Phenomenology of Higher-Order Gravity Theories  

In General > s.a. cosmology in higher-order theories.
* Stability: Certain f(R) theories can stabilize solutions which are unstable in general relativity, such as the Einstein static universe.
@ Reviews: Capozziello & Francaviglia GRG(08); Sotiriou a0810-in.
@ Stability: Schmidt PRD(94); Ezawa et al CQG(99) [higher-dimensional, semiclassical]; Dolgov & Kawasaki ap/03 [R–1 theories]; De Felice et al JCAP(06)ap [superluminal mode propagation]; Faraoni PRD(06)ap, Sotiriou PLB(07)gq/06, Sawicki & Hu PRD(07)ap [f(R) theories]; Sokolowski CQG(07)gq [interpretation and viability]; Böhmer et al PRD(07)-a0706 [Einstein static universe]; Lee a0710; Bertolami & Carvalho Sequeira PRD(09) [and energy conditions]; > s.a. types of theories [Hamiltonian perturbation theory].
@ R–1 theories: Flanagan PRL(04)ap/03, Vollick CQG(04)gq/03, Kremer & Alves PRD(04)gq [Palatini form]; Soussa & Woodard GRG(04)ap/03 [force of gravity]; Vollick PRD(05)gq/04 [with Dirac field]; Shao et al PLB(06)gq/05 [as correction term].
@ Other theories: Clifton & Barrow PRD(05)gq [R1+a Lagrangian]; Navarro & Van Acoleyen JCAP(06)ap [ln f(R), dark energy and MOND]; Olmo a0910-in [general, esp 1/R and f(R) = R + R2/RP theories].
@ Non-local theories: Koivisto PRD(08)-a0807 [newtonian limit]; > s.a. theories of gravitation.

Solutions > s.a. Birkhoff's Theorem; black-hole solutions; gödel solution; schwarzschild spacetime; types of spacetimes [Einstein static universe]; wormhole solutions.
* In general: All solutions of the ordinary Einstein equation still extremize S, and there are other solutions; However, if S does not include the usual R term, the ordinary solutions do not couple to positive-definite matter sources.
* Features: In some theories, torsion and its conjugate momentum play an important role.
* Results: Birkhoff's theorem in general is not valid, but it is in some cases; There is massive radiation (2 Yukawa potentials, 8 degrees of freedom, the usual spin-2 graviton, a massive one – negative energy – and one scalar field); It is claimed that in theories with purely quadratic terms in the action, the energy is identically zero, but this seems strange (RDS).
@ Gravitational waves: Campanelli & Loustó PRD(96)gq/95 [shock waves]; de Rey et al CQG(03)gq, CQG(03)gq, CQG(04)gq/03; Ananda et al PRD(08)-a0708 [4th-order gravity in FRW models]; Corda a0710-in [R–1 theory]; Capozziello et al PLB(08)-a0812 [massive, and LISA]; > s.a. gravitational waves and background.
@ Types of solutions: Campanelli et al PRD(94)gq [perturbative method]; Barraco & Hamity GRG(99) [asymptotically flat, and general relativity solutions]; Clifton & Barrow PRD(05)gq [Gödel, Einstein and de Sitter], CQG(06) [Kasner-type], CQG(06)gq [cosmological, 4th-order theories]; Goswami et al PRD(08)-a0804 [Einstein universes, 4th-order theories]; Azadi et al PLB(08) [static cylindrically symmetric]; > s.a. spherical symmetry.

Newtonian Limit
* Remark: Its existence cannot work as a selection rule among metric f(R) theories, because it is implied by stability.
@ General references: Quandt & Schmidt AN(91)gq/01; Domínguez & Barraco PRD(04)gq [Palatini]; Capozziello gq/04-in [rev]; Capozziello & Troisi PRD(05)ap [4th-order, PPN limit]; Sotiriou GRG(06)gq/05; Bertolami et al PRD(07)-a0704 [extra force]; Capozziello et al PRD(07)-a0708; Corda IJTP(08) [extra repulsive force]; Stabile a0809-PhD; Sokolowski APPB(08)-a0810 [and stability]; Capozziello et al MPLA(09)-a0901 [presence of Yukawa correction]; Capozziello & Stabile a0903 [quadratic Lagrangians].
@ Newtonian limit, R–1: Dick GRG(04)gq/03; Rajaraman ap/03; Navarro & Van Acoleyen PLB(05)gq [and acceleration]; Cembranos PRD(06)gq/05 [as lim at intermediate energy]; Navarro & Van Acoleyen JCAP(06)gq/05 [large distance].
@ Post-Newtonian framework: Allemandi et al GRG(05); Capozziello et al MPLA(06)gq [and experimental constraints]; De Laurentis et al a0911-AdP [and cosmological gravitational waves].

Other Phenomenology > s.a. black-hole formation and laws; phenomenology of gravity; tests of general relativity.
@ Galactic dynamics: Capozziello et al PLA(04), ap/04-in, Frigerio & Salucci MNRAS(07)ap [rotation curves]; Borowiec et al ap/06-in [dark matter and dark energy].
@ Solar system constraints: Olmo PRL(05)gq, PRD(05)gq + gq, Jin et al gq/06 [f(R)]; Faraoni PRD(06)gq; Ruggiero & Iorio JCAP(07)gq/06 [planetary orbits]; Chiba et al PRD(07)ap/06; Zakharov et al PRD(06); Faulkner et al PRD(07)ap/06, Saffari & Rahvar PRD(08)-a0708 [and cosmology]; Hu & Sawicki PRD(07)-a0705 [models that evade solar system tests]; Allemandi & Ruggiero GRG(07); Bertolami & Páramos PRD(08)-a0709; Iorio & Ruggiero SRE(08)-a0711; Capozziello & Tsujikawa PRD(08)-a0712; De Felice & Tsujikawa a0907; Bisabr a0907.
@ Solar system constraints, R–1: Erickcek et al PRD(06)ap [ruled out by solar system tests]; Exirifard a0810 [not ruled out by solar system tests].
@ Star interiors, f(R) gravity: Kainulainen et al PRD(07)-gq/06; Bustelo & Barraco CQG(07)gq/06; Henttunen et al PRD(08)-a0705.
@ Singularities: Holdom PRD(02) [and horizons]; > s.a. types of singularities [isotropic].
@ Related topics: Accioly et al NCB(00), Accioly & Blas PRD(01)gq [light deflection, quadratic]; Magnano & Sokolowski AP(03)gq/02 [massive spin-2 field generated]; Núñez & Solganik PLB(05)ht/04 [IR modifications not viable]; Gabadadze & Iglesias PLB(06) [precession]; Capozziello et al MPLA(07) [gravitational wave background]; Iorio & Ruggiero IJMPA(07) [double pulsar]; Li et al CQG(09)-a0801 [indistinguishable macroscopic behavior]; > s.a. Chameleon Field; energy [virial theorem]; energy conditions; equivalence principle; gravitational radiation; thermodynamics.


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