Messung der Lebensdauer des Ξ0\Xi^{0} -Hyperons mit dem NA48-Detektor

One of the main characteristics of particles is the lifetime. The mean lifetime of the Xi0 hyperon, which can be determined theoretically from the Xi- lifetime by using the Delta I=1/2 rule, has been measured a couple of times. The most recent measurement from 1977 has a relative uncertainty of 5%, which could be improved by usind data from new experiments like NA48/1. The Xi0 lifetime is an important input parameter in the determination of the matrix element Vus of the Cabibbo-Kobayashi-Maskawa matrix in semileptonic Xi0 decays. In 2002 a high intensity data acquisition was performed by the NA48/1 collaboration, in which about 10^9 Xi0 decay candidates were recorded. From this sample 192000 events of the decay "Xi0 to Lambda pi0" were reconstructed and a subsample of 107000 could be used to determine the lifetime. The lifetime was determined by comparison of measured and simulated data in ten energy bins to avoid systematic effects. The result has a higher precision than older measurements. It differs from the world average (tau=(2.90+-0.09)*10^(-10)s) by (+4.99+-0.50(stat)+-0.58(syst))% corresponding to 1.7 standard deviations. The lifetime is tau=(3.045+-0.015(stat)+-0.017(syst))*10^(-10)s. The lifetime of the Anti-Xi0 could be measured using the same data sample. The result is tau=(3.042+-0.045(stat)+-0.017(syst))*10^(-10)s

Messung der Lebensdauer des 0 -Hyperons mit dem NA48-Detektor

Zu den Hauptcharakteristika von Teilchen gehoert - neben der Masse - die Lebensdauer. Die mittlere Lebensdauer des Xi0-Hyperons, die sich aus der mittleren Lebensdauer des Xi--Hyperons ueber die Delta I=1/2-Regel theoretisch voraussagen laesst, wurde bereits mehrfach experimentell bestimmt. Die neueste Messung aus dem Jahr 1977 besitzt jedoch eine relative Unsicherheit von 5%, was sich mit Daten neuerer Experimente deutlich verbessern laesst. Die mittlere Lebensdauer ist ein wichtiger Parameter bei der Bestimmung des Matrixelements Vus der Cabibbo-Kobayashi-Maskawa-Matrix in semileptonischen Xi0-Zerfaellen. Im Jahre 2002 wurde mit dem NA48-Detektor eine Datennahme mit hoher Intensitaet durchgefuehrt, bei der unter anderem etwa 10^9 Xi0-Zerfallskandidaten aufgezeichnet wurden. Davon wurden im Rahmen dieser Arbeit 192000 Ereignisse des Typs "Xi0 nach Lambda pi0" rekonstruiert und 107000 Ereignisse zur Bestimmung der mittleren Lebensdauer durch Vergleich mit simulierten Ereignissen verwendet. Zur Vermeidung von systematischen Fehlern wurde die Lebensdauer in zehn Energieintervallen durch Vergleich von gemessenen und simulierten Daten ermittelt. Das Ergebnis ist wesentlich genauer als bisherige Messungen und weicht vom Literaturwert (tau=(2,90+-0,09)*10^(-10)s) um (+4,99+-0,50(stat)+-0,58(syst))% ab, was 1,7 Standardabweichungen entspricht. Die Lebensdauer ergibt sich zu tau=(3,045+-0,015(stat)+-0,017(syst))*10^(-10)s. Auf die gleiche Weise konnte mit den zur Verfuegung stehenden Daten erstmals die Lebensdauer des Anti-Xi0-Hyperons gemessen werden. Das Ergebnis dieser Messung ist tau=(3,042+-0,045(stat)+-0,017(syst))*10^(-10)s.One of the main characteristics of particles is the lifetime. The mean lifetime of the Xi0 hyperon, which can be determined theoretically from the Xi- lifetime by using the Delta I=1/2 rule, has been measured a couple of times. The most recent measurement from 1977 has a relative uncertainty of 5%, which could be improved by usind data from new experiments like NA48/1. The Xi0 lifetime is an important input parameter in the determination of the matrix element Vus of the Cabibbo-Kobayashi-Maskawa matrix in semileptonic Xi0 decays. In 2002 a high intensity data acquisition was performed by the NA48/1 collaboration, in which about 10^9 Xi0 decay candidates were recorded. From this sample 192000 events of the decay "Xi0 to Lambda pi0" were reconstructed and a subsample of 107000 could be used to determine the lifetime. The lifetime was determined by comparison of measured and simulated data in ten energy bins to avoid systematic effects. The result has a higher precision than older measurements. It differs from the world average (tau=(2.90+-0.09)*10^(-10)s) by (+4.99+-0.50(stat)+-0.58(syst))% corresponding to 1.7 standard deviations. The lifetime is tau=(3.045+-0.015(stat)+-0.017(syst))*10^(-10)s. The lifetime of the Anti-Xi0 could be measured using the same data sample. The result is tau=(3.042+-0.045(stat)+-0.017(syst))*10^(-10)s

Measurement of the form factors of charged kaon semileptonic decays

International audienceA measurement of the form factors of charged kaon semileptonic decays is presented, based on 4.4 × 10$^{6}$K$^{±}$ → π$^{0}$e$^{±}$ν$_{e}$ (K$_{e3}^{±}$ ) and 2.3 × 10$^{6}$K$^{±}$ → π$^{0}$μ±ν$_{μ}$ (K$_{μ3}^{±}$ ) decays collected in 2004 by the NA48/2 experiment. The results are obtained with improved precision as compared to earlier measurements. The combination of measurements in the K$_{e3}^{±}$ and K$_{μ3}^{±}$ modes is also presented

First observation and study of the K±→π0π0μ±νK^{\pm} \rightarrow \pi^{0} \pi^{0} \mu^{\pm} \nu decay

International audienceThe NA48/2 experiment at CERN reports the first observation of the K$^{±}$ → π$^{0}$π$^{0}$μ$^{±}$ν decay based on a sample of 2437 candidates with 15% background contamination collected in 2003–2004. The decay branching ratio in the kinematic region of the squared dilepton mass above 0.03 GeV$^{2}$/c$^{4}$ is measured to be (0.65 ± 0.03) × 10$^{−6}$. The extrapolation to the full kinematic space, using a specific model, is found to be (3.45 ± 0.16) × 10$^{−6}$, in agreement with chiral perturbation theory predictions