447 research outputs found

    Penguin decays of B mesons

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    Penguin, or loop, decays of B mesons induce effective flavor-changing neutral currents, which are forbidden at tree level in the Standard Model. These decays give special insight into the CKM matrix and are sensitive to non-standard model effects. In this review, we give a historical and theoretical introduction to penguins and a description of the various types of penguin processes: electromagnetic, electroweak, and gluonic. We review the experimental searches for penguin decays, including the measurements of the electromagnetic penguins b -> s gamma and B -> K* gamma and gluonic penguins B -> K pi, B+ -> omega K+ and B -> eta' K, and their implications for the Standard Model and New Physics. We conclude by exploring the future prospects for penguin physics.Comment: 49 pages, LATEX, 30 embedded figures, submitted to Annual Reviews of Nuclear and Particle Scienc

    Der Einfluss des metakognitiven Wissens auf die Entwicklung der Mathematikleistung am Beginn der Sekundarstufe I

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    Metakognitives Wissen, also das Wissen über kognitive Prozesse und ihre Steuerung, ist in der Gedächtnis- und Leseverstehensforschung in einem breiten Altersbereich vom Kindergartenalter bis zum Ende der Sekundarstufe I als wichtiger Prädiktor kognitiver Leistungen etabliert. Im Inhaltsbereich Mathematik deuten punktuelle Befunde zu korrelativen Zusammenhängen sowie die Wirknachweise metakognitiver Trainingsprogramme auf leistungsrelevante Effekte des metakognitiven Wissens hin. Jedoch fehlt nach wie vor systematische Forschung zum Zusammenhang zwischen metakognitivem Wissen über Planung, Überwachung und Regulation mathematischer Lösungsprozesse und der Entwicklung in curricularen mathematischen Kompetenzen. Diese Fragestellung wurde anhand von drei Forschungsfragen in der Sekundarstufe I untersucht: (a) Unterscheiden sich die Schüler der drei Schularten zu Beginn der fünften Jahrgangsstufe im metakognitiven Wissen? (b) Kann das metakognitive Wissen die Mathematikleistung zu einem späteren Zeitpunkt vorhersagen? (c) Trägt das metakognitive Wissen einen eigenen Anteil zur Vorhersage der Mathematikleistung bei, der über den Einfluss anderer allgemeiner und mathematikspezifischer Leistungsdeterminanten hinaus geht? Die Analysen basieren auf der längsschnittlichen Untersuchung einer Stichprobe von 763 nordbayerischen Schülerinnen und Schülern aus Gymnasien, Realschulen und Hauptschulen. Neben der Mathematikleistung am Beginn und am Ende der fünften Jahrgangsstufe und dem metakognitiven Wissen wurden als Prädiktoren mathematischer Leistungen allgemeine (Intelligenz und soziale Herkunft) sowie mathematikspezifische Schülermerkmale (Rechenfertigkeiten, mathematisches Selbstkonzept und mathematisches Interesse) erhoben. Die Auswertungen erbrachten bedeutsame Schulartunterschiede im metakognitiven Wissen. Das metakognitive Wissen leistet darüber hinaus auch unter Kontrolle der Vorwissensunterschiede und weiterer allgemeiner und spezifischer Leistungsdeterminanten einen bedeutsamen Beitrag in der Vorhersage der Mathematikleistung am Ende der fünften Jahrgangsstufe. Diese Befunde werden als Nachweis für die substanzielle Bedeutung des metakognitiven Wissens für Ausprägung und Entwicklung mathematischer Kompetenzen am Beginn der Sekundarstufe I interpretiert.Metacognitive knowledge, that is the knowledge about cognitive processes and their regulation is established in memory and reading comprehension research as an important predictor of cognitive achievement. ln mathematics some correlational findings and the effects of metacognitive trainings point to the predictive account of metacognitive knowledge in the prediction of achievement. However, there is no systematic research on the relations between metacognitive knowledge on planning, monitoring and regulation processes in the solution of mathematical problems and the development of curricular mathematical achievement. To explore the relation between metacognitive knowledge and achievement in secondary school three research questions were examined: (a) Are there differences in metacognitive knowledge between the students allocated to the three tracks of German educational system? (b) Does metacognitive knowledge predict mathematics achievement? (c) Does metacognitive knowledge show a unique predictive influence even when other general and specific predictors of mathematics achievement are controlled? Two measurement points at the beginning and at the end of Grade 5 were analyzed. The sample consisted of N=763 students from northern Bavaria on three tracks (academic track, intermediate track and vocational track). Mathematics achievement was assessed at both measurement points. Metacognitive knowledge as well as general (intelligence, socio-economic status) and specific (computation skills, mathematical self-concept and mathematical interest) predictors of achievement were assessed at the first measurement point. Students attending the three tracks differed in metacognitive knowledge. Additionally, metacognitive knowledge predicted mathematics achievement at T2. This predictive influence remained significant even under control for prior knowledge as well as general and the specific determinants of mathematics achievement. The findings show the substantial importance of metacognitive knowledge on mathematics achievement and on development of mathematics achievement at the beginning of secondary school

    Rare radiative B decays to orbitally excited K mesons

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    The exclusive rare radiative B meson decays to orbitally excited axial-vector mesons K_1^*(1270), K_1(1400) and to the tensor meson K_2^*(1430) are investigated in the framework of the relativistic quark model based on the quasipotential approach in quantum field theory. These decays are considered without employing the heavy quark expansion for the s quark. Instead the s quark is treated to be light and the expansion in inverse powers of the large recoil momentum of the final K^{**} meson is used to simplify calculations. It is found that the ratio of the branching fractions of rare radiative B decays to axial vector K^*_1(1270) and K_1(1400) mesons is significantly influenced by relativistic effects. The obtained results for B decays to the tensor meson K_2^*(1430) agree with recent experimental data from CLEO.Comment: 17 pages, revte

    The sensitivity of the zero position of the forward--backward asymmetry to new physics effects in the B -> K^\ast \mu^+ \mu^- decay

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    Starting with the most general effective Hamiltonian comprising scalar and vector operators beyond the standard model, we discuss the impact of various operators on the zero of the forward--backward asymmetry in the dileptonic B decay B -> K^\ast \mu^+ \mu^-. We find that, zero of the asymmetry is highly sensitive to the sign and size of the vector--vector operators and opposite chirality counterparts of the usual operators. The scalar--scalar four--fermion operators, on the other hand, have mild effect on the zero of the asymmetry. Our results are expected to be checked in the near future experiments.Comment: 16 pp, 6 ps fig

    Observation of the Dynamic Beta Effect at CESR with CLEO

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    Using the silicon strip detector of the CLEO experiment operating at the Cornell Electron-positron Storage Ring (CESR), we have observed that the horizontal size of the luminous region decreases in the presence of the beam-beam interaction from what is expected without the beam-beam interaction. The dependence on the bunch current agrees with the prediction of the dynamic beta effect. This is the first direct observation of the effect.Comment: 9 page uuencoded postscript file, postscritp file also available through http://w4.lns.cornell.edu/public/CLNS, submitted to Phys. Rev.

    Measurement of the Inclusive Semi-electronic D0D^0 Branching Fraction

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    Using the angular correlation between the π+\pi^+ emitted in a D+D0π+D^{*+} \rightarrow D^0 \pi^+ decay and the e+e^+ emitted in the subsequent D0Xe+νD^0 \rightarrow Xe^+\nu decay, we have measured the branching fraction for the inclusive semi-electronic decay of the D0D^0 meson to be: {\cal B}(D^0 \rightarrow X e^+ \nu) = [6.64 \pm 0.18 (stat.) \pm 0.29 (syst.)] \%. The result is based on 1.7 fb1^{-1} of e+ee^+e^- collisions recorded by the CLEO II detector located at the Cornell Electron Storage Ring (CESR). Combining the analysis presented in this paper with previous CLEO results we find, \frac{{\cal B} (D^0 \rightarrow X e^+ \nu)} {{\cal B} (D^0 \rightarrow K^- \pi^+)} = 1.684 \pm 0.056 (stat.) \pm 0.093(syst.) and \frac{{\cal B}(D\rightarrow K^-e^+\nu)} {{\cal B}(D\rightarrow Xe^+\nu)} = 0.581 \pm 0.023 (stat.) \pm 0.028(syst.). The difference between the inclusive rate and the sum of the measured exclusive branching fractions (measured at CLEO and other experiments) is (3.3±7.2)%(3.3 \pm 7.2) \% of the inclusive rate.Comment: Latex file, 33pages, 4 figures Submitted to PR

    Precision Measurement of the Ds+Ds+D_s^{*+}- D_s^+ Mass Difference

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    We have measured the vector-pseudoscalar mass splitting M(Ds+)M(Ds+)=144.22±0.47±0.37MeVM(D_s^{*+})-M(D_s^+) = 144.22\pm 0.47\pm 0.37 MeV, significantly more precise than the previous world average. We minimize the systematic errors by also measuring the vector-pseudoscalar mass difference M(D0)M(D0)M(D^{*0})-M(D^0) using the radiative decay D0D0γD^{*0}\rightarrow D^0\gamma, obtaining [M(Ds+)M(Ds+)][M(D0)M(D0)]=2.09±0.47±0.37MeV[M(D_s^{*+})-M(D_s^+)]-[M(D^{*0})-M(D^0)] = 2.09\pm 0.47\pm 0.37 MeV. This is then combined with our previous high-precision measurement of M(D0)M(D0)M(D^{*0})-M(D^0), which used the decay D0D0π0D^{*0}\rightarrow D^0\pi^0. We also measure the mass difference M(Ds+)M(D+)=99.5±0.6±0.3M(D_s^+)-M(D^+)=99.5\pm 0.6\pm 0.3 MeV, using the ϕπ+\phi\pi^+ decay modes of the Ds+D_s^+ and D+D^+ mesons.Comment: 18 pages uuencoded compressed postscript (process with uudecode then gunzip). hardcopies with figures can be obtained by sending mail to: [email protected]

    Further Search for the Two-Photon Production of the Glueball Candidate fJ(2220)f_{J}(2220)

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    The CLEOII detector at the Cornell e+ e- storage ring CESR has been used to search for the two-photon production of the fJ(2220)f_J(2220) decaying into pi+ pi-. No evidence for a signal is found in data corresponding to an integrated luminosity of 4.77/fb and a 95% CL upper limit on ΓtwophotonBRpi+pi\Gamma_{two-photon} * BR{pi+ pi-} of 2.5 eV is set. If this result is combined with the BES Collaboration's measurement of fJ(2220)>pi+pif_J(2220) -> pi+ pi- in radiative J/ψJ/\psi decay, a 95% CL lower limit on the stickiness of the fJ(2220)f_J(2220) of 73 is obtained. If the recent CLEO result for \Gamma_{two-photon} * BR{\K_S K_S} is combined with the present result, the stickiness of the fJ(2220)f_J(2220) is found to be larger than 102 at the 95% CL. These results for the stickiness (the ratio of the probabilities for two-gluon coupling and two-photon coupling) provide further support for a substantial neutral parton content in the fJ(2220)f_J(2220).Comment: 8 pages, postscript file also available through http://w4.lns.cornell.edu/public/CLN

    Measurements of the Ratios B(Ds+η+ν)/B(Ds+ϕ+ν){\cal B}(D_s^+\to \eta\ell^+\nu)/{\cal B}(D_s^+\to \phi\ell^+\nu) and B(Ds+η+ν)/B(Ds+ϕ+ν){\cal B}(D_s^+\to \eta'\ell^+\nu)/{\cal B}(D_s^+\to \phi\ell^+\nu)

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    Using the CLEO~II detector we measure B(Ds+ηe+ν)/B(Ds+ϕe+ν)=1.24±0.12±0.15{\cal B}(D_s^+\to \eta e^+\nu)/{\cal B}(D_s^+\to \phi e^+\nu) =1.24\pm0.12\pm0.15, B(Ds+ηe+ν)/B(Ds+ϕe+ν)=0.43±0.11±0.07{\cal B}(D_s^+\to \eta' e^+\nu)/{\cal B}(D_s^+\to \phi e^+\nu) =0.43\pm0.11\pm0.07 and B(Ds+ηe+ν)/B(Ds+ηe+ν)=0.35±0.09±0.07{\cal B}(D_s^+\to \eta' e^+\nu)/{\cal B}(D_s^+\to \eta e^+\nu) =0.35\pm0.09\pm0.07. We find the vector to pseudoscalar ratio, B(Ds+ϕe+ν)/B(Ds+(η+η)e+ν)=0.60±0.06±0.06{\cal B}(D_s^+\to \phi e^+\nu)/{\cal B}(D_s^+\to (\eta+\eta') e^+\nu) =0.60\pm0.06\pm0.06, which is similar to the ratio found in non strange DD decays.Comment: 11 page uuencoded postscript file, postscript file also available through http://w4.lns.cornell.edu/public/CLN
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