{"arxiv_id":"hep-th/9911147","incoming":{"papers":76,"sentences":84,"groups":[{"kind":"background","label":"Cites it as background","papers":61,"sentences":63,"quotes":[{"arxiv_id":"2607.07295","title":"Massive Graviton Dark Matter from a Gapped Continuum","url":"/paper/2607.07295","section":"Introduction","sentence":"A different theory where the bulk graviton propagator is a gapped continuum appeared in a different class of 5D backgrounds, the so-called linear dilaton (LD) [ref] metric, which is known to be dual to Little String Theories [ref] .","intent_p":0.87,"contests_p":null},{"arxiv_id":"1906.11473","title":"Little Strings, Long Strings, and Fuzzballs","url":"/paper/1906.11473","section":"Fivebrane dynamics","sentence":"The dynamics of coincident fivebranes in string theory is governed by little string theory, a somewhat mysterious non-gravitational, nonlocal theory in six spacetime dimensions [ref] (for reviews, see [ref] ).","intent_p":1.0,"contests_p":null},{"arxiv_id":"2608.16772","title":"Linear Dilaton in Cosmology and Particle Physics","url":"/paper/2608.16772","section":"Introduction","sentence":"Interestingly enough there is another warped geometry for which the holographic dual is known: the linear dilaton (LD) background metric for which the holographic dual is Little String Theory (LST), a six-dimensional theory compactified on a torus [ref] .","intent_p":0.85,"contests_p":null},{"arxiv_id":"2011.01587","title":"The Coulomb and Higgs Branches of $\\mathcal{N}=1$ Theories of Class $\\mathcal{S}_k$","url":"/paper/2011.01587","section":"Deconstruction Limit","sentence":"The $𝒩=(1,1)$ LST arises as the worldvolume theory on a stack of $N$ parallel NS5-branes in type IIB string theory [ref] .","intent_p":0.8,"contests_p":null},{"arxiv_id":"2003.05983","title":"A note on 4d N = 3 from little string theory","url":"/paper/2003.05983","section":"Introduction","sentence":"These theories are known as little string theories (LST) [ref] (for review see [ref] ) and they correspond to 6d theories with maximal supersymmetry, either $𝒩=(1,1)$ or $𝒩=(2,0)$.","intent_p":1.0,"contests_p":null}]}],"unlabelled_sentences":21},"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/9911147"}}