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Dirac bracket revisited
Among all possible singular (Lie) brackets in classical dynamics of discrete systems, the matrix of Dirac brackets between phase‐space coordinates is uniquely characterized by having the symplectic (Lagrange) matrix as a generalized inverse. This result is used to prove an explicit representation of...
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Published in: | Journal of mathematical physics 1988-02, Vol.29 (2), p.362-364 |
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cites | cdi_FETCH-LOGICAL-c324t-d600f17718c675e9798189f3add989e7288e6d269161f8fd4e98a6136b940b263 |
container_end_page | 364 |
container_issue | 2 |
container_start_page | 362 |
container_title | Journal of mathematical physics |
container_volume | 29 |
creator | Ruggeri, G. J. |
description | Among all possible singular (Lie) brackets in classical dynamics of discrete systems, the matrix of Dirac brackets between phase‐space coordinates is uniquely characterized by having the symplectic (Lagrange) matrix as a generalized inverse. This result is used to prove an explicit representation of the Dirac bracket in terms of its singular functions. |
doi_str_mv | 10.1063/1.528076 |
format | article |
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source | AIP_美国物理联合会期刊回溯(NSTL购买) |
subjects | Classical and quantum physics: mechanics and fields Exact sciences and technology Physics Quantum mechanics |
title | Dirac bracket revisited |
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