<p>A measurement of the <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_25632_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="93" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <msup> <mi>K</mi> <mo>+</mo> </msup> <mo>→</mo> <msup> <mi>π</mi> <mo>+</mo> </msup> <mi>ν</mi> <mover accent="true"> <mi>ν</mi> <mo stretchy="true">¯</mo> </mover> </math></EquationSource> <EquationSource Format="TEX">\( {K}^{+}\to {\pi}^{+}\nu \overline{\nu} \)</EquationSource> </InlineEquation> decay by the NA62 experiment at the CERN SPS is presented, using data collected in 2021 and 2022. This dataset was recorded, after modifications to the beamline and detectors, at a higher instantaneous beam intensity with respect to the 2016–2018 data taking. Combining NA62 data collected in 2016–2022, a measurement of <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_25632_Article_IEq3.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="268" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <mi mathvariant="script">B</mi> <mfenced close=")" open="("> <mrow> <msup> <mi>K</mi> <mo>+</mo> </msup> <mo>→</mo> <msup> <mi>π</mi> <mo>+</mo> </msup> <mi>ν</mi> <mover accent="true"> <mi>ν</mi> <mo stretchy="true">¯</mo> </mover> </mrow> </mfenced> <mo>=</mo> <mfenced close=")" open="("> <msubsup> <mn>13.0</mn> <mrow> <mo>−</mo> <mn>3.0</mn> </mrow> <mrow> <mo>+</mo> <mn>3.3</mn> </mrow> </msubsup> </mfenced> <mo>×</mo> <msup> <mn>10</mn> <mrow> <mo>−</mo> <mn>11</mn> </mrow> </msup> </math></EquationSource> <EquationSource Format="TEX">\( \mathcal{B}\left({K}^{+}\to {\pi}^{+}\nu \overline{\nu}\right)=\left({13.0}_{-3.0}^{+3.3}\right)\times {10}^{-11} \)</EquationSource> </InlineEquation> is reported. With 51 signal candidates observed and an expected background of <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_25632_Article_IEq4.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="33" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <msubsup> <mn>18</mn> <mrow> <mo>−</mo> <mn>2</mn> </mrow> <mrow> <mo>+</mo> <mn>3</mn> </mrow> </msubsup> </math></EquationSource> <EquationSource Format="TEX">\( {18}_{-2}^{+3} \)</EquationSource> </InlineEquation> events, <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_25632_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="119" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <mi mathvariant="script">B</mi> <mfenced close=")" open="("> <mrow> <msup> <mi>K</mi> <mo>+</mo> </msup> <mo>→</mo> <msup> <mi>π</mi> <mo>+</mo> </msup> <mi>ν</mi> <mover accent="true"> <mi>ν</mi> <mo stretchy="true">¯</mo> </mover> </mrow> </mfenced> </math></EquationSource> <EquationSource Format="TEX">\( \mathcal{B}\left({K}^{+}\to {\pi}^{+}\nu \overline{\nu}\right) \)</EquationSource> </InlineEquation> becomes the smallest branching ratio measured with a signal significance above 5<i>σ</i>.</p>

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Observation of the \( {K}^{+}\to {\pi}^{+}\nu \overline{\nu} \) decay and measurement of its branching ratio

  • E. Cortina Gil,
  • J. Jerhot,
  • N. Lurkin,
  • T. Numao,
  • B. Velghe,
  • V. W. S. Wong,
  • D. Bryman,
  • Z. Hives,
  • T. Husek,
  • K. Kampf,
  • M. Kolesar,
  • M. Koval,
  • B. De Martino,
  • M. Perrin-Terrin,
  • L. Petit,
  • B. Döbrich,
  • S. Lezki,
  • J. Schubert,
  • A. T. Akmete,
  • R. Aliberti,
  • M. Ceoletta,
  • L. Di Lella,
  • N. Doble,
  • L. Peruzzo,
  • C. Polivka,
  • S. Schuchmann,
  • H. Wahl,
  • R. Wanke,
  • P. Dalpiaz,
  • R. Negrello,
  • I. Neri,
  • F. Petrucci,
  • M. Soldani,
  • L. Bandiera,
  • N. Canale,
  • A. Cotta Ramusino,
  • A. Gianoli,
  • M. Romagnoni,
  • A. Sytov,
  • M. Lenti,
  • P. Lo Chiatto,
  • I. Panichi,
  • G. Ruggiero,
  • A. Bizzeti,
  • F. Bucci,
  • A. Antonelli,
  • V. Kozhuharov,
  • G. Lanfranchi,
  • S. Martellotti,
  • M. Moulson,
  • T. Spadaro,
  • G. Tinti,
  • F. Ambrosino,
  • M. D’Errico,
  • R. Fiorenza,
  • M. Francesconi,
  • R. Giordano,
  • P. Massarotti,
  • M. Mirra,
  • M. Napolitano,
  • I. Rosa,
  • G. Saracino,
  • G. Anzivino,
  • P. Cenci,
  • V. Duk,
  • R. Lollini,
  • P. Lubrano,
  • M. Pepe,
  • M. Piccini,
  • F. Costantini,
  • M. Giorgi,
  • S. Giudici,
  • G. Lamanna,
  • E. Lari,
  • E. Pedreschi,
  • J. Pinzino,
  • M. Sozzi,
  • R. Fantechi,
  • F. Spinella,
  • I. Mannelli,
  • M. Raggi,
  • A. Biagioni,
  • P. Cretaro,
  • O. Frezza,
  • A. Lonardo,
  • M. Turisini,
  • P. Vicini,
  • R. Ammendola,
  • V. Bonaiuto,
  • A. Fucci,
  • A. Salamon,
  • F. Sargeni,
  • R. Arcidiacono,
  • B. Bloch-Devaux,
  • E. Menichetti,
  • E. Migliore,
  • C. Biino,
  • A. Filippi,
  • F. Marchetto,
  • D. Soldi,
  • Y. Mukhamejanov,
  • A. Mukhamejanova,
  • N. Saduyev,
  • S. Sakhiyev,
  • A. Briano Olvera,
  • J. Engelfried,
  • N. Estrada-Tristan,
  • R. Piandani,
  • M. A. Reyes Santos,
  • K. A. Rodriguez Rivera,
  • P. Boboc,
  • A. M. Bragadireanu,
  • S. A. Ghinescu,
  • O. E. Hutanu,
  • T. Blazek,
  • V. Cerny,
  • T. Velas,
  • R. Volpe,
  • J. Bernhard,
  • L. Bician,
  • M. Boretto,
  • F. Brizioli,
  • A. Ceccucci,
  • M. Corvino,
  • H. Danielsson,
  • F. Duval,
  • L. Federici,
  • E. Gamberini,
  • R. Guida,
  • E. B. Holzer,
  • B. Jenninger,
  • Z. Kucerova,
  • G. Lehmann Miotto,
  • P. Lichard,
  • K. Massri,
  • E. Minucci,
  • M. Noy,
  • V. Ryjov,
  • J. Swallow,
  • M. Zamkovsky,
  • X. Chang,
  • A. Kleimenova,
  • R. Marchevski,
  • J. R. Fry,
  • F. Gonnella,
  • E. Goudzovski,
  • J. Henshaw,
  • C. Kenworthy,
  • C. Lazzeroni,
  • C. Parkinson,
  • A. Romano,
  • C. Sam,
  • J. Sanders,
  • A. Sergi,
  • A. Shaikhiev,
  • A. Tomczak,
  • H. Heath,
  • D. Britton,
  • A. Norton,
  • D. Protopopescu,
  • J. B. Dainton,
  • L. Gatignon,
  • R. W. L. Jones,
  • P. Cooper,
  • D. Coward,
  • P. Rubin,
  • A. Baeva,
  • D. Baigarashev,
  • V. Bautin,
  • D. Emelyanov,
  • T. Enik,
  • V. Falaleev,
  • V. Kekelidze,
  • D. Kereibay,
  • A. Korotkova,
  • L. Litov,
  • D. Madigozhin,
  • M. Misheva,
  • N. Molokanova,
  • I. Polenkevich,
  • Yu. Potrebenikov,
  • K. Salamatin,
  • S. Shkarovskiy,
  • S. Fedotov,
  • K. Gorshanov,
  • E. Gushchin,
  • S. Kholodenko,
  • A. Khotyantsev,
  • Y. Kudenko,
  • V. Kurochka,
  • V. Kurshetsov,
  • A. Mefodev,
  • V. Obraztsov,
  • A. Okhotnikov,
  • A. Sadovskiy,
  • V. Sugonyaev,
  • O. Yushchenko

摘要

A measurement of the K + π + ν ν ¯ \( {K}^{+}\to {\pi}^{+}\nu \overline{\nu} \) decay by the NA62 experiment at the CERN SPS is presented, using data collected in 2021 and 2022. This dataset was recorded, after modifications to the beamline and detectors, at a higher instantaneous beam intensity with respect to the 2016–2018 data taking. Combining NA62 data collected in 2016–2022, a measurement of B K + π + ν ν ¯ = 13.0 3.0 + 3.3 × 10 11 \( \mathcal{B}\left({K}^{+}\to {\pi}^{+}\nu \overline{\nu}\right)=\left({13.0}_{-3.0}^{+3.3}\right)\times {10}^{-11} \) is reported. With 51 signal candidates observed and an expected background of 18 2 + 3 \( {18}_{-2}^{+3} \) events, B K + π + ν ν ¯ \( \mathcal{B}\left({K}^{+}\to {\pi}^{+}\nu \overline{\nu}\right) \) becomes the smallest branching ratio measured with a signal significance above 5σ.