Emergence of helicity +/- 2 modes (gravitons) from qubit models

作者：Gu Zheng Cheng; Wen Xiao Gang^*

来源：Nuclear Physics B, 2012, 863(1): 90-129.

DOI：10.1016/j.nuclphysb.2012.05.010

• Strongly correlated quantum systems
• Emergence
• Quantum gravity

We construct two quantum qubit models (or quantum spin models) on three-dimensional lattice in space. L-type model and N-type model. We show that, under a controlled approximation, all the low energy excitations of the L-type model are described by one set of helicity +/- 2 modes with omega alpha k(3) dispersion. We also argue that all the low energy excitations of the N-type model are described by one set of helicity +/- 2 modes with omega alpha k dispersion. In both model, the low energy helicity +/- 2 modes can be described by a symmetric tensor field h(mu nu) in continuum limit, and the gaplessness of the helicity +/- 2 modes is protected by an emergent linearized diffeomorphism gauge symmetry hit h(mu nu) -> h(mu v) + partial derivative(mu) f(nu) + partial derivative(nu) f(mu) at low energies. Thus the linearized quantum gravity emerge from our lattice tnodels. It turns out that the low energy effective Lagrangian density of the L-type model is invariant under the linearized diffeomorphism gauge transformation. Such a property protects the gapless omega alpha k(3) helicity +/- 2 modes. In contrast, the low energy effective Lagrangian of the N-type model changes by a boundary term under the linearized diffeomorphism gauge transformation. Such a property protects the gapless omega alpha k helicity +/- 2 modes. From many-body physics point of view, the ground states of the our two qubit model represent new states of quantum matter, whose low energy excitations are all described by one set of gapless helicity +/- 2 modes.

• 出版日期2012-10-1
• 单位中国科学院理论物理研究所