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A discrete, unitary, causal theory of quantum gravity
General Relativity and Quantum Cosmology · Submitted 12 Jan 2012
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim This allows a Hilbert space of physical states to be constructed.
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The abstract, sentence by sentence
A discrete model of Lorentzian quantum gravity is proposed. The theory is completely background free, containing no reference to absolute space, time, or simultaneity. The states at one slice of time are networks in which each vertex is labelled with two arrows, which point along an adjacent edge, or to the vertex itself. The dynamics is specified by a set of unitary replacement rules, which causally propagate the local degrees of freedom. The inner product between any two states is given by a sum over histories. Assuming it converges (or can be Abel resummed), this inner product is proven to be hermitian and fully gauge-degenerate under spacetime diffeomorphisms. At least for states with a finite past, the inner product is also positive. This allows a Hilbert space of physical states to be constructed.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | A discrete model of Lorentzian quantum gravity is proposed. | contribution 1.00 | 0.89 | 0.31 | asserted 0.88 |
| s1 | The theory is completely background free, containing no reference to absolute space, time, or simultaneity. | contribution 0.86 | 0.59 | 0.10 | asserted 1.00 |
| s2 | The states at one slice of time are networks in which each vertex is labelled with two arrows, which point along an adjacent edge, or to the vertex itself. | method 0.80 | 0.62 | 0.04 | asserted 1.00 |
| s3 | The dynamics is specified by a set of unitary replacement rules, which causally propagate the local degrees of freedom. | method 0.80 | 0.77 | 0.09 | asserted 1.00 |
| s4 | The inner product between any two states is given by a sum over histories. | method 0.78 | 0.77 | 0.10 | asserted 1.00 |
| s5 | Assuming it converges (or can be Abel resummed), this inner product is proven to be hermitian and fully gauge-degenerate under spacetime diffeomorphisms. | result 0.95 | 0.85 | 0.16 | asserted 0.92 |
| s6 | At least for states with a finite past, the inner product is also positive. | result 0.97 | 0.86 | 0.08 | asserted 0.94 |
| s7 | This allows a Hilbert space of physical states to be constructed. | result 0.59 | 0.82 | 0.25 | asserted 0.89 |
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The paper
Original abstract
A discrete model of Lorentzian quantum gravity is proposed. The theory is completely background free, containing no reference to absolute space, time, or simultaneity. The states at one slice of time are networks in which each vertex is labelled with two arrows, which point along an adjacent edge, or to the vertex itself. The dynamics is specified by a set of unitary replacement rules, which causally propagate the local degrees of freedom. The inner product between any two states is given by a sum over histories. Assuming it converges (or can be Abel resummed), this inner product is proven to be hermitian and fully gauge-degenerate under spacetime diffeomorphisms. At least for states with a finite past, the inner product is also positive. This allows a Hilbert space of physical states to be constructed.
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References
How the literature uses it
2 arXiv papers cite this in 4 sentences
Papers citing it · 3 sentences without a confident label
Cites it as support 1 paper
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Additionally, [ref] checked that these are the correct rules in a discrete (but not holographic) model of spacetime that allows for causal propagation.] In order to obtain consistent results one must allow for three possible temporal relationships between the two Cauchy slices:[This classification ignores degenerate cases, e.g. when $N = 0$ in an entire open region.] * $Σ'$ lies entirely to the future of $Σ$, * $Σ'$ lies entirely to the past of $Σ$, * $Σ'$ straddles $Σ$ so that it lies partly to the future (in some open spatial region $R$ of $Σ$) and partly to the past (in the complementary open region $R$ of $Σ$).
Cauchy Slice Holography: A New AdS/CFT Dictionary · Why we use both Signs for the Lapse · 0.98
What it cites · 29 sentences without a confident label
Cites as support 4 papers
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However, there is no way to embed such a structure in Minkowski space without picking out a frame, because the hyperboloid of unit timelike vectors has infinite volume [ref] .
Discreteness without symmetry breaking: a theorem · Prospects · 0.99
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There is some evidence that quantum gravity should be digital, from the finiteness of black hole entropy in generalized thermodynamics [ref] (based on the idea that the black hole entropy should count the entropy of some set of microscopic degrees of freedom associated with the horizon [ref] .) Also, in loop quantum gravity, area and volume operators have discrete eigenvalues [ref] .
Dynamical Origin of the Entropy of a Black Hole · Motivating Remarks · 1.00
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There is some evidence that quantum gravity should be digital, from the finiteness of black hole entropy in generalized thermodynamics [ref] (based on the idea that the black hole entropy should count the entropy of some set of microscopic degrees of freedom associated with the horizon [ref] .) Also, in loop quantum gravity, area and volume operators have discrete eigenvalues [ref] .
Counting surface states in the loop quantum gravity · Motivating Remarks · 1.00
Cites as background 3 papers
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In the “causal set” approach to quantum gravity [ref] , spacetime is assumed to be nothing but a partially ordered set of events.
The causal set approach to quantum gravity · Motivating Remarks · 0.91
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This is a highly nontrivial problem in loop quantum gravity, whose solution is still unclear [ref] .
Loop quantum gravity: an outside view · Motivating Remarks · 0.80
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See Refs. [ref] for additional attempts to impose a causal structure for spin foam models.
Causality in Spin Foam Models · Motivating Remarks · 0.87
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