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Among the still unmeasured neutrino properties, the third neutrino mixing angle, theta13, is likely to be the one we will next find out.
We compute the strange quark mass from the analysis of the $f_1(1420)-f_1(1285)$ mass difference QCD sum rule, where the operator-product-expansion series is up to dimension six and to ${\cal O}(\alph...
We compute the strange quark mass from the analysis of the f1(1420) − f1(1285) mass difference QCD sum rule, where the operator-product-expansion series is up to dimension six and to O(α3 s )a...
We compute the strange quark mass from the analysis of the f1(1420) − f1(1285) mass difference QCD sum rule, where the operator-product-expansion series is up to dimension six and to O(α3 s )a...
We compute the strange quark mass from the analysis of the f1(1420) − f1(1285) mass difference QCD sum rule, where the operator-product-expansion series is up to dimension six and to O(α3 s )a...
Some claim that there are two independent mixing angles ($\theta = 35.3^\circ$, $-54.7^\circ$) between $^3P_1$ and $^1P_1$ states of heavy-light mesons in heavy quark symmetric limit, and others claim...

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