{"arxiv_id":"hep-th/0602120","incoming":{"papers":31,"sentences":67,"groups":[{"kind":"comparison","label":"Compares with it","papers":1,"sentences":1,"quotes":[{"arxiv_id":"2004.13110","title":"Non-supersymmetric branes","url":"/paper/2004.13110","section":"Intersecting D6-branes","sentence":"These differ from the conventions used by Villadoro and Zwirner (VZ) in [ref] , so that our $Ω$ satisfies $Ω=Ω^VZ$, and our $Ω_Σ$ is $Ω̃_π$ in [ref] .] Ω_Σ= ∫_Σ_3 e^-ϕ Ω ,","intent_p":0.9,"contests_p":null}]},{"kind":"supports_this_paper","label":"Cites it as support","papers":3,"sentences":3,"quotes":[{"arxiv_id":"2004.13110","title":"Non-supersymmetric branes","url":"/paper/2004.13110","section":"Intersecting D6-branes","sentence":"This supports the argument in [ref] .] Another interesting case are anti-D6-branes, which are wrapping supersymmetric cycles with the opposite orientation and therefore also have $Ω_Σ=0$.","intent_p":0.99,"contests_p":null},{"arxiv_id":"0710.2551","title":"On general flux backgrounds with localized sources","url":"/paper/0710.2551","section":"D-branes on flux backgrounds","sentence":"Analogously, in the presence of fluxes the cancellation of gauge anomalies in the effective theory is realized only when both bulk and localized BI are satisfied [ref] .","intent_p":0.98,"contests_p":null},{"arxiv_id":"0809.2610","title":"Neutrino Masses, Baryon Asymmetry, Dark Matter and the Moduli Problem : A Complete Framework","url":"/paper/0809.2610","section":"$D$-term contribution to masses of Moduli","sentence":"This is also supported by arguments given in [ref] .","intent_p":1.0,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":11,"sentences":13,"quotes":[{"arxiv_id":"0802.0202","title":"D-terms on the resolved conifold","url":"/paper/0802.0202","section":"D-terms from non–primitive background flux on D7–branes","sentence":"Soft supersymmetry breaking via D–terms on D7–branes has been considered in [ref] , and was later applied to more realistic type IIB orientifolds [ref] or their F–theory lift [ref] (see also [ref] for a IIA scenario); the most general study for generalised CYs has appeared in [ref] .","intent_p":0.98,"contests_p":null},{"arxiv_id":"1503.07634","title":"A Flux-Scaling Scenario for High-Scale Moduli Stabilization in String Theory","url":"/paper/1503.07634","section":"Introduction","sentence":"Vacua of this potential have been discussed in toroidal backgrounds in [ref] and in more general CY three-folds [ref] .","intent_p":0.93,"contests_p":null},{"arxiv_id":"0706.3049","title":"Beyond Twisted Tori","url":"/paper/0706.3049","section":"Introduction","sentence":"Recently, this type of fluxes has received a renewed interest in string compactifications for several reasons, such as the possibility to construct new gauged supergravities [ref] , stabilize moduli [ref] , improve the understanding of string dualities [ref] and consistency conditions [ref] .","intent_p":0.91,"contests_p":null},{"arxiv_id":"1303.6726","title":"Towards New Classes of Flux Compactifications","url":"/paper/1303.6726","section":"D-terms from non–primitive background flux on D7–branes","sentence":"Soft supersymmetry breaking via D–terms on D7–branes has been considered in [ref] , and was later applied to more realistic type IIB orientifolds [ref] or their F–theory lift [ref] (see also [ref] for a IIA scenario); the most general study for generalised CYs has appeared in [ref] .","intent_p":0.97,"contests_p":null},{"arxiv_id":"0809.0544","title":"Stable de Sitter Vacua in 4 Dimensional Supergravity Originating from 5 Dimensions","url":"/paper/0809.0544","section":"Introduction","sentence":"One can start from a fundamental theory (a superstring or M-theory), study compactifications on various internal manifolds and, with the combined effects of the warped geometries of the internal manifold and tree-level corrections to the $4D$ Kähler potential, obtain a potential in four dimensions that admits de Sitter critical points [ref] .","intent_p":0.89,"contests_p":null}]}],"unlabelled_sentences":50},"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/0602120"}}