Black hole solutions in R2 gravity

被引:63
|
作者
Kehagias, Alex [1 ,2 ,3 ]
Kounnas, Costas [4 ]
Luest, Dieter [5 ,6 ,7 ]
Riotto, Antonio [2 ,3 ]
机构
[1] Natl Tech Univ Athens, Div Phys, Athens 15780, Greece
[2] Univ Geneva, Dept Theoret Phys, CH-1211 Geneva 4, Switzerland
[3] CAP, CH-1211 Geneva 4, Switzerland
[4] Ecole Normale Super, Lab Phys Theor, F-75231 Paris 05, France
[5] Max Planck Inst Phys & Astrophys, Werner Heisenberg Inst, D-80805 Munich, Germany
[6] LMU, Arnold Sommerfeld Ctr Theoret Phys, D-80333 Munich, Germany
[7] CERN, PH TH Div, CH-1211 Geneva 23, Switzerland
来源
基金
瑞士国家科学基金会;
关键词
Black Holes; Classical Theories of Gravity; INFLATIONARY UNIVERSE; SUPERGRAVITY; FLATNESS; ENTROPY; HORIZON; ENERGY; MODELS;
D O I
10.1007/JHEP05(2015)143
中图分类号
O412 [相对论、场论]; O572.2 [粒子物理学];
学科分类号
摘要
We find static spherically symmetric solutions of scale invariant R-2 gravity. The latter has been shown to be equivalent to General Relativity with a positive cosmological constant and a scalar mode. Therefore, one expects that solutions of the R-2 theory will be identical to that of Einstein theory. Indeed, we find that the solutions of R-2 gravity are in one-to-one correspondence with solutions of General Relativity in the case of non-vanishing Ricci scalar. However, scalar-flat R = 0 solutions are global minima of the R-2 action and they cannot in general be mapped to solutions of the Einstein theory. As we will discuss, the R = 0 solutions arise in Einstein gravity as solutions in the tensionless, strong coupling limit M-P -> 0. As a further result, there is no corresponding Birkhoff theorem and the Schwarzschild black hole is by no means unique in this framework. In fact, R-2 gravity has a rich structure of vacuum static spherically symmetric solutions partially uncovered here. We also find charged static spherically symmetric backgrounds coupled to a U(1) field. Finally, we provide the entropy and energy formulas for the R-2 theory and we find that entropy and energy vanish for scalar-flat backgrounds.
引用
收藏
页数:20
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