{"arxiv_id":"1512.02091","incoming":{"papers":13,"sentences":15,"groups":[{"kind":"method_or_tool","label":"Uses its method or tool","papers":5,"sentences":5,"quotes":[{"arxiv_id":"2209.03863","title":"$M_W$, Dark Matter and $a_\\mu$ in the NMSSM","url":"/paper/2209.03863","section":"Experimental Constraints","sentence":"Finally, we also require that viable points satisfy (at the $2 σ$ level) all the phenomenological requirements implemented within [ implements a collection of constraints from Higgs and SUSY searches (LEP, Tevatron, LHC) and low-energy observables (flavor, quarkonia, electroweak) which are listed on the website [ref] .], in particular on the properties of the SM-like Higgs, flavor observables [ref] , the dark matter relic density as measured by Planck [ref] , and constraints on direct detection cross sections using [ref] .","intent_p":0.89,"contests_p":null},{"arxiv_id":"1703.03275","title":"Dark matter in U(1) extensions of the MSSM with gauge kinetic mixing","url":"/paper/1703.03275","section":"Phenomenological constraints","sentence":"The spectrum and all the DM observables are calculated using micrOMEGAs version 4.3.1 [ref] with the help of UMSSMTools [ref] adapted from NMSSMTools v5.0.2 routines [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"1710.10785","title":"Testing Higgs boson scenarios in the phenomenological NMSSM","url":"/paper/1710.10785","section":"Experimental constraints and fit procedure","sentence":"During the global fits, the experimental constraints used were those implemented in NMSSMTools [ref] , Lilith [ref] , and MicrOMEGAs [ref] .","intent_p":0.99,"contests_p":null},{"arxiv_id":"1602.03344","title":"A 750 GeV Diphoton Signal from a Very Light Pseudoscalar in the NMSSM","url":"/paper/1602.03344","section":"Viable scenarios with a light NMSSM pseudoscalar","sentence":"We have implemented the computation of these and many more $B$-physics observables and some $K$-physics observables in the code NMSSMTools [ref] following the update in [ref] and checked that, for the scenario presented here, the constraints are satisfied due to the mostly singlet-like nature of $A_1$ and the relatively heavy SUSY spectrum.","intent_p":0.98,"contests_p":null},{"arxiv_id":"1611.02353","title":"Enhanced Higgs associated production with a top quark pair in the NMSSM with light singlets","url":"/paper/1611.02353","section":"Non-SM-like Higgs phenomenology","sentence":"We computed these observables with NMSSMTools that follows the calculation of Ref. [ref] , which assumes Minimal Flavor Violation (MFV).","intent_p":0.96,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":2,"sentences":2,"quotes":[{"arxiv_id":"1602.03344","title":"A 750 GeV Diphoton Signal from a Very Light Pseudoscalar in the NMSSM","url":"/paper/1602.03344","section":"Viable scenarios with a light NMSSM pseudoscalar","sentence":"Constraints on such a light NMSSM pseudoscalar with a mass below $∼1$ GeV have been discussed previously in [ref] .","intent_p":0.99,"contests_p":null},{"arxiv_id":"1903.06927","title":"$B_{s(d)}-\\bar{B}_{s(d)}$ Mixing and $B_s\\to\\mu^+\\mu^-$ Decay in the NMSSM with the Flavour Expansion Theorem","url":"/paper/1903.06927","section":"Introduction","sentence":"Along with the dedicated direct searches at the Large Hadron Collider (LHC) for SUSY particles [ref] , it is also interesting and even complementary to investigate the virtual effects of these hypothesized particles on the low-energy processes, such as the neutral-meson mixings as well as the CP violation and rare decays of various hadrons [ref] .","intent_p":0.83,"contests_p":null}]}],"unlabelled_sentences":8},"outgoing":{"papers":52,"sentences":126,"groups":[{"kind":"extends","label":"Builds on","papers":2,"sentences":4,"quotes":[{"arxiv_id":"0710.3714","title":"Updated Constraints from B Physics on the MSSM and the NMSSM","url":"/paper/0710.3714","section":"Conclusions","sentence":"We have considered a set of flavour observables in the NMSSM, updating and extending our former analysis in [ref] .","intent_p":0.99,"contests_p":null},{"arxiv_id":"hep-ph/0406215","title":"NMHDECAY: A Fortran Code for the Higgs Masses, Couplings and Decay Widths in the NMSSM","url":"/paper/hep-ph/0406215","section":"Introduction","sentence":"Our aims consist in updating our previous work in [ref] to the current status of flavour observables and accordingly designing a tool for a test in the flavour-sector which will be attached to the public package [ref] .","intent_p":0.82,"contests_p":null}]},{"kind":"method_or_tool","label":"Uses the method or tool of","papers":8,"sentences":10,"quotes":[{"arxiv_id":"hep-ph/0404220","title":"b-physics signals of the lightest CP-odd Higgs in the NMSSM at large tan beta","url":"/paper/hep-ph/0404220","section":"$BR[B^0_s(d)→μ^+μ^-]$","sentence":"As in [ref] – see also [ref] –, we replace the squared Higgs mass in the denominator by a Breit-Wigner function, so as to account for potentially light Higgs states.","intent_p":0.94,"contests_p":null},{"arxiv_id":"0710.3714","title":"Updated Constraints from B Physics on the MSSM and the NMSSM","url":"/paper/0710.3714","section":"$BR[B^0_s(d)→μ^+μ^-]$","sentence":"As in [ref] – see also [ref] –, we replace the squared Higgs mass in the denominator by a Breit-Wigner function, so as to account for potentially light Higgs states.","intent_p":0.94,"contests_p":null},{"arxiv_id":"1503.01791","title":"The (Q_7,Q_{1,2}) contribution to B -> X_s gamma at O(alpha_s^2)","url":"/paper/1503.01791","section":"$B→X_s(d)γ$","sentence":"In the NNLO formalism, one can write [ref] : [equation] where: * $C$ accounts for the normalization using semi-leptonic decays: a current estimate can be extracted from Eqs.(D.1)-(D.3) of [ref] . * $P(E_0)$ encodes the perturbative contribution in the $ΔB=1$ OPE in terms of the Wilson coefficients $C_i^$ at the low-energy scale $μ_b≃2$ GeV.","intent_p":0.86,"contests_p":null},{"arxiv_id":"1206.2634","title":"Explaining B->D\\tau\\nu, B->D*\\tau\\nu and B->\\tau\\nu in a 2HDM of type III","url":"/paper/1206.2634","section":"Flavour transitions via a charged current","sentence":"We follow the analysis in [ref] which presents the corrections to the observables in a 2HDM context, allowing to account for modified Higgs-quark vertices with respect to Type II, such as those induced by $tanβ$-enhanced supersymmetric loops: see Eqs.(7-15) in the reference under consideration.","intent_p":0.89,"contests_p":null},{"arxiv_id":"1409.4557","title":"$B\\to K^{(*)}\\nu\\bar\\nu$ decays in the Standard Model and beyond","url":"/paper/1409.4557","section":"The $b→sνν̅$ transition","sentence":"We follow the analysis of [ref] (section 5.9), updated in [ref] .","intent_p":0.89,"contests_p":null}]},{"kind":"data_used","label":"Uses data or values from","papers":21,"sentences":39,"quotes":[{"arxiv_id":"1311.0903","title":"B_{s,d} -> l+ l- in the Standard Model with Reduced Theoretical Uncertainty","url":"/paper/1311.0903","section":"$BR[B^0_s(d)→μ^+μ^-]$","sentence":"The experimental status has seen the upper bound $.BR[B^0_s→μ^+μ^-]|^ <5.8·10^-8$ ($95%$ CL) replaced by an actual measurement at LHCb and CMS [ref] : [equation] The corresponding value agrees well with the recent SM calculation [ref] : [equation] It is thus no longer sufficient to consider $tanβ$-enhanced effects only, and we therefore design a full test at NLO in the new version of .","intent_p":0.84,"contests_p":null},{"arxiv_id":"1412.7515","title":"Averages of $b$-hadron, $c$-hadron, and $\\tau$-lepton properties as of summer 2014","url":"/paper/1412.7515","section":"$BR[B^0_s(d)→μ^+μ^-]$","sentence":"The experimental status has seen the upper bound $.BR[B^0_s→μ^+μ^-]|^ <5.8·10^-8$ ($95%$ CL) replaced by an actual measurement at LHCb and CMS [ref] : [equation] The corresponding value agrees well with the recent SM calculation [ref] : [equation] It is thus no longer sufficient to consider $tanβ$-enhanced effects only, and we therefore design a full test at NLO in the new version of .","intent_p":0.84,"contests_p":null},{"arxiv_id":"1411.4413","title":"Observation of the rare $B^0_s\\to\\mu^+\\mu^-$ decay from the combined analysis of CMS and LHCb data","url":"/paper/1411.4413","section":"$BR[B^0_s(d)→μ^+μ^-]$","sentence":"The experimental status has seen the upper bound $.BR[B^0_s→μ^+μ^-]|^ <5.8·10^-8$ ($95%$ CL) replaced by an actual measurement at LHCb and CMS [ref] : [equation] The corresponding value agrees well with the recent SM calculation [ref] : [equation] It is thus no longer sufficient to consider $tanβ$-enhanced effects only, and we therefore design a full test at NLO in the new version of .","intent_p":0.84,"contests_p":null},{"arxiv_id":"1310.8555","title":"Review of lattice results concerning low energy particle physics","url":"/paper/1310.8555","section":"$BR[B^0_s(d)→μ^+μ^-]$","sentence":"In practice, we use the quantities $m_B_d=5.27958$ [ref] , $τ_B_d=(1.520±0.004)$ ps [ref] , $f_B_d=(188.5±5.25)$ MeV – again an ad-hoc combination of the various results presented in [ref] – and $|V_tbV_td^*|= (8.6±2.8)·10^-3$ [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"1503.01789","title":"Updated NNLO QCD predictions for the weak radiative B-meson decays","url":"/paper/1503.01789","section":"$B→X_s(d)γ$","sentence":"As before, the SM + CKM + Non-Perturbative uncertainties are taken over from [ref] , Eq.(8) – again we double the error bands to test the observable at the $2σ$ level – and we add linearly the new physics uncertainties.","intent_p":0.96,"contests_p":null}]},{"kind":"comparison","label":"Compares with","papers":7,"sentences":9,"quotes":[{"arxiv_id":"1412.7515","title":"Averages of $b$-hadron, $c$-hadron, and $\\tau$-lepton properties as of summer 2014","url":"/paper/1412.7515","section":"$B_d,s^0$ oscillation parameters $ΔM_d,s$","sentence":"These results are then confronted to the experimental measurements [ref] : [equation]","intent_p":0.86,"contests_p":null},{"arxiv_id":"1108.2036","title":"Next-to-Next-to-Leading-Order Charm-Quark Contribution to the CP Violation Parameter epsilon_K and Delta M_K","url":"/paper/1108.2036","section":"$K-K̅$ mixing","sentence":"Note that [ref] and [ref] also propose recent evaluations of the quantity $η_cc$, with slightly lower central value, but we choose to stick to the conservative estimate of [ref] .","intent_p":0.81,"contests_p":null},{"arxiv_id":"1304.6835","title":"Stringent Tests of Constrained Minimal Flavour Violation through Delta F=2 Transitions","url":"/paper/1304.6835","section":"$K-K̅$ mixing","sentence":"Note that [ref] and [ref] also propose recent evaluations of the quantity $η_cc$, with slightly lower central value, but we choose to stick to the conservative estimate of [ref] .","intent_p":0.81,"contests_p":null},{"arxiv_id":"1503.05388","title":"Standard Model evaluation of $\\varepsilon_K$ using lattice QCD inputs for $\\hat{B}_K$ and $V_{cb}$","url":"/paper/1503.05388","section":"$K-K̅$ mixing","sentence":"Note that [ref] and [ref] also propose recent evaluations of the quantity $η_cc$, with slightly lower central value, but we choose to stick to the conservative estimate of [ref] .","intent_p":0.81,"contests_p":null},{"arxiv_id":"1310.8555","title":"Review of lattice results concerning low energy particle physics","url":"/paper/1310.8555","section":"$B_d,s^0$ oscillation parameters $ΔM_d,s$","sentence":"This is essentially due to the choice for the lattice input: [ref] have their own averaging, leading to a smaller form factor, while we follow [ref] .","intent_p":0.89,"contests_p":null}]},{"kind":"background","label":"Cites as background","papers":14,"sentences":15,"quotes":[{"arxiv_id":"1311.1348","title":"Electroweak Corrections to $B_{s,d} \\to \\ell^+ \\ell^-$","url":"/paper/1311.1348","section":"$BR[B^0_s(d)→μ^+μ^-]$","sentence":"* The SM contribution to $BR[B^0_s→μ^+μ^-]$ is known up to three-loop QCD [ref] and leading QED order [ref] .","intent_p":0.8,"contests_p":null},{"arxiv_id":"1311.1347","title":"Three-loop QCD corrections to B_s -> mu^+ mu^-","url":"/paper/1311.1347","section":"$BR[B^0_s(d)→μ^+μ^-]$","sentence":"* The SM contribution to $BR[B^0_s→μ^+μ^-]$ is known up to three-loop QCD [ref] and leading QED order [ref] .","intent_p":0.8,"contests_p":null},{"arxiv_id":"0710.3714","title":"Updated Constraints from B Physics on the MSSM and the NMSSM","url":"/paper/0710.3714","section":"$BR[B^0_s(d)→μ^+μ^-]$","sentence":"$BR[B^0_s→μ^+μ^-]$ is the observable where the evolution since [ref] has been the most critical.","intent_p":0.86,"contests_p":null},{"arxiv_id":"1005.4087","title":"Study of B -> X gamma Decays and Determination of |V_td/V_ts|","url":"/paper/1005.4087","section":"$B→X_s(d)γ$","sentence":"Now let us turn to $BR[B̅→X_dγ]$. $BR[B̅→X_dγ]$ was originally considered in [ref] at NLO and then, in view of the BABAR measurement [ref] , by [ref] .","intent_p":0.91,"contests_p":null},{"arxiv_id":"1106.5499","title":"B -> X_d gamma and constraints on new physics","url":"/paper/1106.5499","section":"$B→X_s(d)γ$","sentence":"Now let us turn to $BR[B̅→X_dγ]$. $BR[B̅→X_dγ]$ was originally considered in [ref] at NLO and then, in view of the BABAR measurement [ref] , by [ref] .","intent_p":0.91,"contests_p":null}]}],"unlabelled_sentences":49},"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/1512.02091"}}