1,738,824 research outputs found

    Observation of the rare decay B+ -> K+π0π0 and measurement of the quasi-two-body contributions B+ -> K*(892)+π0, B+ -> f0(980)K+, and B+ -> χc0K+

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    We report an analysis of charmless hadronic decays of charged B mesons to the final state K(+) pi(0)pi(0), using a data sample of (470.9 +/- 2.8) x 10(6) B (B) over bar events collected with the BABAR detector at the Y(4S) resonance. We observe an excess of signal events, with a significance above 10 standard deviations including systematic uncertainties, and measure the branching fraction and CP asymmetry to be B(B(+) -> K(+) pi(0)pi(0)) = (16.2 +/- 1.2 +/- 1.5) x 10(-6) and A(CP)(B(+) -> K(+) pi(0)pi(0)) = -0.06 +/- 0.06 +/- 0.04, where the uncertainties are statistical and systematic, respectively. Additionally, we study the contributions of the B(+) -> K*(892)(+) pi(0), B(+) -> f(0)(980)K(+), and B(+) -> chi(c0)K(+) quasi-two-body decays. We report the world's best measurements of the branching fraction and CP asymmetry of the B(+) -> K(+) pi(0)pi(0) and B(+) -> K(+)(892)(+) pi(0) channels

    Grammar [892]

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    Grammar. This manuscript is now IO Islamic 293 in the India Office collections. [metadata: Otto Loth, A Catalogue of the Arabic Manuscripts in the Library of the India Office, (volume 1), no. 892 here with further notations and hyperlinks]. 892. 293. Size 83/4 in. by 43/4 in.; foll. 280. Eleven lines in a page. Another copy of the same Commentary, plainly written, by Muḥammad Ja׳far, A.H. 1189. Seal of Khân Jahân. [Tippu.

    gD(s)*DK*(892) and gB(s)*BK*(892) coupling constants in QCD sum rules

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    The coupling constants gD*(s) DK*(892) and gB*sBK*(892) are calculated in the framework of three-point QCD sum rules. The correlation functions responsible for these coupling constants are evaluated considering contributions of both D(B) and K*(892) mesons as off-shell states, but in the absence of radiative corrections. The results gD*sDK*(892) = (3.74 +/- 1.38) GeV-1 and gB*sBK*(892) = (3.24 +/- 1.08) GeV-1 are obtained for the considered strong coupling constants

    Measurement of K^{*}(892)±^{\mathrm{\pm}} production in inelastic pp collisions at the LHC

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    The first results on K⁎(892)± resonance production in inelastic pp collisions at LHC energies of s=5.02, 8, and 13 TeV are presented. The K⁎(892)± has been reconstructed via its hadronic decay channel K⁎(892)→±KS0+π± with the ALICE detector. Measurements of transverse momentum distributions, pT-integrated yields, and mean transverse momenta for charged K⁎(892) are found to be consistent with previous ALICE measurements for neutral K⁎(892) within uncertainties. For pT&gt;1 GeV/c the K⁎(892)± transverse momentum spectra become harder with increasing centre-of-mass energy from 5.02 to 13 TeV, similar to what previously observed for charged kaons and pions. For pT&lt;1 GeV/c the K⁎(892)± yield does not evolve significantly and the abundance of K⁎(892)± relative to K is rather independent of the collision energy. The transverse momentum spectra, measured for K⁎(892)± at midrapidity in the interval 0 &lt;pT&lt;15 GeV/c, are not well described by predictions of different versions of PYTHIA 6, PYTHIA 8 and EPOS-LHC event generators. These generators reproduce the measured pT-integrated K⁎±/K ratios and describe well the momentum dependence for pT&lt;2 GeV/c.The first results on K^{*}(892)±^{\mathrm{\pm}} resonance production in inelastic pp collisions at LHC energies of s=5.02\sqrt{s} = 5.02, 8, and 13 TeV are presented. The K^{*}(892)±^{\mathrm{\pm}} has been reconstructed via its hadronic decay channel K^{*}(892)±^{\mathrm{\pm}}\rightarrowKS0\mathrm {K^0_S} + π±~+~\pi^{\pm} with the ALICE detector. Measurements of transverse momentum distributions, pTp_{\mathrm{T}}-integrated yields, and mean transverse momenta for charged K^{*}(892) are found to be consistent with previous ALICE measurements for neutral K^{*}(892) within uncertainties. For pT>1p_{\mathrm{T}} > 1 GeV/cc the K^{*}(892)±^{\mathrm{\pm}} transverse momentum spectra become harder with increasing centre-of-mass energy from 5.02 to 13 TeV, similar to what previously observed for charged kaons and pions. For pT<1p_{\mathrm{T}} < 1 GeV/cc the K^{*}(892)±^{\mathrm{\pm}} yield does not evolve significantly and the abundance of K^{*}(892)±^{\mathrm{\pm}} relative to K is rather independent of the collision energy. The transverse momentum spectra, measured for K^{*}(892)±^{\mathrm{\pm}} at midrapidity in the interval 0<pT<150 < p_{\mathrm{T}} < 15 GeV/cc, are not well described by predictions of different versions of PYTHIA 6, PYTHIA 8 and EPOS-LHC event generators. These generators reproduce the measured pTp_{\mathrm{T}}-integrated K±^{*\mathrm{\pm}}/K ratios and describe well the momentum dependence for pT<2p_{\mathrm{T}} < 2 GeV/cc

    Going Beyond Counting First Authors in Author Co-citation Analysis

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    The present study examines one of the fundamental aspects of author co-citation analysis (ACA) - the way co-citation counts are defined. Co-citation counting provides the data on which all subsequent statistical analyses and mappings are based, and we compare ACA results based on two different types of co-citation counting - the traditional type that only counts the first one among a cited work's authors on the one hand and a non-traditional type that takes into account the first 5 authors of a cited work on the other hand. Results indicate that the picture produced through this non-traditional author co-citation counting contains more coherent author groups and is therefore considerably clearer. However, this picture represents fewer specialties in the research field being studied than that produced through the traditional first-author co-citation counting when the same number of top-ranked authors is selected and analyzed. Reasons for these effects are discussed

    RAAPNOTITIE 892

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    onderzoeksrappor

    RAAPRAPPORT 892

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    Mandurama photograph collection [892] [picture] /

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    Also available in an electronic version via the Internet at: http://nla.gov.au/nla.pic-an8526486-892

    ADC 892

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