Abstract <p>Five rare radiative kaon decays, <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(K^{+}\to\pi^{0}\mu^{+}\nu_{\mu}\gamma\)</EquationSource> <!--BPhysMGU2570272Tiurin-m3--> </InlineEquation>, <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(K^{+}\to\pi^{0}e^{+}\nu_{e}\gamma\)</EquationSource> <!--BPhysMGU2570272Tiurin-m4--> </InlineEquation>, <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(K^{+}\to\mu^{+}\nu_{\mu}\gamma\)</EquationSource> <!--BPhysMGU2570272Tiurin-m5--> </InlineEquation>, <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(K^{+}\to e^{+}\nu_{e}\gamma\)</EquationSource> <!--BPhysMGU2570272Tiurin-m6--> </InlineEquation>, <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(K^{+}\to\pi^{+}\pi^{0}\pi^{0}\gamma\)</EquationSource> <!--BPhysMGU2570272Tiurin-m7--> </InlineEquation> are studied by OKA experiment at the RF-separated 17.7 GeV/<i>c</i> momentum kaon beam of the IHEP U-70 proton synchrotron. For the first two decays, branching ratios are obtained and <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(T\)</EquationSource> <!--BPhysMGU2570272Tiurin-m8--> </InlineEquation>-odd correlation is measured. For the <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(K^{+}\to\mu^{+}\nu_{\mu}\gamma\)</EquationSource> <!--BPhysMGU2570272Tiurin-m9--> </InlineEquation> decay vector and axial-vector form factors difference <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(F_{V}-F_{A}\)</EquationSource> <!--BPhysMGU2570272Tiurin-m10--> </InlineEquation> is measured. For the <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(K^{+}\to e^{+}\nu_{e}\gamma\)</EquationSource> <!--BPhysMGU2570272Tiurin-m11--> </InlineEquation> decay branching ratio is measured. For the <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(K^{+}\to\pi^{+}\pi^{0}\pi^{0}\gamma\)</EquationSource> <!--BPhysMGU2570272Tiurin-m12--> </InlineEquation> decay branching ratios is obtained. For <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(K^{+}\to\pi^{0}\mu^{+}\nu_{\mu}\gamma\)</EquationSource> <!--BPhysMGU2570272Tiurin-m13--> </InlineEquation> a discrepancy of 4.6<InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(\sigma\)</EquationSource> <!--BPhysMGU2570272Tiurin-m14--> </InlineEquation> above calcullations without structure radiation is observed. For Br (<InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(K^{+}\to\pi^{0}e^{+}\nu_{e}\gamma\)</EquationSource> <!--BPhysMGU2570272Tiurin-m15--> </InlineEquation>) a discrepancy of &gt; 5<InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(\sigma\)</EquationSource> <!--BPhysMGU2570272Tiurin-m16--> </InlineEquation> for the same case is observed. For <InlineEquation ID="IEq17"> <EquationSource Format="TEX">\(F_{V}-F_{A}\)</EquationSource> <!--BPhysMGU2570272Tiurin-m17--> </InlineEquation> (<InlineEquation ID="IEq18"> <EquationSource Format="TEX">\(K^{+}\to\mu^{+}\nu_{\mu}\gamma\)</EquationSource> <!--BPhysMGU2570272Tiurin-m18--> </InlineEquation> decay) a discrepancy of 2.9<InlineEquation ID="IEq19"> <EquationSource Format="TEX">\(\sigma\)</EquationSource> <!--BPhysMGU2570272Tiurin-m19--> </InlineEquation> above <InlineEquation ID="IEq20"> <EquationSource Format="TEX">\(\chi\)</EquationSource> <!--BPhysMGU2570272Tiurin-m20--> </InlineEquation>PT is observed. Our results are considered as preliminary.</p>

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Current Status of Study of the Rare Radiative \(\boldsymbol{K^{+}}\) Decays by OKA Collaboration

  • I. S. Tiurin

摘要

Abstract

Five rare radiative kaon decays, \(K^{+}\to\pi^{0}\mu^{+}\nu_{\mu}\gamma\) , \(K^{+}\to\pi^{0}e^{+}\nu_{e}\gamma\) , \(K^{+}\to\mu^{+}\nu_{\mu}\gamma\) , \(K^{+}\to e^{+}\nu_{e}\gamma\) , \(K^{+}\to\pi^{+}\pi^{0}\pi^{0}\gamma\) are studied by OKA experiment at the RF-separated 17.7 GeV/c momentum kaon beam of the IHEP U-70 proton synchrotron. For the first two decays, branching ratios are obtained and \(T\) -odd correlation is measured. For the \(K^{+}\to\mu^{+}\nu_{\mu}\gamma\) decay vector and axial-vector form factors difference \(F_{V}-F_{A}\) is measured. For the \(K^{+}\to e^{+}\nu_{e}\gamma\) decay branching ratio is measured. For the \(K^{+}\to\pi^{+}\pi^{0}\pi^{0}\gamma\) decay branching ratios is obtained. For \(K^{+}\to\pi^{0}\mu^{+}\nu_{\mu}\gamma\) a discrepancy of 4.6 \(\sigma\) above calcullations without structure radiation is observed. For Br ( \(K^{+}\to\pi^{0}e^{+}\nu_{e}\gamma\) ) a discrepancy of > 5 \(\sigma\) for the same case is observed. For \(F_{V}-F_{A}\) ( \(K^{+}\to\mu^{+}\nu_{\mu}\gamma\) decay) a discrepancy of 2.9 \(\sigma\) above \(\chi\) PT is observed. Our results are considered as preliminary.