88:, but with the generalisation of including a certain type of metric discontinuities: the face shared by two adjacent polyhedra has a unique area, but its shape can be different. This is a consequence of the quantum geometry of spin networks: ordinary Regge calculus is "too rigid" to account for all the geometric degrees of freedom described by the semiclassical limit of a spin network.
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The name twisted geometry captures the relation between these additional degrees of freedom and the off-shell presence of torsion in the theory, but also the fact that this classical description can be derived from
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S. Speziale and
Wolfgang M. Wieland (2012). "The twistorial structure of loop-gravity transition amplitudes".
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L. Freidel and S. Speziale (2010). "Twisted geometries: A geometric parametrisation of SU(2) phase space".
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E. R. Livine and J. Tambornino (2012). "Spinor
Representation for Loop Quantum Gravity".
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C. Rovelli and S. Speziale (2010). "On the geometry of loop quantum gravity on a graph".
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E. Bianchi, P. Dona and S. Speziale (2011). "Polyhedra in loop quantum gravity".
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L. Freidel and S. Speziale (2010). "From twistors to twisted geometries".
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