{"arxiv_id":"1001.1189","incoming":{"papers":0,"sentences":0,"groups":[],"unlabelled_sentences":0},"outgoing":{"papers":13,"sentences":21,"groups":[{"kind":"contests","label":"Contests","papers":2,"sentences":2,"quotes":[{"arxiv_id":"hep-ph/9811291","title":"Quantum Gravity and Extra Dimensions at High-Energy Colliders","url":"/paper/hep-ph/9811291","section":"Introduction","sentence":"However, as we will see below, the cross section of such processes in past works (for example in Ref. [ref] ) does not satisfy the approximate expression in eq.([ref]).","intent_p":0.82,"contests_p":0.83},{"arxiv_id":"hep-ph/9811350","title":"On Kaluza-Klein States from Large Extra Dimensions","url":"/paper/hep-ph/9811350","section":"Introduction","sentence":"However, as we will see below, the cross section of such processes in past works (for example in Ref. [ref] ) does not satisfy the approximate expression in eq.([ref]).","intent_p":0.82,"contests_p":0.83}]},{"kind":"comparison","label":"Compares with","papers":1,"sentences":1,"quotes":[{"arxiv_id":"hep-ph/9811350","title":"On Kaluza-Klein States from Large Extra Dimensions","url":"/paper/hep-ph/9811350","section":"Two body scattering via KK graviton","sentence":"The cross section in eq.([ref]) reproduces the result that we get using the $i ϵ$ method or the principal value integration of the propagators to regularize the on-shell pole divergence of KK scalars ( for more details, see Ref. [ref] )[ The leading terms in the two methods correspond the result assuming $$ and $Γ(m)$ in the denominator in eq.([ref]) to be zero.].","intent_p":0.86,"contests_p":null}]},{"kind":"background","label":"Cites as background","papers":9,"sentences":9,"quotes":[{"arxiv_id":"hep-ph/9811356","title":"Indirect Collider Signals for Extra Dimensions","url":"/paper/hep-ph/9811356","section":"Introduction","sentence":"In case of a hadron collider, dominant channels are the real KK graviton emission process $pp →jet + (missing)$ [ref] , and the virtual KK graviton exchange process $pp →ll̅, γγ$ [ref] .","intent_p":0.95,"contests_p":null},{"arxiv_id":"hep-ph/9811337","title":"Collider Signatures of New Large Space Dimensions","url":"/paper/hep-ph/9811337","section":"Introduction","sentence":"In case of a hadron collider, dominant channels are the real KK graviton emission process $pp →jet + (missing)$ [ref] , and the virtual KK graviton exchange process $pp →ll̅, γγ$ [ref] .","intent_p":0.95,"contests_p":null},{"arxiv_id":"hep-ph/9811350","title":"On Kaluza-Klein States from Large Extra Dimensions","url":"/paper/hep-ph/9811350","section":"Virtual Kaluza-Klein graviton exchanges and a toy model","sentence":"For more detail, see Ref. [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"hep-ph/9811291","title":"Quantum Gravity and Extra Dimensions at High-Energy Colliders","url":"/paper/hep-ph/9811291","section":"Virtual Kaluza-Klein graviton exchanges and a toy model","sentence":"For more detail, see Ref. [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"hep-ph/9803315","title":"The Hierarchy Problem and New Dimensions at a Millimeter","url":"/paper/hep-ph/9803315","section":"Introduction","sentence":"The simplest and explicit model with this scenario is the one by Arkani-hamed, Dimopoulos, and Dvali (ADD) [ref] .","intent_p":1.0,"contests_p":null}]}],"unlabelled_sentences":9},"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/1001.1189"}}