{"arxiv_id":"1512.01547","incoming":{"papers":1,"sentences":1,"groups":[],"unlabelled_sentences":1},"outgoing":{"papers":6,"sentences":9,"groups":[{"kind":"data_used","label":"Uses data or values from","papers":1,"sentences":2,"quotes":[{"arxiv_id":"cond-mat/0306273","title":"The critical behavior of magnetic systems described by Landau-Ginzburg-Wilson field theories","url":"/paper/cond-mat/0306273","section":"Introduction","sentence":"Here $Δ_xy$ is the scaling dimension of $r̃$ at the $3d$ XY universality class, which is very close to $3/2$ [ref] .","intent_p":0.98,"contests_p":null}]},{"kind":"supports_this_paper","label":"Cites as support","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1510.08455","title":"Explicit derivation of duality between a free Dirac cone and quantum electrodynamics in (2+1) dimensions","url":"/paper/1510.08455","section":"Introduction","sentence":"Recently a coupled wire construction of the duality further supports this idea [ref] .","intent_p":0.99,"contests_p":null}]},{"kind":"background","label":"Cites as background","papers":3,"sentences":3,"quotes":[{"arxiv_id":"1306.3286","title":"A symmetry-respecting topologically-ordered surface phase of 3d electron topological insulators","url":"/paper/1306.3286","section":"Introduction","sentence":"It was demonstrated that under strong interaction the boundary of a $3d$ TI can have various topological orders that cannot be realized in a pure $2d$ system [ref] .","intent_p":0.83,"contests_p":null},{"arxiv_id":"1506.01376","title":"Mirror symmetry and the half-filled Landau level","url":"/paper/1506.01376","section":"Introduction","sentence":"Ref. [ref] has applied the mirror symmetry [ref] (duality between supersymmetric field theories) to the half-filled Landau level [ref] , which is a system closely related to the boundary of $3d$ TI [ref] .","intent_p":0.8,"contests_p":null},{"arxiv_id":"0803.2868","title":"Topological superfluids with time reversal symmetry","url":"/paper/0803.2868","section":"Introduction","sentence":"Although it is well-known that the boundary state of a noninteracting $3d$ topological insulator (TI) is described by one or odd number of free $(2+1)d$ Dirac fermions [ref] , curiosity drives theorists to look for all possible boundary states of $3d$ TI under strong interaction.","intent_p":0.99,"contests_p":null}]}],"unlabelled_sentences":3},"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/1512.01547"}}