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KπννK\to \pi \nu\overline{\nu} in the MSSM in Light of the ϵK/ϵK\epsilon^{\prime}_K/\epsilon_K Anomaly

Abstract

The Standard-Model (SM) prediction for the CP-violating quantity ϵK/ϵK\epsilon_K^{\prime}/\epsilon_K deviates from its measured value by 2.8 σ\sigma. It has been shown that this tension can be resolved within the Minimal Supersymmetric Standard Model (MSSM) through gluino-squark box diagrams, even if squarks and gluinos are much heavier than 1 TeV. The rare decays KLπ0ννˉK_L \to \pi^0\nu\bar{\nu} and K+π+ννˉK^+ \to \pi^+\nu\bar{\nu} are similarly sensitive to very high mass scales and the first one also measures CP violation. In this article, we analyze the correlations between ϵK/ϵK\epsilon^{\prime}_K/\epsilon_K and B(KLπ0ννˉ)B(K_L \to \pi^0\nu\bar{\nu}) and B(K+π+ννˉ)B(K^+ \to \pi^+\nu\bar{\nu}) within the MSSM aiming at an explanation of ϵK/ϵK\epsilon_K^{\prime}/\epsilon_K via gluino-squark box diagrams. The dominant MSSM contribution to the KπννˉK \to \pi\nu\bar{\nu} branching fractions stems from box diagrams with squarks, sleptons, charginos, and neutralinos, and the pattern of the correlations is different from the widely studied ZZ-penguin scenarios. This is interesting in light of future precision measurements by KOTO and NA62 at J-PARC and CERN, respectively. We find B(KLπ0ννˉ)/BSM(KLπ0ννˉ)2(1.2)B(K_L \to \pi^0\nu\bar{\nu})/B^{SM} (K_L \to \pi^0\nu\bar{\nu})\lesssim 2\,(1.2) and B(K+π+ννˉ)/BSM(K+π+ννˉ)1.4(1.1)B(K^+ \to \pi^+\nu\bar{\nu})/B^{SM}(K^+ \to \pi^+\nu\bar{\nu}) \lesssim 1.4\,(1.1), if all squark masses are above 1.5 TeV, gaugino masses obey GUT relations, and if one allows for a fine-tuning at the 1%(10%)1\%\,(10\%) level for the gluino mass. Larger values are possible for a tuned CP violating phase. Furthermore, the sign of the MSSM contribution to ϵK\epsilon_K^{\prime} imposes a strict correlation between B(KLπ0ννˉ)B(K_L \to \pi^0\nu\bar{\nu}) and the hierarchy between the masses mUˉm_{\bar{U}}, mDˉm_{\bar{D}} of the right-handed up-squark and down-squark: sgn[B(KLπ0ννˉ)BSM(KLπ0ννˉ)]=[B(K_L \to \pi^0\nu\bar{\nu})-B^{SM} (K_L \to \pi^0\nu\bar{\nu})] = sgn(mUˉmDˉ)(m_{\bar{U}}-m_{\bar{D}}) .Comment: 9 pages, 5 figures; references added, version published in PR

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