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On lattice extraction of K --> pi pi amplitudes to O(p^4) in Chiral Perturbation Theory
High Energy Physics - Phenomenology · Submitted 12 Mar 2002
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We show that lattice calculation of K --> pi pi and $epe$ amplitudes for (8,1) and (27,1) operators to O(p^4) in chiral perturbation theory is feasible when one uses K --> pi pi computations at the two unphysical kinematics allowed by the Maiani-Testa theorem, along with the usual (computable) two and three point functions, namely K --> 0, K --> pi (with momentum) and K - bar{K}.
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The abstract, sentence by sentence
We show that lattice calculation of K --> pi pi and $epe$ amplitudes for (8,1) and (27,1) operators to O(p^4) in chiral perturbation theory is feasible when one uses K --> pi pi computations at the two unphysical kinematics allowed by the Maiani-Testa theorem, along with the usual (computable) two and three point functions, namely K --> 0, K --> pi (with momentum) and K - bar{K}. Explicit expressions for the finite logarithms emerging from our O(p^4) analysis to the above amplitudes are also given.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We show that lattice calculation of K --> pi pi and $epe$ amplitudes for (8,1) and (27,1) operators to O(p^4) in chiral perturbation theory is feasible when one uses K --> pi pi computations at the two unphysical kinematics allowed by the Maiani-Testa theorem, along with the usual (computable) two and three point functions, namely K --> 0, K --> pi (with momentum) and K - bar{K}. | contribution 0.64 | 0.80 | 0.89 | asserted 0.96 |
| s1 | Explicit expressions for the finite logarithms emerging from our O(p^4) analysis to the above amplitudes are also given. | result 0.56 | 0.92 | 0.07 | asserted 1.00 |
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The paper
Original abstract
We show that lattice calculation of K --> pi pi and $epe$ amplitudes for (8,1) and (27,1) operators to O(p^4) in chiral perturbation theory is feasible when one uses K --> pi pi computations at the two unphysical kinematics allowed by the Maiani-Testa theorem, along with the usual (computable) two and three point functions, namely K --> 0, K --> pi (with momentum) and K - bar{K}. Explicit expressions for the finite logarithms emerging from our O(p^4) analysis to the above amplitudes are also given.
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How the literature uses it
4 arXiv papers cite this in 6 sentences
Papers citing it · 4 sentences without a confident label
Uses its method or tool 1 paper
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For $ℳ_(27,1)^log$ we use Eq. (C5) in [ref] , (where we have added logarithmic terms from $(m_K^2-m_π^2)_1-loop$ by hand as necessitated by Eq. ([ref]) and corrected a factor of $1/f^2$ in equation (A2)), and for $ℳ_(8,8)^log$ we use Eq. (E3) in [ref] .
Lattice determination of the $K \to (\pi\pi)_{I=2}$ Decay Amplitude $A_2$ · Finite-Volume Corrections · 0.88
Cites it as background 1 paper
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[For important theoretical and numerical developments regarding nonleptonic weak decay on the lattice see Refs. [ref] .]).
Multichannel one-to-two transition amplitudes in a finite volume · Introduction · 0.99
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