@article{AIHPA_1977__27_4_407_0,
author = {Droz-Vincent, Ph.},
title = {Two-body relativistic systems},
journal = {Annales de l'institut Henri Poincar\'e. Section A, Physique Th\'eorique},
pages = {407--424},
year = {1977},
publisher = {Gauthier-Villars},
volume = {27},
number = {4},
mrnumber = {496313},
language = {en},
url = {https://www.numdam.org/item/AIHPA_1977__27_4_407_0/}
}
TY - JOUR AU - Droz-Vincent, Ph. TI - Two-body relativistic systems JO - Annales de l'institut Henri Poincaré. Section A, Physique Théorique PY - 1977 SP - 407 EP - 424 VL - 27 IS - 4 PB - Gauthier-Villars UR - https://www.numdam.org/item/AIHPA_1977__27_4_407_0/ LA - en ID - AIHPA_1977__27_4_407_0 ER -
Droz-Vincent, Ph. Two-body relativistic systems. Annales de l'institut Henri Poincaré. Section A, Physique Théorique, Tome 27 (1977) no. 4, pp. 407-424. https://www.numdam.org/item/AIHPA_1977__27_4_407_0/
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[7] Our argument about it in ref. [4] is wrong, a term being omitted, thus its p. 8 is erroneous. However the theorem thereby stated in covariant form is true in the Poincaré invariant case. The correct proof is due to J. Martin (unpublished).
[8] , Hamiltonian Construction of Predictive Systems. Book in the honor of A. Lichnerowicz, Cahen and Flato, ed. D. Reidel, Dordrecht, 1977. | Zbl | MR
[9] Recall that, even in classical mechanics, the positions are H-J-coordinates only in the free case.
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[13] A different generalization is considered in ref. [8].
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[16] In contrast with our point of view, some authors have introduced quantum relativistic oscillators by wave equations which are not derived from a classical system by the procedure of quantization:
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, , Preprint, 1976.
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