{"arxiv_id":"1207.3016","incoming":{"papers":10,"sentences":14,"groups":[{"kind":"extends","label":"Builds on it","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1205.5787","title":"Gluinos lighter than squarks and detection at the LHC","url":"/paper/1205.5787","section":"Limits from kaon physics","sentence":"Then, according to the motivations above, what do here, as a complement of [ref] , is to * Assess the importance of considering NLO effects in setting the limits of the masses of d type squarks and the flavour violating parameters $(δ^d_XY)_12$ for the case of three heavy squarks families and a light gluino. * Check that the values of squarks masses, in the range considered, and the real parts of $(δ^d_XY)_12$ satisfy the bounds set by $Δm_K$. * Put constraints on the imaginary parts of $(δ^d_XY)_12$.","intent_p":1.0,"contests_p":null}]},{"kind":"method_or_tool","label":"Uses its method or tool","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1606.07090","title":"Dirac vs Majorana 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Next-to-Leading Order","url":"/paper/hep-ph/9809437","section":"Conclusions","sentence":"In order to estimate the gluino contributions to $Δm_K$ and the CP-violating parameter $ϵ$, we used the evolution of Wilson coefficients from reference [ref] , where a scenario with two heavy families of squarks and a lighter third family with a mass comparable to that of the gluino was considered.","intent_p":0.91,"contests_p":null},{"arxiv_id":"hep-ph/9606211","title":"Precision Corrections in the Minimal Supersymmetric Standard Model","url":"/paper/hep-ph/9606211","section":"Evolution between squark and gluino mass scales","sentence":"We transform to the running mass $M_3(m_g̃)$, taking into account one-loop corrections [ref] involving gluinos and (if applicable) one generation of squarks with mass $m_g̃$, [equation] In the case of three heavy generations of squarks, we run using the $β$ functions of eq:betafuncts_3heavysquarks.","intent_p":0.89,"contests_p":null},{"arxiv_id":"1204.2645","title":"Decoupling heavy sparticles in Effective SUSY scenarios: Unification, Higgs masses and tachyon bounds","url":"/paper/1204.2645","section":"Beta functions","sentence":"Initially guessing values for $ĝ_s(m_g̃)$ and $γ_s(m_g̃)$, we run up to the scale $m_q̃$, where we apply the $$ matching conditions [ref] [equation] We then run down to $m_g̃$ and again set the QCD coupling to the correct value determined initially.","intent_p":0.98,"contests_p":null}]},{"kind":"data_used","label":"Uses data or values from","papers":11,"sentences":14,"quotes":[{"arxiv_id":"1207.1287","title":"Kaon Mixing Beyond the SM from Nf=2 tmQCD and model independent constraints from the UTA","url":"/paper/1207.1287","section":"Limits from $Δm_K$","sentence":"These expressions differ by a factor of $1/8 M_K$ from the corresponding ones in the lattice study [ref] , whose results for the bag parameters $B_i$ we use.","intent_p":0.91,"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":"Limits from $Δm_K$","sentence":"Hence, the best one can do is to compare the best estimate obtained from the short-distance contributions [ref] , denoted by $Δm_K^SD$, to the experimental value Δm_K^exp = (3.483 ±0.0059)×10^-15 , Δm_K^SD = (3.1 ±1.2)×10^-15 ,","intent_p":0.97,"contests_p":null},{"arxiv_id":"1111.1699","title":"The $K\\to(\\pi\\pi)_{I=2}$ Decay Amplitude from Lattice QCD","url":"/paper/1111.1699","section":"Limits from $ϵ$","sentence":"We use the same value $κ_ϵ=0.923$ [ref] as [ref] .","intent_p":0.98,"contests_p":null},{"arxiv_id":"hep-ph/9711402","title":"Next-to-Leading Order QCD Corrections to $\\Delta F =2$ effective Hamiltonians","url":"/paper/hep-ph/9711402","section":"Renormalization group evolution of the Wilson 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the NLO QCD corrections and (iii) to understand the difference between the scenarios with two and three heavy families of squarks.","intent_p":1.0,"contests_p":null},{"arxiv_id":"1207.1287","title":"Kaon Mixing Beyond the SM from Nf=2 tmQCD and model independent constraints from the UTA","url":"/paper/1207.1287","section":"Limits from $Δm_K$","sentence":"This work uses the same state normalization as [ref] , as one can verify by comparing their definitions of operators and matrix elements, taking into account that the kaon decay constant is normalized differently ($f_K$ of [ref] corresponds to $√(2) F_K$ of [ref] ).] The definition [ref] ensures that the numerical values of the bag parameters are the same in both conventions.","intent_p":0.8,"contests_p":null},{"arxiv_id":"hep-lat/0605016","title":"K^0-\\bar K^0 mixing beyond the standard model and CP-violating electroweak penguins in quenched QCD with exact chiral symmetry","url":"/paper/hep-lat/0605016","section":"Limits from 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