S. Herrlich

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hep-ph1996

The Complete $∣Δ S ∣ = 2$ Hamiltonian in the Next-To-Leading Order and its Phenomenological Implications

Stefan Herrlich

We briefly sketch the calculation of the effective low-energy $∣Δ S ∣ = 2$ -hamiltonian in the next-to-leading order of renormalization group improved perturbation theory. The result fo…

hep-ph1996

The Coefficient η_3 of the |ΔS|=2 Hamiltonian in the Next-To-Leading Order

Stefan Herrlich

I present the calculation of the QCD short distance coefficient $η_{3}$ of the $∣Δ S ∣ = 2$ -hamiltonian in the next-to-leading order (NLO) of renormalization group improved perturbation…

hep-ph1995

Indirect CP-Violation in the Neutral Kaon System Beyond Leading Logarithms and Related Topics

Ulrich Nierste

I describe in detail the calculation of the coefficients eta_3 and eta_1 of the low-energy Delta S=2 -hamiltonian describing K^0-K^0-bar-mixing in the next-to-leading order of reno…

The Complete ∣ΔS∣=2 Hamiltonian in the Next-To-Leading Order and its Phenomenological Implications

The Coefficient η_3 of the |ΔS|=2 Hamiltonian in the Next-To-Leading Order

Indirect CP-Violation in the Neutral Kaon System Beyond Leading Logarithms and Related Topics

The Complete $∣Δ S ∣ = 2$ Hamiltonian in the Next-To-Leading Order and its Phenomenological Implications