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[ref] for a SUSY mass of $100$ GeV and in [ref] for a mass of $500$ GeV – as explained above, our limits can be confronted to the bounds applying on $∑_iλ'_i13λ'_i31$, etc., in these references.","intent_p":0.99,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":2,"sentences":2,"quotes":[{"arxiv_id":"1810.08228","title":"Updating Bounds on $R$-Parity Violating Supersymmetry from Meson Oscillation Data","url":"/paper/1810.08228","section":"Introduction","sentence":"Such observables have been discussed in the R-parity conserving [ref] as well as in an RpV context in the past [ref] .","intent_p":0.95,"contests_p":null},{"arxiv_id":"1511.09466","title":"CP Violation in the $B_s^0$ system","url":"/paper/1511.09466","section":"Model independent constraints on new physics","sentence":"We present here some examples, not an exhaustive list: super-symmetric contributions were discussed e.g. by [ref] ; contributions of 2 Higgs-double models were discussed e.g. by [ref] ; extra dimensions were discussed in [ref] ; L-R symmetric models were discussed e.g. in [ref] ; extended gauge sectors were discussed e.g. in [ref] ; additional fermions[A sequential, chiral, perturbative fourth generation of fermions is already excluded by experiment, see e.g. [ref] .","intent_p":0.96,"contests_p":null}]}],"unlabelled_sentences":6},"outgoing":{"papers":33,"sentences":52,"groups":[{"kind":"data_used","label":"Uses data or values from","papers":11,"sentences":13,"quotes":[{"arxiv_id":"1005.2757","title":"Evidence for an anomalous like-sign dimuon charge asymmetry","url":"/paper/1005.2757","section":"Numerical results and discussions","sentence":"The following experimental data at 95% C.L. are used to constrain relevant $R_p$ couplings [ref]","intent_p":1.0,"contests_p":null},{"arxiv_id":"0712.2397","title":"First Flavor-Tagged Determination of Bounds on Mixing-Induced CP Violation in Bs -> J/psi phi Decays","url":"/paper/0712.2397","section":"Numerical results and discussions","sentence":"The following experimental data at 95% C.L. are used to constrain relevant $R_p$ couplings [ref]","intent_p":1.0,"contests_p":null},{"arxiv_id":"0802.2255","title":"Measurement of $\\boldmath {B_s^0}$ mixing parameters from the flavor-tagged decay","url":"/paper/0802.2255","section":"Numerical results and discussions","sentence":"The following experimental data at 95% C.L. are used to constrain relevant $R_p$ couplings [ref]","intent_p":1.0,"contests_p":null},{"arxiv_id":"0906.0953","title":"New Physics from Flavour","url":"/paper/0906.0953","section":"Introduction","sentence":"The CP violating phase measured by both CDF and DØ is [ref] [equation] However, the CP violating phase is predicted precisely to be small in the SM [ref] , $ϕ^J/ψϕ,_s=2β_s^≡2(-V_tsV^*_tb/V_csV^*_cb)≈0.04$.","intent_p":0.9,"contests_p":null},{"arxiv_id":"0803.0659","title":"First Evidence of New Physics in b <--> s Transitions","url":"/paper/0803.0659","section":"Introduction","sentence":"The CP violating phase measured by both CDF and DØ is [ref] [equation] However, the CP violating phase is predicted precisely to be small in the SM [ref] , $ϕ^J/ψϕ,_s=2β_s^≡2(-V_tsV^*_tb/V_csV^*_cb)≈0.04$.","intent_p":0.9,"contests_p":null}]},{"kind":"comparison","label":"Compares with","papers":5,"sentences":9,"quotes":[{"arxiv_id":"hep-ph/0608341","title":"$B_s-\\bar{B_s}$ mixing, B decays and R-parity violating supersymmetry","url":"/paper/hep-ph/0608341","section":"Summary","sentence":"The similar analysis was performed only from the bound on $ΔM_s$ in Refs. [ref] , in this paper we have used the current bounds not only on $ΔM_s$ but also on $ϕ_s^J/ψϕ$ and $ΔΓ_s$ as given in Eqs. ([ref]-[ref]).","intent_p":0.8,"contests_p":null},{"arxiv_id":"hep-ph/0609276","title":"Probe the R-parity Violating Supersymmetry Effects in the $B^0_s-\\bar{B}^0_s$ Mixing","url":"/paper/hep-ph/0609276","section":"Summary","sentence":"The similar analysis was performed only from the bound on $ΔM_s$ in Refs. [ref] , in this paper we have used the current bounds not only on $ΔM_s$ but also on $ϕ_s^J/ψϕ$ and $ΔΓ_s$ as given in Eqs. ([ref]-[ref]).","intent_p":0.8,"contests_p":null},{"arxiv_id":"hep-ph/9609443","title":"R-Parity Violation and Quark Flavour Violation","url":"/paper/hep-ph/9609443","section":"$L$ couplings","sentence":"* Almost all bounds on the moduli of $L$ coupling products from current 95% C.L. data of $ΔM_s$, $ϕ_s^J/ψϕ$ and $ΔΓ_s$ are stronger than previous ones in Refs. 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[ref] , and some moduli of them may have better bounds from the decays.","intent_p":0.99,"contests_p":null},{"arxiv_id":"hep-ph/0610338","title":"Probe R-parity Violating Supersymmetry Effects in $B\\to K^{(*)}\\ell^+\\ell^-$ and $B_s\\to \\ell^+\\ell^-$ Decays","url":"/paper/hep-ph/0610338","section":"$L$ couplings","sentence":"* Almost all bounds on the moduli of $L$ coupling products from current 95% C.L. data of $ΔM_s$, $ϕ_s^J/ψϕ$ and $ΔΓ_s$ are stronger than previous ones in Refs. [ref] , which are obtained only from the 68% C.L. data of $ΔM_s$. $L$ couplings that may contribute to $B_s^0-B̅_s^0$ mixing also affect various decays, relevant $L$ coupling effects in the decays have already been studied in Refs. 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