{ "id": "quant-ph/9507004", "version": "v1", "published": "1995-07-07T16:27:35.000Z", "updated": "1995-07-07T16:27:35.000Z", "title": "Generalized uncertainty relations: Theory, examples, and Lorentz invariance", "authors": [ "Samuel L. Braunstein", "Carlton M. Caves", "G. J. Milburn" ], "comment": "39 pages of text plus one figure; text formatted in LaTeX", "doi": "10.1006/aphy.1996.0040", "categories": [ "quant-ph" ], "abstract": "The quantum-mechanical framework in which observables are associated with Hermitian operators is too narrow to discuss measurements of such important physical quantities as elapsed time or harmonic-oscillator phase. We introduce a broader framework that allows us to derive quantum-mechanical limits on the precision to which a parameter---e.g., elapsed time---may be determined via arbitrary data analysis of arbitrary measurements on $N$ identically prepared quantum systems. The limits are expressed as generalized Mandelstam-Tamm uncertainty relations, which involve the operator that generates displacements of the parameter---e.g., the Hamiltonian operator in the case of elapsed time. This approach avoids entirely the problem of associating a Hermitian operator with the parameter. We illustrate the general formalism, first, with nonrelativistic uncertainty relations for spatial displacement and momentum, harmonic-oscillator phase and number of quanta, and time and energy and, second, with Lorentz-invariant uncertainty relations involving the displacement and Lorentz-rotation parameters of the Poincar\\'e group.", "revisions": [ { "version": "v1", "updated": "1995-07-07T16:27:35.000Z" } ], "analyses": { "keywords": [ "generalized uncertainty relations", "lorentz invariance", "harmonic-oscillator phase", "hermitian operator", "elapsed time" ], "tags": [ "journal article" ], "note": { "typesetting": "LaTeX", "pages": 39, "language": "en", "license": "arXiv", "status": "editable", "inspire": 397113 } } }