{"arxiv_id":"1206.1502","incoming":{"papers":22,"sentences":39,"groups":[{"kind":"method_or_tool","label":"Uses its method or tool","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1305.3173","title":"Photon Polarization in the b->s gamma processes in the Left-Right Symmetric Model","url":"/paper/1305.3173","section":"Impacts of the future photon polarization measurement on the LRSM","sentence":"Here, following the discussion in [ref] , we study the three types of methods; i) The time-dependent $CP$-asymmetry of $B→K_Sπ^0γ$ ($S_K_Sπ^0γ$), ii) The angular distribution of the $B→K_1→Kππ$ decay ($λ_$), and iii) The angular analysis of $B→K^*(→Kπ)ℓ^+ℓ^-$ ($A_T^(2), A_T^(im)$).","intent_p":0.85,"contests_p":null}]},{"kind":"data_used","label":"Uses its data or values","papers":1,"sentences":2,"quotes":[{"arxiv_id":"1501.00668","title":"Search for new physics via photon polarization of $b \\rightarrow s \\gamma$","url":"/paper/1501.00668","section":"Photon polarization in SUSY SU(5) with right-handed neutrino","sentence":"The superKEKB with an integrated luminosity of $75 ab^-1$ and the LHCb with $2 fb^-1$ might reach the 20 ($|λ_γ|=0.8 |λ_γ^SM|$) and $10%$ ($|λ_γ|=0.9 |λ_γ^SM|$) precision, respectively [ref] .","intent_p":0.81,"contests_p":null}]},{"kind":"supports_this_paper","label":"Cites it as support","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1608.02556","title":"Constraints on new physics from radiative $B$ decays","url":"/paper/1608.02556","section":"Discussion of hadronic contributions","sentence":"While simple power counting leads to a relatively large possible range for this quantity [ref] , based on more refined parametric arguments implying the existence of a helicity suppression [ref] as well as on the above numerical estimates of the soft gluon charm loop contribution to $ΔC_7'$ from LCSR, we assume an uncertainty of $±0.4×10^-2$ on the real and imaginary parts of $ΔC_7'$ and consider this to be a conservative choice.","intent_p":0.97,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":8,"sentences":8,"quotes":[{"arxiv_id":"1209.0262","title":"New Physics constraints from optimized observables in B -> K*ll at large recoil","url":"/paper/1209.0262","section":"Status of $b→s ℓ^+ℓ^-$ decays","sentence":"A wealth of model-independent combined analyses of $b→sγ$ and $b→sℓ^+ℓ^-$ decays have appeared recently in the literature [ref] .","intent_p":0.88,"contests_p":null},{"arxiv_id":"1303.5794","title":"Optimizing the basis of B->K*ll observables in the full kinematic range","url":"/paper/1303.5794","section":"Comparison with other works","sentence":"In addition to general global fits to radiative $B$-decays [ref] (see also Refs. [ref] ), there has been a growing literature aiming at determining the best set of observables with a reduced sensitivity to hadronic inputs, and the ability of these observables to find New Physics.","intent_p":0.97,"contests_p":null},{"arxiv_id":"1308.4379","title":"B -> K^* Form Factors from Flavor Data to QCD and Back","url":"/paper/1308.4379","section":"Maximum recoil","sentence":"For works exploiting the suppression of $f_+$, see [ref] .","intent_p":0.9,"contests_p":null},{"arxiv_id":"1308.1501","title":"New physics in $B \\to K^*\\mu\\mu$?","url":"/paper/1308.1501","section":"Introduction","sentence":"All of this makes this decay mode a unique laboratory to test the size, chirality structure and CP phase of the FCNC transition in the SM and beyond, as has been discussed extensively in the literature (see e.g. [ref] for recent studies).","intent_p":0.96,"contests_p":null},{"arxiv_id":"1501.04838","title":"Summary of the CKM 2014 working group on rare decays","url":"/paper/1501.04838","section":"Radiative decays","sentence":"In addition to $B→K^* ℓ^+ℓ^-$ angular observables discussed in section [ref], two important observables to access the photon polarisation are the mixing-induced asymmetry, $S_K^*γ$, in $B^0→K^*0γ$ decays and the up-down asymmetry $λ_γ$ in $B→K_1(→)γ$ decays (see [ref] and references therein).","intent_p":0.88,"contests_p":null}]}],"unlabelled_sentences":27},"outgoing":{"papers":43,"sentences":76,"groups":[{"kind":"contests","label":"Contests","papers":2,"sentences":2,"quotes":[{"arxiv_id":"1111.6307","title":"The strong decays of K1 resonances","url":"/paper/1111.6307","section":"GGPR and DDLR-inspired methods using $B→K_1(→Kππ)γ$","sentence":"Contrary to Refs. [ref] we pointed out the complex hadronic structure of $K_1(1270)→Kππ$, that we studied in great detail in Ref. [ref] .","intent_p":1.0,"contests_p":0.8},{"arxiv_id":"hep-ph/0107254","title":"Measuring the Photon Helicity in Radiative B Decays","url":"/paper/hep-ph/0107254","section":"GGPR and DDLR-inspired methods using $B→K_1(→Kππ)γ$","sentence":"Contrary to Refs. [ref] we pointed out the complex hadronic structure of $K_1(1270)→Kππ$, that we studied in great detail in Ref. [ref] .","intent_p":1.0,"contests_p":0.8}]},{"kind":"method_or_tool","label":"Uses the method or tool of","papers":1,"sentences":1,"quotes":[{"arxiv_id":"hep-ph/9911245","title":"Gluino Contribution to Radiative B Decays: Organization of QCD Corrections and Leading Order Results","url":"/paper/hep-ph/9911245","section":"SUSY models with large $(δ_RL^d)_23$ mass insertion","sentence":"Using the anomalous dimension matrix from Ref. [ref] and running the coefficients $C_7γ^ (') ()$ from the SUSY scale $M_S$ (See Eq. [ref]) to the low scale $μ_b=m_b,pole$, in Fig. [ref] we show the potential constraints on the dominant $(δ_RL^d)_23$ MIA parameter for $m_≃m_=500$ GeV (plots on the left) and 1000 GeV (plots on the right) respectively.","intent_p":0.98,"contests_p":null}]},{"kind":"data_used","label":"Uses data or values from","papers":11,"sentences":14,"quotes":[{"arxiv_id":"1010.1589","title":"Averages of b-hadron, c-hadron, and tau-lepton Properties","url":"/paper/1010.1589","section":"Current constraint on $_7γ$ by $(B→X_sγ)$ and $S_K_Sπ^0γ$","sentence":"The region outside the gray (dark gray) circle is excluded at $3σ$ ($1σ$) level by the current measurement [ref] , [equation] which we combined with the SM prediction given in Ref. [ref] .","intent_p":0.98,"contests_p":null},{"arxiv_id":"hep-ph/9805303","title":"QCD Anatomy of B -> X_s gamma Decays","url":"/paper/hep-ph/9805303","section":"Current constraint on $_7γ$ by $(B→X_sγ)$ and $S_K_Sπ^0γ$","sentence":"The region outside the gray (dark gray) circle is excluded at $3σ$ ($1σ$) level by the current measurement [ref] , [equation] which we combined with the SM prediction given in Ref. [ref] .","intent_p":0.98,"contests_p":null},{"arxiv_id":"hep-ph/9910220","title":"Photonic penguins at two loops and m_t-dependence of BR[ B -> X_s l^+ l^-]","url":"/paper/hep-ph/9910220","section":"Photon polarization in the $b→sγ$ process","sentence":"In our numerics we use $_7γ(μ_b)=-0.304$ [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"hep-ph/0412079","title":"B_{d,s}->rho, omega, K*, phi Decay Form Factors from Light-Cone Sum Rules Revisited","url":"/paper/hep-ph/0412079","section":"Intercepts and slopes of $_T^(2, im)(q^2)$ at low $q^2$","sentence":"For the ratio of the tensor form factors we use the approximation [equation] with $z=-0.030(3)$ [ref] .","intent_p":0.95,"contests_p":null},{"arxiv_id":"hep-ph/0611295","title":"An estimate of the B-->K*gamma form factor","url":"/paper/hep-ph/0611295","section":"Intercepts and slopes of $_T^(2, im)(q^2)$ at low $q^2$","sentence":"For the ratio of the tensor form factors we use the approximation [equation] with $z=-0.030(3)$ [ref] .","intent_p":0.95,"contests_p":null}]},{"kind":"comparison","label":"Compares with","papers":1,"sentences":1,"quotes":[{"arxiv_id":"hep-ph/0609037","title":"Time-dependent CP Asymmetry in B->K* gamma as a (Quasi) Null Test of the Standard Model","url":"/paper/hep-ph/0609037","section":"Discussion of the $Ø_2$ contribution to the “wrong\" helicity amplitude","sentence":"This is larger than the estimate made in Ref. [ref] (see Eq. [ref]).","intent_p":0.85,"contests_p":null}]},{"kind":"background","label":"Cites as background","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1008.2367","title":"New Physics in b -> s mu+ mu-: CP-Conserving Observables","url":"/paper/1008.2367","section":"Introduction","sentence":"In this sense the content of this paper is a contribution to the broad effort in the particle physics community to search for NP through $b→s$ exclusive decays [ref] .","intent_p":0.83,"contests_p":null}]}],"unlabelled_sentences":57},"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/1206.1502"}}