Strings on AdS2 and the high-energy limit of noncritical M-theory

被引:3
|
作者
Horava, Petr [1 ]
Keeler, Cynthia A.
机构
[1] Univ Calif Berkeley, Berkeley Ctr Theoret Phys, Berkeley, CA 94720 USA
[2] Univ Calif Berkeley, Dept Phys, Berkeley, CA 94720 USA
[3] Univ Calif Berkeley, Lawrence Berkeley Lab, Theoret Phys Grp, Berkeley, CA 94720 USA
来源
基金
美国国家科学基金会;
关键词
M-theory; gauge-gravity correspondence; Bosonic Strings;
D O I
10.1088/1126-6708/2007/06/031
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
Noncritical M-theory in 2 + 1 dimensions has been defined as a double-scaling limit of a nonrelativistic Fermi liquid on a flat two-dimensional plane. Here we study the noncritical M-theory in the limit of high energies, analogous to the alpha '-> infinity limit of string theory. In the related case of two-dimensional Type 0A strings, it has been argued that the conformal alpha ' -> infinity limit leads to AdS(2) with a propagating fermion whose mass is set by the value of the RR flux. Here we provide evidence that in the high-energy limit, the natural ground state of noncritical M-theory similarly describes the AdS(2) X S-1 spacetime, with a massless propagating fermion. We argue that the spacetime effective theory in this background is captured by a topological higher-spin extension of conformal Chern-Simons gravity in 2 + 1 dimensions, consistently coupled to a massless Dirac field. Intriguingly, the two-dimensional plane populated by the original nonrelativistic fermions is essentially the twistor space associated with the symmetry group of AdS(2) X S-1 spacetime; thus, at least in the high-energy limit, noncritical M-theory can be nonperturbatively described as a "Fermi liquid on twistor space".
引用
收藏
页数:31
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