{"arxiv_id":"hep-th/0002073","incoming":{"papers":23,"sentences":41,"groups":[{"kind":"comparison","label":"Compares with it","papers":4,"sentences":6,"quotes":[{"arxiv_id":"2507.02339","title":"Supersymmetry-breaking compactifications on Riemann-flat manifolds","url":"/paper/2507.02339","section":"1-dimensional orbifolds","sentence":"Inserting all this information in ([ref]) gives [equation] which matches the value computed by [ref] , upon setting $L = 2 L̃$, where $L̃$ is the length of the interval.","intent_p":0.99,"contests_p":null},{"arxiv_id":"2507.02037","title":"An M-theory dS maximum from Casimir energies on Riemann-flat manifolds","url":"/paper/2507.02037","section":"Explict formula for RFM Casimir energy & “Casimir branes”","sentence":"We will use eq:VC-invariant-subspace to compute the Casimir energy for M-theory on the interval $S^1/_2$ and compare the result with equations (2.12) and (2.13) of [ref] [Equation (2.13) in [ref] is written in terms of the Jacobi theta function $θ_4(0,iτ)$ and only argued to be convergent and positive.","intent_p":1.0,"contests_p":null},{"arxiv_id":"0808.3186","title":"Tunneling with negative tension","url":"/paper/0808.3186","section":"Relation to Witten's “bubble of nothing\"","sentence":"The solution of [ref] involves a $Z_2$ projection, much like the solutions we describe in Sections [ref] and [ref].","intent_p":0.85,"contests_p":null},{"arxiv_id":"2410.07322","title":"End of the World Boundaries for Chiral Quantum Gravity Theories","url":"/paper/2410.07322","section":"Generalization","sentence":"This resembles the behaviour in the bubble of nothing in [ref] , when regarded from the 10d perspective (it is also reminiscent of the folding trick used to define boundary states in 2d theories).","intent_p":1.0,"contests_p":null}]},{"kind":"supports_this_paper","label":"Cites it as support","papers":1,"sentences":1,"quotes":[{"arxiv_id":"2603.25786","title":"Ho\\v{r}ava-Witten theory on ${\\mathbf{S}}^1\\vee{\\mathbf{S}}^1$ as type 0 orientifold","url":"/paper/2603.25786","section":"The Hořava-Witten and Fabinger-Hořava configurations","sentence":"This is also supported by the fact that the tachyons in the bifundamental, which stretch from one boundary to the other, are generically massive for large interval size, but become tachyonic when the interval size becomes very small, signaling the instability against brane-antibrane annihilation; this dovetails the discussion of the instability of the compactification of M-theory on the interval with oppositely oriented boundaries [ref] .","intent_p":0.97,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":9,"sentences":9,"quotes":[{"arxiv_id":"2603.12319","title":"Quantum Signatures of Cosmic Topology: How Casimir Backreaction Transmits Isotropy Violation","url":"/paper/2603.12319","section":"Introduction","sentence":"Although this effect is well understood [ref] and has been explored in a variety of settings—including semiclassical bouncing cosmologies [ref] and higher-dimensional theories, where Casimir energies influence moduli or brane dynamics [ref] —its role as a direct imprint of non-trivial spatial topology in the early Universe has remained unexplored.","intent_p":0.89,"contests_p":null},{"arxiv_id":"0710.1628","title":"A stable vacuum of the tachyonic E8 string","url":"/paper/0710.1628","section":"Review of the unstable $E_8$ string in 10 dimensions","sentence":"The string [ref] , like all perturbative heterotic string theories, is described in (super)conformal gauge as a (0,1) superconformal field theory (SCFT).","intent_p":0.99,"contests_p":null},{"arxiv_id":"2410.21372","title":"Morse-Bott inequalities, Topology Change and Cobordisms to Nothing","url":"/paper/2410.21372","section":"Bubbles of Nothing","sentence":"While much effort has been done in the past years in finding explicit BoN constructions [ref] (see also [ref] for related problems and techniques), most of the solutions feature relatively simple topologies along the bordism direction.","intent_p":0.93,"contests_p":null},{"arxiv_id":"2105.10507","title":"de Sitter Decays to Infinity","url":"/paper/2105.10507","section":"Introduction","sentence":"A number of studies have explored relatives of Witten's bubble from a top-down perspective, including in string compactifications [ref] , in higher-dimensional models [ref] , and in flux compactifications with stabilized moduli [ref] .","intent_p":0.96,"contests_p":null},{"arxiv_id":"2105.08068","title":"Bubble of nothing decays of unstable theories","url":"/paper/2105.08068","section":"I. Introduction","sentence":"Most prior work has focused on the existence of bubbles of nothing from the top-down in string compactifications [ref] , and on the role of supersymmetry in suppressing decay rates [ref] .","intent_p":0.93,"contests_p":null}]}],"unlabelled_sentences":25},"outgoing":{"papers":0,"sentences":0,"groups":[],"unlabelled_sentences":0},"claims":[],"thresholds":{"intent_p":0.8,"supports_p":0.95,"contests_p":0.7},"method":"Citing sentences come from each paper's LaTeX source; every \\cite marks the sentence and the works it cites. Pith's classifier typed each sentence. A label is shown at intent probability 0.8 or more (0.95 for support), a contest at 0.7 or more. Measured accuracy against two blind model families is at https://pith.science/accuracy. The quoted sentences are the citing authors' own.","held_up":null,"_links":{"html":"https://pith.science/paper/hep-th/0002073"}}