Dilaton Field / Gravity  

In General > s.a. 2D gravity; 2D quantum gravity; solutions in general relativity.
* Idea: A theory arising in dimensional reduction from higher-dimensions (Kaluza-Klein, large extra dimensions, strings), which includes a U(1) gauge field Aa, and depends on a constant ; The dilaton also arises as the Goldstone boson of spontaneously broken conformal field theories (in flat spacetime).
* Action: If Fab is the curvature of Aa,

S[g, A, ] = (1/16G) dv (R gaba b + exp{}Fab Fab) .

@ General references: Nojiri & Odintsov IJMPA(01) [quantum, D = 2, 4, 5]; Sundrum ht/03 [as scalar analog of general relativity].
@ Dynamics: Burton & Mann CQG(98) [Palatini, N-dimensional]; Cadoni & Mana CQG(01)gq/00 [Hamiltonian with boundary].
@ Inflaton: Cabo & Amezaga ht/99-in [and redshift].
@ Related topics: Álvarez & Gómez PLB(00)ht [soft dilaton theorem]; Cavaglià MPLA(00)ht [Weyl invariance]; > s.a. anomaly, cosmological constant, dark energy, dark matter, tests of newtonian gravity [constraints].

Specific Models and Solutions > s.a. black hole solutions; gauge theory solutions; solutions of general relativity; topological defects.
@ With other matter: Meyer ht/05-in [fermions]; Grumiller & Meyer CQG(06)ht [Dirac fermion, quantum].
@ Black holes: Gibbons & Maeda NPB(88); Garfinkle et al PRD(91); Chan et al NPB(95); Gibbons & Kallosh PRD(95)ht/94; Kiem & Park; Casadio et al PRD(97); Casadio & Harms MPLA(99) [different frames]; Vorontsova & Sharov TMP(05) [d-dimensional Schwarzschild-like].
@ Cosmology: Billyard et al JMP(00)gq; Chen et al PRD(00)ht [Bianchi I]; Cabo & Brandenberger a0806 [stabilized by fermion masses]; > s.a. bianchi models.
@ Quantum cosmology: Catren & Simeone mp/05-in; Ahmed gq/06 [+ pfluid].
@ Related topics: Maeda et al PRL(98)gq [naked singularities].

Axion-Dilaton Gravity > s.a. axion; black hole solutions.
* Idea: A theory arising in the low-energy limit of heterotic string theory, via toroidal compactification to 4D.
* Action: If H = dBA F (which implies dH = –F F),

SADJ = M dv [exp{–2}(R + 4 a a Habc HabcFab Fab) + matter]
SADE = M dv [R – 2 a a exp{–4} Habc Habc – exp{–2} Fab Fab + exp{4}matter(exp{2}g)] .


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