{"arxiv_id":"2103.12724","incoming":{"papers":23,"sentences":29,"groups":[{"kind":"supports_this_paper","label":"Cites it as support","papers":1,"sentences":1,"quotes":[{"arxiv_id":"2212.10516","title":"Constraints on Lepton Universality Violation from Rare $B$ Decays","url":"/paper/2212.10516","section":"Introduction","sentence":"Combining angular distributions with LUV data strengthened the case for New Physics (NP), since a single NP contribution could reproduce the whole set of data [ref] .","intent_p":0.97,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":8,"sentences":10,"quotes":[{"arxiv_id":"2209.05890","title":"Phenomenology of Scalar Leptoquarks at the LHC in Explaining the Radiative Neutrino Mass, Muon $g-2$ and Lepton Flavour Violating Observables","url":"/paper/2209.05890","section":"Introduction","sentence":"The phenomenology of leptoquark models has been studied in literature [ref] , specially in the context of the Large Hadron Collider (LHC) experiment.","intent_p":0.94,"contests_p":null},{"arxiv_id":"2112.05127","title":"Probing B-Anomalies via Dimuon Tails at a Future Collider","url":"/paper/2112.05127","section":"Introduction","sentence":"The sensitivity of the LHC and future colliders to tree-level mediators that can underpin the rare $B$-decay anomalies has been studied for the $Z'$ case in [ref] and for leptoquarks in [ref] (see also [ref] ); for the collider signatures of other models of the $B$-physics anomalies see [ref] and references therein.","intent_p":0.93,"contests_p":null},{"arxiv_id":"2103.16558","title":"Reading the footprints of the B-meson flavor anomalies","url":"/paper/2103.16558","section":"Note Added","sentence":"While this project was under completion, a few papers containing updated EFT analysis of the $$ anomalies [ref] and of the simplified $U_1$ model [ref] appeared.","intent_p":0.97,"contests_p":null},{"arxiv_id":"2301.04119","title":"Constraining flavoured leptoquarks with LHC and LFV","url":"/paper/2301.04119","section":"Introduction","sentence":"We do not consider in detail the flavour patterns where the leptoquark couples only to one letpon flavour, as that is presented in [ref] .","intent_p":0.81,"contests_p":null},{"arxiv_id":"2106.05192","title":"Lepton flavour violation in rare $\\Lambda_b$ decays","url":"/paper/2106.05192","section":"Introduction","sentence":"The NP explanations for $B$ anomalies span a broad class of new heavy particles, from vectors to scalars states [ref] .","intent_p":0.86,"contests_p":null}]}],"unlabelled_sentences":18},"outgoing":{"papers":71,"sentences":132,"groups":[{"kind":"extends","label":"Builds on","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1801.09399","title":"Flavorful leptoquarks at hadron colliders","url":"/paper/1801.09399","section":"Introduction","sentence":"In this paper we focus on the collider signatures of spin-1 (vector) leptoquarks, as a sequel to [ref] on the scalar leptoquark $S_3$.","intent_p":0.99,"contests_p":null}]},{"kind":"method_or_tool","label":"Uses the method or tool of","papers":10,"sentences":12,"quotes":[{"arxiv_id":"1405.0301","title":"The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations","url":"/paper/1405.0301","section":"Single and pair production cross sections","sentence":"For the evaluation of the cross sections and the corresponding uncertainty bands we used [ref] with the [ref] output of the leptoquark models that we implemented using [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"1108.2040","title":"UFO - The Universal FeynRules Output","url":"/paper/1108.2040","section":"Single and pair production cross sections","sentence":"For the evaluation of the cross sections and the corresponding uncertainty bands we used [ref] with the [ref] output of the leptoquark models that we implemented using [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"1310.1921","title":"FeynRules 2.0 - A complete toolbox for tree-level phenomenology","url":"/paper/1310.1921","section":"Single and pair production cross sections","sentence":"For the evaluation of the cross sections and the corresponding uncertainty bands we used [ref] with the [ref] output of the leptoquark models that we implemented using [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"1502.01701","title":"Future tests of Higgs compositeness: direct vs indirect","url":"/paper/1502.01701","section":"Sensitivity projections for future colliders","sentence":"The method assumes that the exclusion limits are determined by the numbers of background events and involves the appropriate re-scaling of the background processes with the corresponding parton luminosity functions, see [ref] for more details.","intent_p":0.99,"contests_p":null},{"arxiv_id":"1710.06363","title":"The Case for Future Hadron Colliders From $B \\to K^{(*)} \\mu^+ \\mu^-$ Decays","url":"/paper/1710.06363","section":"Sensitivity projections for future colliders","sentence":"The method assumes that the exclusion limits are determined by the numbers of background events and involves the appropriate re-scaling of the background processes with the corresponding parton luminosity functions, see [ref] for more details.","intent_p":0.99,"contests_p":null}]},{"kind":"data_used","label":"Uses data or values from","papers":10,"sentences":17,"quotes":[{"arxiv_id":"2006.05872","title":"Search for pairs of scalar leptoquarks decaying into quarks and electrons or muons in $\\sqrt{s}=13$ TeV pp collisions with the ATLAS detector","url":"/paper/2006.05872","section":"Current mass bounds","sentence":"We evaluate the current mass limits for the $V_1$ leptoquark using the limits on the cross sections found in the ATLAS Collaboration search [ref] for the pair production of scalar leptoquarks.","intent_p":0.96,"contests_p":null},{"arxiv_id":"1509.03744","title":"Search for pair production of first and second generation leptoquarks in proton-proton collisions at sqrt(s) = 8 TeV","url":"/paper/1509.03744","section":"Sensitivity projections for future colliders","sentence":"For the extrapolations of the limits on cross sections for pair production we use the search performed by the ATLAS Collaboration in Ref. [ref] at 13TeV with $ℒ=139$, see also Refs. [ref] for earlier searches.","intent_p":0.95,"contests_p":null},{"arxiv_id":"1808.05082","title":"Search for pair production of second-generation leptoquarks at $\\sqrt{s} =$ 13 TeV","url":"/paper/1808.05082","section":"Sensitivity projections for future colliders","sentence":"For the extrapolations of the limits on cross sections for pair production we use the search performed by the ATLAS Collaboration in Ref. [ref] at 13TeV with $ℒ=139$, see also Refs. [ref] for earlier searches.","intent_p":0.95,"contests_p":null},{"arxiv_id":"2103.11769","title":null,"url":"/paper/2103.11769","section":"Introduction","sentence":"Specifically, $R_K$ and $R_K^*$ constrain the leptoquark's coupling to strange quarks and leptons $ℓ$, $λ_sℓ$, and to $b$-quarks and leptons, $λ_bℓ$, divided by the square of the leptoquark mass $M_V$ as [equation] where we included $R_K$ [ref] combined with $R_K^∗$ [ref] in $q^2$-bin $(1.1, 6) GeV^2$, see Refs. [ref] for details.","intent_p":0.99,"contests_p":null},{"arxiv_id":"1411.4773","title":"Diagnosing lepton-nonuniversality in $b \\to s \\ell \\ell$","url":"/paper/1411.4773","section":"Introduction","sentence":"Specifically, $R_K$ and $R_K^*$ constrain the leptoquark's coupling to strange quarks and leptons $ℓ$, $λ_sℓ$, and to $b$-quarks and leptons, $λ_bℓ$, divided by the square of the leptoquark mass $M_V$ as [equation] where we included $R_K$ [ref] combined with $R_K^∗$ [ref] in $q^2$-bin $(1.1, 6) GeV^2$, see Refs. [ref] for details.","intent_p":0.99,"contests_p":null}]},{"kind":"comparison","label":"Compares with","papers":4,"sentences":4,"quotes":[{"arxiv_id":"1710.06363","title":"The Case for Future Hadron Colliders From $B \\to K^{(*)} \\mu^+ \\mu^-$ Decays","url":"/paper/1710.06363","section":"Sensitivity projections for future colliders","sentence":"We find good agreement with the similar extrapolations for the case of single-production in Ref. [ref] .[Up to date analysis of the future sensitivity for the pair production of scalar leptoquarks were recently presented in Ref. [ref] .]","intent_p":1.0,"contests_p":null},{"arxiv_id":"1911.04455","title":"Sensitivity of Future Hadron Colliders to Leptoquark Pair Production in the Di-Muon Di-Jets Channel","url":"/paper/1911.04455","section":"Sensitivity projections for future colliders","sentence":"We find good agreement with the similar extrapolations for the case of single-production in Ref. [ref] .[Up to date analysis of the future sensitivity for the pair production of scalar leptoquarks were recently presented in Ref. [ref] .]","intent_p":1.0,"contests_p":null},{"arxiv_id":"1801.09399","title":"Flavorful leptoquarks at hadron colliders","url":"/paper/1801.09399","section":"Conclusions","sentence":"We find similar cross sections for $V_1$ and the scalar leptoquark $S_3$ in pair production while in single production the scalar ones are a few times lower [ref] .","intent_p":0.98,"contests_p":null},{"arxiv_id":"1801.07641","title":"Leptoquark toolbox for precision collider studies","url":"/paper/1801.07641","section":"Single and pair production cross sections","sentence":"We checked the consistency of our implementations with the corresponding implementations from Ref. [ref] .","intent_p":0.98,"contests_p":null}]},{"kind":"supports_this_paper","label":"Cites as support","papers":2,"sentences":2,"quotes":[{"arxiv_id":"1503.01084","title":"Clues for flavor from rare lepton and quark decays","url":"/paper/1503.01084","section":"Conclusions","sentence":"The reason why this simplified framework is sensible is two-fold: There is presently no necessity to consider couplings to electrons, and flavor symmetries explaining neutrino masses and mixing result in leptoquark couplings to a single lepton species [ref] .","intent_p":0.99,"contests_p":null},{"arxiv_id":"1812.01603","title":"Left-Right SU(4) Vector Leptoquark Model for Flavor Anomalies","url":"/paper/1812.01603","section":"Introduction","sentence":"However, choosing muons over electrons as the main contributors to ([ref]) is consistent with the global $b →s$ fits[It is possible that both muon- and electron channels are affected by contributions of opposite sign [ref] .], which also suggest NP in $b →s μμ$ angular distributions.","intent_p":0.98,"contests_p":null}]},{"kind":"background","label":"Cites as background","papers":25,"sentences":27,"quotes":[{"arxiv_id":"1206.2970","title":"Model independent constraints on leptoquarks from b -> s l+ l- processes","url":"/paper/1206.2970","section":"The vector leptoquarks V1 and V3","sentence":"For a selection of references studying the $V_1$ leptoquark in the context of the $b→s ℓℓ$ transitions we refer the reader to Refs. [ref] .","intent_p":0.96,"contests_p":null},{"arxiv_id":"1512.01560","title":"Anomalies in $B$-decays and $U(2)$ flavour symmetry","url":"/paper/1512.01560","section":"The vector leptoquarks V1 and V3","sentence":"For a selection of references studying the $V_1$ leptoquark in the context of the $b→s ℓℓ$ transitions we refer the reader to Refs. [ref] .","intent_p":0.96,"contests_p":null},{"arxiv_id":"1609.08895","title":"Leptoquark Flavor Patterns & B Decay Anomalies","url":"/paper/1609.08895","section":"The vector leptoquarks V1 and V3","sentence":"For a selection of references studying the $V_1$ leptoquark in the context of the $b→s ℓℓ$ transitions we refer the reader to Refs. [ref] .","intent_p":0.96,"contests_p":null},{"arxiv_id":"1611.04930","title":"B-decay Anomalies in a Composite Leptoquark Model","url":"/paper/1611.04930","section":"The vector leptoquarks V1 and V3","sentence":"For a selection of references studying the $V_1$ leptoquark in the context of the $b→s ℓℓ$ transitions we refer the reader to Refs. [ref] .","intent_p":0.96,"contests_p":null},{"arxiv_id":"1708.08450","title":"Gauge leptoquark as the origin of B-physics anomalies","url":"/paper/1708.08450","section":"The vector leptoquarks V1 and V3","sentence":"For a selection of references studying the $V_1$ leptoquark in the context of the $b→s ℓℓ$ transitions we refer the reader to Refs. [ref] .","intent_p":0.96,"contests_p":null}]}],"unlabelled_sentences":69},"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/2103.12724"}}