Abstract

We present recent updates for εK\varepsilon_K determined directly from the standard model (SM) with lattice QCD inputs such as B^K\hat{B}_K, ∣Vcb∣|V_{cb}|, ∣Vus∣|V_{us}|, ξ0ξ_0, ξ2ξ_2, ξLDξ_\text{LD}, fKf_K, and mcm_c. We find that the standard model with exclusive ∣Vcb∣|V_{cb}| and other lattice QCD inputs describes only 66\% of the experimental value of ∣εK∣|\varepsilon_K| and does not explain its remaining 34\%, which leads to a strong tension in ∣εK∣|\varepsilon_K| at the 4.5σ∼3.7σ4.5σ\sim 3.7σ level between the SM theory and experiment. We also find that this tension disappears when we use the inclusive value of ∣Vcb∣|V_{cb}| obtained using the heavy quark expansion based on the QCD sum rule approach.

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