|  Conformal Gravity | 
In General
  > s.a. 3D gravity; gravity theories;
  covariant quantum gravity; gauge theory of gravity.
  * Idea: A theory of gravity
    that is invariant under conformal (local scale) transformations; There are
    several versions in the literature, a popular one being the higher-derivative
    theory with the Bach equation as the vacuum field equation, and action
    \[ S = \alpha \int{\rm d}^4x\, |g|^{1/2}\,C_{abcd}\,C^{abcd}\;. \]
  * Motivation: Initially, the
    dimensionless coupling constant α, for quantization; Later,
    used to explain flat galactic rotation curves without dark matter; It can
    also give rise to a cosmological acceleration.
  * And general relativity:
    One can obtain Einstein gravity from conformal gravity in 4D by introducing
    a scalar compensator with a vacuum expectation value that spontaneously breaks
    the conformal invariance and generates the Planck mass, or by compactifying
    extra dimensions in a higher-dimensional conformal theory of gravity (without
    the need to introduce the scalar compensator).
  * Solutions, and phenomenology:
    All vacuum solutions of general relativity (e.g., Schwarzschild spacetime) are
    solutions of conformal gravity, but not the other way around, and not with
    matter; Linearized theory gives a 4th-order wave equation, \((\partial_t^{\,2}
    + \nabla^2)^2 \phi = 0\) around Minkowski spacetime.
  * Results: One gets an extra
    attractive effect on matter (from motion in Schwarzschild-like solutions, the
    Newtonian potential is modified to \(V(r) = -b/r + cr\)), but also an additional
    repulsive term for light, affecting light deflection (and the latter does not fit
    observed data); The cosmological \(G_{\rm eff}\) is smaller than the Cavendish one;
    > s.a. dark matter [alternatives].
  @ General references:
    Boulware et al PRL(83) [zero-energy theorem];
    Gorbatenko et al GRG(02)gq/01 [and geometrodynamics];
    Gorbatenko & Pushkin GRG(02) [and causality];
    Gorbatenko GRG(05) [properties];
    Carroll a0705 [and quantum theory];
    Mannheim FP(11)-a1101-conf [the case for];
    Yoon PRD(13)-a1305 [criticism],
    Mannheim PRD(16)-a1506 [response];
    Lovrekovic PoS-a1505 [canonical charges and asymptotic symmetries].
  @ And general relativity: Maldacena a1105;
    Wheeler PRD(14)-a1310;
    Ohanian GRG(16)-a1502 [breaking of conformal symmetry];
    Anastasiou & Olea PRD(16)-a1608 [equivalence with Einstein gravity with Neumann boundary conditions].
  @ Quantum: Wang JPCS(06)gq/05,
    PTRS(06)gq [canonical, new variables and Immirzi parameter];
    Mannheim a0707-proc [no ghosts];
    Jizba et al EPJC(15)-a1410 [and inflationary cosmology];
    Modesto & Rachwal a1605 [spontaneous breaking of Weyl symmetry and non-singular spacetimes];
    Campiglia et al CQG(17)-a1609 [lqg approach, coupled to the Standard Model];
    Veraguth & Wang PRD(17)-a1705 [loop quantization];
    Rachwal Univ(18)-a1808 [scattering amplitudes and quantum effective action].
  @ Barbour's version: Barbour CQG(03)gq/02 [particle motion],
    Anderson et al CQG(03)gq/02 [geometrodynamics].
  > Related topics: see conformal invariance
    in physics; schwarzschild spacetime; unified theories
    [Weyl, conformal gravity].
Solutions and Phenomenology
  > s.a. causality violations [warp drive].
  *  Newtonian limit: It appears that
    in this model gravity is attractive on small scales and repulsive on large scales.
  @ Solutions: Schmidt AdP(84)gq/01,
    AN(85)gq/01 [of Bach equation];
    Le Brun CMP(91);
    Edery PRL(99)gq;
    Dzhunushaliev  & Schmidt JMP(00)gq/99 [vacuum];
    Bhattacharya et al JCAP(10)-a0910 [Mannheim-Kazanas solution];
    Brihaye & Verbin PRD(10)-a0912 [cylindrically-symmetric].
  @ With coupled matter: Brihaye & Verbin PRD(09)-a0907 [and scalar-tensor extension],
    PRD(10)-a0910 [+ gauge theory, spherical symmetry];
    Fabbri AFLB-a1101 [Dirac matter],
    PRD(12)-a1101 [ELKO spinor field].
  @ Astrophysics: O'Brien & Mannheim MNRAS(12)-a1107,
    Mannheim & O'Brien JPCS(13)-a1211 [dwarf galaxy rotation curves];
    Yang et al PLB(13)-a1311 [constraints from SNIa and Hubble parameter data];
    Varieschi GRG(14)-a1401 [Kerr geometry and geodesic motion];
    Bambi et al PRD(17)-a1701 [astrophysical black holes];
    Zhang et al EPJC(18)-a1805 [black holes].
  @ Galactic rotation curves: Campigotto et al CQG(19)-a1712 [failure];
    Li & Modesto a1906 [predicted];
    Hobson & Lasenby a2103 [not predicted].
  @ Cosmology: Mannheim GRG(90),
    ap/96 [age of the universe],
    ap/98,
    ap/98-proc,
    gq/99-proc,
    ApJ(01)ap/99 [cosmic acceleration];
    Varieschi GRG(10)-a0809,
    ISRN-AA(11)-a0812 [kinematical approach];
    Mannheim PRD(12) [perturbations];
    Nesbet Ent(13)-a1208 [dark matter and dark energy, rev];
    Modesto et al a1906 [singularity avoidance];
    > s.a. bianchi I models;
      cosmological-constant problem.
  @ Other phenomenology: Barabash & Shtanov PRD(99)ap [Newtonian limit];
    Navarro & Van Acoleyen JHEP(05)ht [compactification and general relativity];
    Varieschi PRI(12)-a1010 [and the Pioneer anomaly];
    Phillips MNRAS(15)-a1502 [attractive and repulsive gravity];
    Yang PLB(18)-a1710 [gravitational waves].
Variations
  @ Spatially conformally invariant theories:
    Gomes AP(15)-a1310 [canonical description and duality];
    > s.a. Shape Dynamics.
  @ Other variations: Fabbri PLB(12)-a1101 [with torsion];
    Faria AHEP-a1312 [massive conformal gravity];
Dunajski & Tod CMP(14) [self-dual].
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