Duality and the Equivalence Principle of Quantum Mechanics
arXiv:hep-th/0009221 · doi:10.1142/S0217751X01005353
Abstract
Following a suggestion by Vafa, we present a quantum-mechanical model for S-duality symmetries observed in the quantum theories of fields, strings and branes. Our formalism may be understood as the topological limit of Berezin's metric quantisation of the upper half-plane H, in that the metric dependence has been removed. Being metric-free, our prescription makes no use of global quantum numbers. Quantum numbers arise only locally, after the choice of a local vacuum to expand around. Our approach may be regarded as a manifestly non perturbative formulation of quantum mechanics, in that we take no classical phase space and no Poisson brackets as a starting point. The reparametrisation invariance of H under SL(2,R) induces a natural SL(2,R) action on the quantum mechanical operators that implements S-duality. We also link our approach with the equivalence principle of quantum mechanics recently formulated by Faraggi and Matone.
14 pages, JHEP style
References in corpus (5)
- Operads and Motives in Deformation Quantization
- Free motion time-of-arrival operator and probability distribution
- N=4 Superconformal Mechanics and the Potential Structure of AdS Spaces
- Generalized Affine Coherent States: A Natural Framework for Quantization of Metric-like Variables
- A New Superconformal Mechanics