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1
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85033962627
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note
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By "standard general relativity" we mean general relativity without any supplementary element like tetrads, second metric, or an arbitrary vector field.
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2
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85033964538
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note
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Called canonical because it can be obtained as canonical one from a suitable Lagrangian (see Ref. 3).
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4
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85033972279
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Duhita Publishers c/o Einstein Foundation International, Nagpur
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J. Garecki, in Proceedings: Einstein Centenary Symposium, Vol. II (Duhita Publishers c/o Einstein Foundation International, Nagpur, 1981).
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(1981)
Proceedings: Einstein Centenary Symposium
, vol.2
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Garecki, J.1
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15
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0009283744
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Canonical energetic and canonical superenergetic quantities for friedman universes
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J. Garecki, "Canonical Energetic and Canonical Superenergetic Quantities for Friedman Universes," paper accepted for publication in Rep. Math. Phys. (Toruń) 43, 377 (1999).
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(1999)
Rep. Math. Phys. (Toruń)
, vol.43
, pp. 377
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Garecki, J.1
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16
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0002509859
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Angular momentum in general relativity
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edited by A. Held Plenum, New York
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J. Winicour, "Angular Momentum in General Relativity" in General Relativity and Gravitation, edited by A. Held (Plenum, New York, 1980).
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(1980)
General Relativity and Gravitation
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Winicour, J.1
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17
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0039147568
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Invariant transformations, conservation laws and energy-momentum
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edited by A. Held Plenum, New York
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J. Goldberg, "Invariant Transformations, Conservation Laws and Energy-Momentum," in General Relativity and Gravitation, edited by A. Held (Plenum, New York, 1980).
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(1980)
General Relativity and Gravitation
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Goldberg, J.1
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19
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0003795518
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Nauka, Moscow, (in Russian) English: edition of Petrov's book: Einstein Spaces Pergamon, New York
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A. Z. Petrov, New Methods In General Relativity (Nauka, Moscow, 1966) (in Russian) [English: edition of Petrov's book: Einstein Spaces (Pergamon, New York, 1969)].
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(1966)
New Methods in General Relativity
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Petrov, A.Z.1
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21
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0003493190
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North-Holland, Amsterdam, We have used the world function σ(P;y) in the formula (1) already
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J. L. Synge, Relativity: the General Theory (North-Holland, Amsterdam, 1960). We have used the world function σ(P;y) in the formula (1) already.
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(1960)
Relativity: the General Theory
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Synge, J.L.1
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26
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85033964773
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note
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i} mean normal coordinates. But they always form components of a geometric object (see, e.g., Ref. 18).
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28
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85033959586
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note
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Calculations of these components are very simple but tedious. The analytic form of the calculated nonzero components is too complicated to be presented here.
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29
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85033962217
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note
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2.
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30
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85033957205
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note
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1). 32 See Ref. 29.
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31
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85033957454
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note
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In special relativity the antisymmetric part of a conserved energy-momentum tensor is proportional to the ordinary divergence of the three-index tensor which describes intrinsic angular momentum density (see, e.g., Refs. 34 and 35). Here we follow this line.
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