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3
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85037192437
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R.S. Tung, Ph.D. dissertation, National Central University, 1996
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R.S. Tung, Ph.D. dissertation, National Central University, 1996.
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6
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85037251921
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gr-qc/9904008
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R.S. Tung, “Gravitation as a supersymmetric gauge theory,” gr-qc/9904008.
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Tung, R.S.1
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9
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85037229437
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For the body of our work, we consider the source free “vacuum” theory. The issue of coupling to sources is noted later
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For the body of our work, we consider the source free “vacuum” theory. The issue of coupling to sources is noted later.
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10
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85037197339
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J.A. Schouten, Ricci Calculus, 2nd ed. (Springer-Verlag, London, 1954), p. 141
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J.A. Schouten, Ricci Calculus, 2nd ed. (Springer-Verlag, London, 1954), p. 141.
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22
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0033472426
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There are other teleparallel representations of GR, see J.M. Nester and H.-J. Yo, Chin. J. Phys.37, 113 (1999).
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(1999)
Chin. J. Phys.
, vol.37
, pp. 113
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Nester, J.M.1
Yo, H.-J.2
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23
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0001117240
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Also note that there are many teleparallel theories which are not equivalent to GR, e.g., K. Hayashi and T. Shirafuji, Phys. Rev. D 19, 3524 (1979).
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(1979)
Phys. Rev. D
, vol.19
, pp. 3524
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Hayashi, K.1
Shirafuji, T.2
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24
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85037233678
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Concerning the inclusion of sources in the field equations, the proper source coupling is such that a test particle without spin will only feel the Riemannian structure. In GR sources with spin couple to the connection, their standard GR coupling is not equivalent to “minimal coupling” with respect to the teleparallel geometry
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Concerning the inclusion of sources in the field equations, the proper source coupling is such that a test particle without spin will only feel the Riemannian structure. In GR sources with spin couple to the connection, their standard GR coupling is not equivalent to “minimal coupling” with respect to the teleparallel geometry.
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31
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85037189013
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For the equation of motion with sources, the equivalent to the GR source coupling is reproduced by incorporating the metric (via the tetrad) into the source Lagrangian. In some cases that may be easily translated into an equivalent coupling to the spinor field (Formula presented). However, we do not expect to find a general prescription for coupling the QSL spinor field to a source in a way that would be compatible with the spinor’s local Lorentz gauge freedom
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For the equation of motion with sources, the equivalent to the GR source coupling is reproduced by incorporating the metric (via the tetrad) into the source Lagrangian. In some cases that may be easily translated into an equivalent coupling to the spinor field (Formula presented). However, we do not expect to find a general prescription for coupling the QSL spinor field to a source in a way that would be compatible with the spinor’s local Lorentz gauge freedom.
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32
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85037203095
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This Hamiltonian is similar to, but distinct from the one associated with the Witten positive energy proof
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This Hamiltonian is similar to, but distinct from the one associated with the Witten positive energy proof 126.
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36
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85037243531
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Some recent works, For a connection with Ashtekar’s new variables, see
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Some recent works 3031 have noted a connection between the QSL formulation and chiral supergravity.For a connection with Ashtekar’s new variables, see 32.
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