{"arxiv_id":"1006.2444","incoming":{"papers":4,"sentences":4,"groups":[{"kind":"background","label":"Cites it as background","papers":3,"sentences":3,"quotes":[{"arxiv_id":"1310.2610","title":"Holographic plasma and anyonic fluids","url":"/paper/1310.2610","section":"Discussion","sentence":"Such backgrounds [ref] , and their normal quantisation perturbations [ref] , are well understoood.","intent_p":0.97,"contests_p":null},{"arxiv_id":"1306.5792","title":"Momentum relaxation in holographic massive gravity","url":"/paper/1306.5792","section":"A preliminary search for spatially modulated instabilities","sentence":"The violation of the near-horizon BF bound is a well-studied topic in holography [ref] and typically leads to a BKT-type transition in the dual field theory.","intent_p":0.95,"contests_p":null},{"arxiv_id":"1412.1489","title":"A strongly coupled anyon material","url":"/paper/1412.1489","section":"Future directions","sentence":"In the original D3-D5 system this corresponds to breaking the chiral symmetry of the fermions in the strongly coupled field theory [ref] .","intent_p":0.9,"contests_p":null}]}],"unlabelled_sentences":1},"outgoing":{"papers":28,"sentences":58,"groups":[{"kind":"contests","label":"Contests","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1002.3159","title":"Holographic Berezinskii-Kosterlitz-Thouless Transitions","url":"/paper/1002.3159","section":"Conclusion","sentence":"In [ref] , it was shown that, for the BKT type of transition to happen, the charge density and magnetic fields are essential.","intent_p":0.5,"contests_p":0.74}]},{"kind":"method_or_tool","label":"Uses the method or tool of","papers":7,"sentences":14,"quotes":[{"arxiv_id":"hep-th/0512125","title":"Holographic Renormalization of Probe D-Branes in AdS/CFT","url":"/paper/hep-th/0512125","section":"Calculation of 1-pt function","sentence":"In this section we shall present the calculation of the 1-pt function for systems that violates the BF bound at IR, mostly following [ref] , [ref] and [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"1002.3159","title":"Holographic Berezinskii-Kosterlitz-Thouless Transitions","url":"/paper/1002.3159","section":"Calculation of 1-pt function","sentence":"In this section we shall present the calculation of the 1-pt function for systems that violates the BF bound at IR, mostly following [ref] , [ref] and [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"hep-th/0002230","title":"Holographic Reconstruction of Spacetime and Renormalization in the AdS/CFT Correspondence","url":"/paper/hep-th/0002230","section":"Calculation of 1-pt function","sentence":"In this section we shall present the calculation of the 1-pt function for systems that violates the BF bound at IR, mostly following [ref] , [ref] and [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"hep-th/0205236","title":"Adding flavor to AdS/CFT","url":"/paper/hep-th/0205236","section":"Dp-Dq system","sentence":"The way we shall proceed to address the Dp-Dq brane system is by considering the Dq branes as probe branes in the background generated by the Dp branes in the quenched limit as prescribed in [ref] .","intent_p":0.98,"contests_p":null},{"arxiv_id":"hep-th/0105132","title":"Open and Closed String Interpretation of SUSY CFT's on Branes with Boundaries","url":"/paper/hep-th/0105132","section":"D3-D5 system with Full action","sentence":"This choice to momentum is chosen so as to have a regular solution to the field $x_3$; this kind of choice is also used in [ref] , [ref] (see the study of this configuration at finite temperature in [ref] ).","intent_p":0.93,"contests_p":null}]},{"kind":"comparison","label":"Compares with","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1006.3066","title":"More Holographic Berezinskii-Kosterlitz-Thouless Transitions","url":"/paper/1006.3066","section":"Acknowledgment","sentence":"Jensen [ref] , which also studies the BKT transition and with which there are some overlaps.","intent_p":0.92,"contests_p":null}]},{"kind":"background","label":"Cites as background","papers":1,"sentences":1,"quotes":[{"arxiv_id":"hep-th/9802042","title":"Supergravity and The Large N Limit of Theories With Sixteen Supercharges","url":"/paper/hep-th/9802042","section":"Dp-Dq system","sentence":"In the large $N$ and large 'tHooft coupling limit, the coincident Dp branes are described as [ref]","intent_p":0.89,"contests_p":null}]}],"unlabelled_sentences":41},"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/1006.2444"}}