJGMP(17)-a1706 [approach based on the covariant derivative commutator algebra];
    Clifton & Sanghai a1803 [parameterizations of alternative theories];
    Alex & Reinhart PRD(20)-a1909 [guide for constructing alternative theories];
    Velten & Caramês Univ(21)-a2102 [non-conserved energy-momentum];
    Böhmer & Jensko a2103 [unified approach].
  @ And matter: Pani et al PRD(13)-a1306 [auxiliary fields];
    Gümrükçüoğlu & Namba PRD(19)-a1907,
    Feng & Carloni PRD(20)-a1910 [generalized coupling].
  @ Non-relativistic theories: Kocharyan PRD(09)-a0905;
    Greenwald et al JCAP(10)-a1010 [compact objects and solar-system tests];
    > s.a. hořava-lifshitz gravity; lorentz-symmetry
      violations; newtonian gravity.
  @ As a spin-2 field theory in Minkowski space:
    Barceló et al PRD(14)-a1401,
    AP(18)-a1406 [graviton self-interactions and the cosmological constant];
    Hertzberg & Sandora JHEP(17)-a1702 [general relativity from causality];
    Blasi & Maggiore EPJC(17)-a1706 [and Fierz-Pauli theory];
    > s.a. formulations of general relativity.
  @ Other theories: Moffat EPJP(11)-a1008 [ultraviolet complete];
    Letelier a1105
      [non-covariant, with L = |g|ω R];
    Greenberger FP(12) [Tic-Tac-Toe theory, negative masses and the equivalence principle];
    Salvio & Strumia JHEP(14)-a1403 [agravity, theory without scales];
    Markou et al CQG(19)-a1811 [vierbein, antisymmetric tensor];
    Jokela et al JHEP(19)-a1901 [dual to a system of (2+1)-dimensional layers];
    > s.a. differential geometry.
   General relativity and related theories: see general relativity,
    its formulations and variants [including infrared modifications].
 General relativity and related theories: see general relativity,
    its formulations and variants [including infrared modifications].
   Modified theories: 2D and 3D theories;
    higher-dimensional gravity; higher-order theories;
    modified gravity; non-local theories.
 Modified theories: 2D and 3D theories;
    higher-dimensional gravity; higher-order theories;
    modified gravity; non-local theories.
   Other types: see ads-cft correspondence [gauge/gravity
    duality]; Constructive Gravity; Disformal Gravity;
    emergent gravity [including analog gravity]; entropic gravity;
    parity-violating theories; Projective Relativity;
    Screened Modified Gravity.
 Other types: see ads-cft correspondence [gauge/gravity
    duality]; Constructive Gravity; Disformal Gravity;
    emergent gravity [including analog gravity]; entropic gravity;
    parity-violating theories; Projective Relativity;
    Screened Modified Gravity.
Phenomenology > s.a. Antigravity [repulsive component];
  black holes; gravitational phenomenology;
  tests of general relativity.
  @ References: Fischbach & Talmadge 99 [non-Newtonian];
    Capozziello & Faraoni 11 [cosmology and astrophysics];
    Linder JPCS(14)-a1201;
    Dupré a1403
      [tidal acceleration and the structure of local gravity theories];
    Di Virgilio et al proc(17)-a1702 [rev];
    Albarran et al EPJC(18)-a1706 [gravity could become repulsive in the future];
Ezquiaga & Zumalacárregui a1710 [neutron-star merger GW170817].
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