|  Phenomenology of Scalar-Tensor Theories of Gravity | 
In General
  > s.a. fifth force; higher-order
  gravity phenomenology; (post-)newtonian gravity.
  * Idea: These theories in
    general agree with general relativity in the weak-field, slow-motion regime,
    but may differ significantly from it in strong-field situations; So far, the
    best constraints come from binary neutron stars; In the future we expect
    better binary-object constraints, and gravitational-wave ones.
  * Scalar fields: In order to
    be astrophysically and cosmologically relevant they would have to be light.
  * Weak equivalence principle:
    It is violated if there are types of matter that couple to different combinations
    of φ and gab.
  @ General references: Esposito-Farèse AIP(04)gq [test, rev];
    Lindroos et al PRD(16)-a1512 [propagation of scalar waves];
    Alonso et al PRD(17)-a1610 [future cosmological experiments];
    Sakstein & Jain PRL(17)-a1710,
    Baker et al PRL(17)-a1710,
    Langlois et al PRD(18)-a1711 [constraints from GW170817].
  @ Lorentz symmetry violations: Bezerra et al PRD(05)ht/04 [with torsion];
    Brax PLB(12) [environmentally dependent].
  @ Solar system tests: Devi et al PRD(11)-a1104 [Dirac-Born-Infeld action];
    Anderson & Yunes PRD(17)-a1705;
    Faraoni et al EPJC-a1906.
  @ Binary systems: Freire et al MNRAS(12)-a1205 [the pulsar-white dwarf binary PSR J1738+0333];
    Mirshekari & Will PRD(13)-a1301 [compact binaries to 2.5 PN order];
    > s.a. neutron stars.
  @ Quantum theory:
    Shojai et al MPLA(98),
    MPLA(98);
    > s.a. brans-dicke theory; quantum-gravity
      renormalization and asymptotic safety.
  @ Other effects and results: Faraoni & Gunzig A&A(98) [light amplification];
    Burton et al PLA(08)-a0711 [spinning particles];
    Armendáriz-Picón & Penco PRD(12) [equivalence-principle violations];
    Farajollahi et al PRD(11)-a1201;
    > s.a. equivalence principle;
    gravitational-constant variation; lensing.
  > Cosmology:
    see cosmology in modified gravity;
    dark-energy models; quantum
    cosmology models.
  > Gravitational waves: see gravitational
    radiation; gravitational-wave propagation.
Solutions
  > s.a. astrophysics [Buchdahl inequality]; Birkhoff
  Theorem; multipole moments; Q-Stars.
  * Compact objects:
    Scalar-tensor theories can be compatible with Solar System experiments and
    still produce large modifications in the observable properties of neutron
    stars, such as masses and radii (Damour and Esposito-Farèse, 1990s);
    Black holes in these theories have no hair, but could grow "wigs" supported
    by time-dependent boundary conditions or spatial gradients;
    > s.a. neutron stars.
  @ Black holes, hair: Bekenstein PRD(95);
    Cardoso et al PRL(13)-a1308 [and instabilities];
    Sotiriou & Zhang PRL(14);
    Sotiriou & Zhou PRD(14)-a1408.
  @ Black holes, other: Jacobson PRL(99)ap [primordial];
    Stefanov et al MPLA(07)-a0708 [and non-linear electrodynamics];
    Sotiriou & Faraoni PRL(12)-a1109 [stationary];
    Cardoso et al PRD(13)-a1305 [scalarization and superradiant instability];
    Rupert & Woolgar CQG(14)-a1310 [properties of horizons];
    Bronnikov et al IJMPD(16)-a1603-conf.
  @ Numerical models: Gerosa et al CQG(16)-a1602 [simulations of stellar collapse].
  @ Other solutions: Moffat gq/07 [spherically symmetric, non-singular];
    Sobreira et al JMP(09) [Einstein-Maxwell, static cylindrically symmetric];
    Obukhov & Puetzfeld PRD(14)-a1404 [dynamics of extended test bodies, covariant multipolar approach];
    > s.a. gravitating bodies [relativistic stars];
    wormhole solutions.
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