<p>We reconsider the constraints on the form factors <i>W</i><sub>+</sub>(<i>s</i>) and <i>W</i><sub><i>S</i></sub>(<i>s</i>), describing the radiative decay modes <i>K</i><sup>+</sup> → <i>π</i><sup>+</sup><i>ℓ</i><sup>+</sup><i>ℓ</i><sup><i>−</i></sup> and <i>K</i><sub><i>S</i></sub> → <i>π</i><sup>0</sup><i>ℓ</i><sup>+</sup><i>ℓ</i><sup><i>−</i></sup>, associated with the general properties of analyticity and unitarity. Starting from the simple consideration of the asymptotic behaviours of the two combinations 2<i>W</i><sub>+</sub>(<i>s</i>) − <i>W</i><sub><i>S</i></sub>(<i>s</i>) and <i>W</i><sub>+</sub>(<i>s</i>) + <i>W</i><sub><i>S</i></sub>(<i>s</i>), we derive a minimal pair of dispersive representations which involves only two free parameters. An important input for these representations consists of the <i>K</i> → 3<i>π</i> decay amplitudes, for which we use a set of solutions of the Khuri-Treiman equations obtained recently. These solutions provide an extrapolation from the physical <i>K</i> → 3<i>π</i> decay region up to the resonant <i>Kπ</i> → <i>ππ</i> scattering regions. We show that the experimental energy dependence of |<i>W</i><sub>+</sub>|<sup>2</sup> can be well reproduced and that the sign of <i>W</i><sub>+</sub> is unambiguously determined. We also show that the yet unknown ∆<i>I</i> = 1<i>/</i>2 part of the <i>K</i><sub><i>S</i></sub> → <i>π</i><sup>+</sup><i>π</i><sup><i>−</i></sup><i>π</i><sup>0</sup> amplitude can be determined from the value of <i>W</i><sub>+</sub>(0) + <i>W</i><sub><i>S</i></sub>(0). The possibility of fixing the sign of <i>W</i><sub><i>S</i></sub>(0) using experimental data on both |<i>W</i><sub>+</sub>|<sup>2</sup> and |<i>W</i><sub><i>S</i></sub>|<sup>2</sup> is discussed.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

A dispersive approach to the CP conserving K → πℓ+ radiative decays

  • Véronique Bernard,
  • Sébastien Descotes-Genon,
  • Marc Knecht,
  • Bachir Moussallam

摘要

We reconsider the constraints on the form factors W+(s) and WS(s), describing the radiative decay modes K+π++ and KSπ0+, associated with the general properties of analyticity and unitarity. Starting from the simple consideration of the asymptotic behaviours of the two combinations 2W+(s) − WS(s) and W+(s) + WS(s), we derive a minimal pair of dispersive representations which involves only two free parameters. An important input for these representations consists of the K → 3π decay amplitudes, for which we use a set of solutions of the Khuri-Treiman equations obtained recently. These solutions provide an extrapolation from the physical K → 3π decay region up to the resonant ππ scattering regions. We show that the experimental energy dependence of |W+|2 can be well reproduced and that the sign of W+ is unambiguously determined. We also show that the yet unknown ∆I = 1/2 part of the KSπ+ππ0 amplitude can be determined from the value of W+(0) + WS(0). The possibility of fixing the sign of WS(0) using experimental data on both |W+|2 and |WS|2 is discussed.