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Holography for the Lorentz Group Racah Coefficients
General Relativity and Quantum Cosmology · Submitted 21 Dec 2004
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Starting from this construction and carrying out the bulk integrals we obtain a realization of the Racah coefficients that is ``holographic'' in the sense that it only involves boundary objects.
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The abstract, sentence by sentence
A known realization of the Lorentz group Racah coefficients is given by an integral of a product of 6 ``propagators'' over 4 copies of the hyperbolic space. These are ``bulk-to-bulk'' propagators in that they are functions of two points in the hyperbolic space. It is known that the bulk-to-bulk propagator can be constructed out of two bulk-to-boundary ones. We point out that there is another way to obtain the same object. Namely, one can use two bulk-to-boundary and one boundary-to-boundary propagator. Starting from this construction and carrying out the bulk integrals we obtain a realization of the Racah coefficients that is ``holographic'' in the sense that it only involves boundary objects. This holographic realization admits a geometric interpretation in terms of an ``extended'' tetrahedron.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | A known realization of the Lorentz group Racah coefficients is given by an integral of a product of 6 ``propagators'' over 4 copies of the hyperbolic space. | background 1.00 | 0.05 | 0.09 | asserted 1.00 |
| s1 | These are ``bulk-to-bulk'' propagators in that they are functions of two points in the hyperbolic space. | background 1.00 | 0.06 | 0.03 | asserted 1.00 |
| s2 | It is known that the bulk-to-bulk propagator can be constructed out of two bulk-to-boundary ones. | background 1.00 | 0.04 | 0.03 | asserted 1.00 |
| s3 | We point out that there is another way to obtain the same object. | contribution 0.85 | 0.70 | 0.08 | asserted 0.80 |
| s4 | Namely, one can use two bulk-to-boundary and one boundary-to-boundary propagator. | contribution 0.52 | 0.53 | 0.16 | asserted 0.62 |
| s5 | Starting from this construction and carrying out the bulk integrals we obtain a realization of the Racah coefficients that is ``holographic'' in the sense that it only involves boundary objects. | result 0.54 | 0.93 | 0.71 | asserted 1.00 |
| s6 | This holographic realization admits a geometric interpretation in terms of an ``extended'' tetrahedron. | interpretation 0.99 | 0.82 | 0.24 | asserted 0.98 |
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Original abstract
A known realization of the Lorentz group Racah coefficients is given by an integral of a product of 6 ``propagators'' over 4 copies of the hyperbolic space. These are ``bulk-to-bulk'' propagators in that they are functions of two points in the hyperbolic space. It is known that the bulk-to-bulk propagator can be constructed out of two bulk-to-boundary ones. We point out that there is another way to obtain the same object. Namely, one can use two bulk-to-boundary and one boundary-to-boundary propagator. Starting from this construction and carrying out the bulk integrals we obtain a realization of the Racah coefficients that is ``holographic'' in the sense that it only involves boundary objects. This holographic realization admits a geometric interpretation in terms of an ``extended'' tetrahedron.
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