Two-dimensional higher derivative gravity and conformal transformations

Sep 26, 1994
14 pages
Published in:
  • Class.Quant.Grav. 12 (1995) 849-858
e-Print:
Report number:
  • INFN-CA-TH-94-22

Citations per year

199420012008201520221320
Abstract: (arXiv)
We consider the lagrangian L=F(R)L=F(R) in classical (=non-quantized) two-dimensional fourth-order gravity and give new relations to Einstein's theory with a non-minimally coupled scalar field. We distinguish between scale-invariant lagrangians and scale-invariant field equations. LL is scale-invariant for F = c_1 R\sp {k+1} and a divergence for F=c2RF=c_2 R. The field equation is scale-invariant not only for the sum of them, but also for F=RlnRF=R\ln R. We prove this to be the only exception and show in which sense it is the limit of \frac{1}{k} R\sp{k+1} as k0k\rightarrow 0. More generally: Let HH be a divergence and FF a scale-invariant lagrangian, then L=HlnFL= H\ln F has a scale-invariant field equation. Further, we comment on the known generalized Birkhoff theorem and exact solutions including black holes.
  • gravitation: action
  • dimension: 2
  • transformation: conformal
  • Einstein equation: solution
Loading ...