Canonical quantization of a massive particle on
arXiv:hep-th/0303228 · doi:10.1088/1126-6708/2003/05/017
Abstract
The classical theory for a massive free particle moving on the group manifold is analysed in detail. In particular a symplectic structure and two different sets of canonical coordinates are explicitly found, corresponding to the Cartan and Iwasawa decomposition of the group. Canonical quantization is performed in two different ways; by imposing the future-directed constraint before and after quantization. It is found that this leads to different quantum theories. The Hilbert space of either theory decomposes into the sum of certain irreducible representations of ; however, depending on how the constraint is imposed we get different representations. Quantization of the mass occurs, although a continuum exists in the unconstrained theory corresponding to particles that can reverse their direction in time. A quantization in terms of the ``chiral'' variables of the theory is also carried out giving the same results. Comparisons are made between QFT in and the quantum mechanics derived, and it is found that one of the quantum theories is consistent with the Breitenlohner-Freedman bound.
18 pages, revised version published in JHEP, some sections removed one added
References in corpus (8)
- Geometry of the 2+1 Black Hole
- Strings in AdS_3 and the SL(2,R) WZW Model. Part 1: The Spectrum
- The No-ghost Theorem for AdS_3 and the Stringy Exclusion Principle
- Entropies of Scalar Fields on Three Dimensional Black Holes
- Ghost-Free Spectrum of a Quantum String in SL(2,R) Curved Spacetime
- Quantization of a relativistic particle on the SL(2,R) manifold based on Hamiltonian reduction
- Quantisation of a particle moving on a group manifold
- Relativistic quantum mechanics on the SL(2,R) spacetime