{"arxiv_id":"hep-th/9912152","incoming":{"papers":79,"sentences":124,"groups":[{"kind":"extends","label":"Builds on it","papers":5,"sentences":7,"quotes":[{"arxiv_id":"1909.07391","title":"Dictionary for the type II nongeometric flux compactifications","url":"/paper/1909.07391","section":"Introduction","sentence":"In this regard, the symplectic approach of [ref] for the standard type IIB flux compactification with the $H_3/F_3$ fluxes, has been recently generalized by taking several iterative steps; first via including the non-geometric $Q$-flux in [ref] , and subsequently providing its $S$-dual completion via adding the non-geometric $P$-flux in [ref] .","intent_p":0.9,"contests_p":null},{"arxiv_id":"1508.01197","title":"A symplectic rearrangement of the four dimensional non-geometric scalar potential","url":"/paper/1508.01197","section":"Introduction","sentence":"Now the question arises if it could be possible to take the next step to include generalized (non-geometric) fluxes in symplectic formalism of [ref] .","intent_p":0.84,"contests_p":null},{"arxiv_id":"0804.4006","title":"Nonsupersymmetric Flux Vacua and Perturbed N=2 Systems","url":"/paper/0804.4006","section":"Introduction","sentence":"While this flux is not directly piercing the compact cycles we show that, once appropriately regularized, it does introduce an effective superpotential for the complex structure moduli, which is generalization of the usual Gukov-Vafa-Witten superpotential [ref] to 3-form flux with noncompact support.","intent_p":0.98,"contests_p":null},{"arxiv_id":"1306.2761","title":"Dimensional Oxidation of Non-geometric Fluxes in Type II Orientifolds","url":"/paper/1306.2761","section":"Flux induced superpotential","sentence":"Generalizing the celebrated type IIB computation of Taylor/Vafa [ref] , the superpotential for turning on the R-R fluxes and the H-flux in massive type IIA orientifolds on Calabi-Yau threefolds was derived via dimensional reduction of [ref] in [ref] (see also [ref] ) and reads W=14 ( -i ∫_X H∧Ω^C +∫_X e^iJ_c ∧G ) , where the complexified Kähler modulus is defined as $J_c=J+i B$, and the complex structure moduli are encoded in Ω^c =Re (i e^-ϕ Ω_3) + i C^(3) .","intent_p":0.96,"contests_p":null},{"arxiv_id":"1507.08059","title":"Relating Double Field Theory to the Scalar Potential of N=2 Gauged Supergravity","url":"/paper/1507.08059","section":"Introduction","sentence":"This can be considered as the generalization of the computation first performed in [ref] , where the dimensional reduction of the kinetic terms of the NS-NS and R-R type IIB three-form on a (non-toroidal) CY three-fold gives the no-scale scalar potential described in supergravity language by the tree-level Kähler potential for the complex structure/axio-dilaton moduli and the Gukov-Vafa-Witten (GVW) superpotential [ref] .","intent_p":0.95,"contests_p":null}]},{"kind":"comparison","label":"Compares with it","papers":2,"sentences":2,"quotes":[{"arxiv_id":"1505.00544","title":"On modular completion of generalized flux orbits","url":"/paper/1505.00544","section":"Conclusions and discussions","sentence":"These flux orbits consistently reproduce the results of [ref] .","intent_p":0.89,"contests_p":null},{"arxiv_id":"1702.05435","title":"Effective action from M-theory on twisted connected sum $G_2$-manifolds","url":"/paper/1702.05435","section":"Conclusions","sentence":"[ref] , in which, however, gravity is decoupled.","intent_p":0.9,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":34,"sentences":37,"quotes":[{"arxiv_id":"1605.06299","title":"String Moduli Stabilization at the Conifold","url":"/paper/1605.06299","section":"Introduction","sentence":"In this respect it is important to keep in mind that this analysis was employing the usual effective supergravity action described by the leading order Kähler potential and the Gukov-Vafa-Witten (GVW) superpotential [ref] .","intent_p":0.92,"contests_p":null},{"arxiv_id":"2409.03847","title":"All-orders moduli for type II flux backgrounds","url":"/paper/2409.03847","section":"Introduction","sentence":"Probably the most famous example of stabilisation is that of adding complex three-form flux $G_3$ to type IIB Calabi–Yau O3/O7-plane orientifolds discussed by Giddings–Kachru–Polchinski [ref] , for which the superpotential has the Gukov–Vafa–Witten form [ref] [equation] where $Ω$ is the holomorphic three-form on the Calabi–Yau space.","intent_p":0.97,"contests_p":null},{"arxiv_id":"1704.05686","title":"Partial Breaking in Rigid Limit of $\\mathcal{N}=2$ Gauged Supergravity","url":"/paper/1704.05686","section":"Introduction","sentence":"It has been shown since a long time that the no-go theorem of [ref] , which forbids the partial breaking of extended supersymmetries, can be overcome by turning on appropriate fluxes [ref] , or by using non linear realisations of extended supersymmetry [ref] , or also by taking rigid limits of extended gauged supergravities [ref] ; see also [ref] for the local case.","intent_p":0.91,"contests_p":null},{"arxiv_id":"2308.15529","title":"Taxonomy of scalar potential with U-dual fluxes","url":"/paper/2308.15529","section":"Brief summary of the iterative steps:","sentence":"* Step-0: In the context of standard type IIB flux compactification with the usual NS-NS and RR fluxes, $H_3$ and $F_3$, the four-dimensional scalar potential induced via the so-called Gukov-Vafa-Witten (GVW) flux superpotential [ref] has been compactly derived through the dimensional reduction of the 10D kinetic pieces [ref] .","intent_p":0.86,"contests_p":null},{"arxiv_id":"0707.4270","title":"AdS4 flux vacua in type II superstrings and their domain-wall solutions","url":"/paper/0707.4270","section":"Fluxes in type IIA/B and mirror map","sentence":"Type IIB We will start without geometrical fluxes; then the tree-level 3-form flux superpotential in type IIB on a Calabi–Yau 3-fold $X$ is of the standard form [ref] .","intent_p":0.91,"contests_p":null}]}],"unlabelled_sentences":78},"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/9912152"}}