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Ivanov, E.1
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E. Gozzi, M. Reuter, and W. D. Thacker, Phys. Rev. D 40, 3363 (1989); E. Gozzi and M. Reuter, Phys. Lett. B 233, 383 (1989).
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84972500802
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14
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85015125647
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note
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0 on H.
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17
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0000195485
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B. O. Koopman, Proc. Natl. Acad. Sci. U.S.A. 17, 315 (1931); J. von Neumann, Ann. Math. 33, 587 (1932).
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Von Neumann, J.1
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18
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4243218802
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Gozzi, E.1
Regini, M.2
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19
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0034347143
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E. Gozzi and M. Regini, Phys. Rev. D 62, 067702 (2000); E. Gozzi and D. Mauro, J. Math. Phys. 41, 1916 (2000).
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Gozzi, E.1
Mauro, D.2
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20
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85015130478
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note
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The charges which in Table III have been indicated as C and C̄ are those that in Ref. 6 were called K and K̄. We change their names in order not to confuse them with the K operator of the conformal algebra (see Table I).
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-
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21
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85015123484
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note
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ab of Eq. (25).
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22
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85015117311
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note
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The commutators used in Eq. (41) are those of our path integral for classical mechanics derived in Eq. (37).
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-
-
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23
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-
85015129415
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note
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(⋯). Obviously all commutators are between quantities calculated at the same time.
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24
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85015109549
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note
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The conventions (79) and (80) are slightly different than the ones in Ref. 6. Here we also correct some misprints present in that reference.
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-
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25
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85015119915
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note
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0 in Eqs. (A1) and (A9).
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-
-
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26
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85015128983
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note
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i, which in our case of a one-dimensional system is just one variable.
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-
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27
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85015112351
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note
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t functions were via Eqs. (95) and (98).
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28
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85015127786
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J. Kumar, J. High Energy Phys. 9904, 006 (1999); S. Cacciatori, D. Klemm, and D. Zanor, hep-th/9910065.
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, vol.9904
, pp. 6
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Kumar, J.1
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31
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85015117270
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note
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Actually we should take the classical version of (17) and (18) as we are doing classical mechanics.
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32
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85015110890
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note
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ab, to stick to the conventions of Eqs. (84) and (87).
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