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We consider the issue of attaining a consistent Hamiltonian formulation, after a 3+1 splitting, of a well defined action principle for asymptotically flat gravity.
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A. Ashtekar, · 1991
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A. Ashtekar, L. Bombelli, and O. Reula, · 1991
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J. D. Romano, · 1993
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Quasilocal energy and conserved charges derived from the gravitational action
J. D. Brown and J. W. York, · 1993
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Generalized boundary conditions for general relativity for the asymptotically flat case in terms of Ashtekar’s variables
T. Thiemann, · 1995
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Surface terms, asymptotics and thermodynamics of the Holst action
A. Corichi and E. Wilson-Ewing, · 2010
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On asymptotic flatness and Lorentz charges
G. Compère, F. Dehouck, and A. Virmani, · 2011
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Canonical gravity and applications
M. Bojowald, · 2011
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Relaxing the parity conditions of asymptotically flat gravity
G. Compere and F. Dehouck, · 2011
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Boundary terms and the 3 + 1 decomposition of the Holst action
A. Corichi and J. D. Reyes, · 2012
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Supertranslations and Holographic Stress Tensor
A. Virmani, · 2012
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W. Wieland, · 2012
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Imaginary action, spinfoam asymptotics and the ‘transplanckian’ regime of loop quantum gravity
N. Bodendorfer and Y. Neiman, · 2013
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Note on the phase space of asymptotically flat gravity in Ashtekar-Barbero variables
M. Campiglia, · 2014
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First order gravity: Actions, topological terms and boundaries
A. Corichi, I. Rubalcava-García, and T. Vukasinac, · 2014
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Energy in first order 2+1 gravity
A. Corichi and I. Rubalcava-Garcia, · 2015
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