225 research outputs found

    Search for B0K0K0B^0 \to K^{*0} \overline{K}{}^{*0}, B0K0K0B^0 \to K^{*0} K^{*0} and B0K+πKπ±B^0 \to K^+\pi^- K^{\mp}\pi^{\pm} Decays

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    We report a search for the decays B0K0K0B^0\to K^{*0} \overline{K}{}^{*0} and B0K0K0B^0\to K^{*0} K^{*0}. We also measure other charmless decay modes with K+πKπ+K^+\pi^-K^-\pi^+ and K+πK+πK^{+}\pi^{-}K^{+}\pi^{-} final states. The results are obtained from a data sample containing 657×106657 \times 10^6 BBB \overline B pairs collected with the Belle detector at the KEKB asymmetric-energy e+ee^+e^- collider. We set upper limits on the branching fractions for B^0\to K^{*0} \kstarbar and B0K0K0B^0\to K^{*0} K^{*0} of 0.81×1060.81 \times 10^{-6} and 0.20×1060.20\times 10^{-6}, respectively, at the 90% confidence level

    First observation of γγppˉK+K\gamma \gamma \to p \bar{p} K^+ K^- and search for exotic baryons in pKpK systems

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    The process γγ→pp¯K+K- and its intermediate processes are measured for the first time using a 980 fb-1 data sample collected with the Belle detector at the KEKB asymmetric-energy e+e- collider. The production of pp¯K+K- and a Λ(1520)0 (Λ¯(1520)0) signal in the pK- (p¯K+) invariant mass spectrum are clearly observed. However, no evidence for an exotic baryon near 1540 MeV/c2, denoted as Θ(1540)0 (Θ¯(1540)0) or Θ(1540)++ (Θ(1540)--), is seen in the pK- (p¯K+) or pK+ (p¯K-) invariant mass spectra. Cross sections for γγ→pp¯K+K-, Λ(1520)0p¯K++c.c. and the products σ(γγ→Θ(1540)0p¯K++c.c.)B(Θ(1540)0→pK-) and σ(γγ→Θ(1540)++p¯K-+c.c.)B(Θ(1540)++→pK+) are measured. We also determine upper limits on the products of the χc0 and χc2 two-photon decay widths and their branching fractions to pp¯K+K- at the 90% credibility level

    Search for CPCP Violation and Measurement of the Branching Fraction in the Decay D0KS0KS0D^{0} \to K^0_S K^0_S

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    We report a study of the decay D0KS0KS0D^0 \to K^0_S K^0_S using 921~fb1^{-1} of data collected at or near the Υ(4S)\Upsilon(4S) and Υ(5S)\Upsilon(5S) resonances with the Belle detector at the KEKB asymmetric-energy e+ee^+e^- collider. The measured time-integrated CP asymmetry is ACP(D0KS0KS0)=(0.02±1.53±0.02±0.17)% A_{CP}(D^0 \to K^0_S K^0_S) = (-0.02 \pm 1.53 \pm 0.02 \pm 0.17) \% and the branching fraction is B(D0KS0KS0)\mathcal{B} (D^{0}\rightarrow K_{S}^{0}K_{S}^{0}) = (1.32 ±\pm 0.02 ±\pm 0.04 ±\pm 0.04) ×\times 104^{-4}, where the first uncertainty is statistical, the second is systematic, and the third is due to the normalization mode (D0KS0π0D^0 \to K_S^0 \pi^0) used in the analysis. These results are significantly more precise than previous measurements for this mode. The ACPA_{CP} measurement is consistent with the Standard Model expectation

    Assessment of the Vibration Influence on Humans in Buildings in the Standards of Different Countries

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    AbstractGround-born vibration produced by different sources can be annoying to nearby building occupants. Analysing the influence of vibration on humans residing in buildings a similar trend is noticeable. After 2003 there have been changes in standards in this area in many countries. There are some trends to connect the regulations for passive and active perception of vibration in standards approach. Seemingly similar regulations specified in standards can be interpreted differently in various countries. This study presents an analysis of such interpretation in the following standards: Polish PN-88/B-02171, British BS 6472-1, Japanese AIJ-GEH-2004, Australian AS 2670.1–2001, American ANSI S3.29-1983, German DIN 4150-2, and ISO international standards ISO 2631-1 and ISO 2631-2. There were analysed in particular parameters for assessing the influence of vibration on humans, the range of considered frequencies, duration of vibration, signal processing and general approach to the problem

    Search for B^{0}→K^{*0}K[over ¯]^{*0}, B^{0}→K^{*0}K^{*0} and B^{0}→K^{+}π^{-}K^{∓}π^{±} decays

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    We report a search for the decays B-0 -> K*(0)(K) over bar*(0) and B-0 -> K*K-0*(0) . We also measure other charmless decay modes with K+ pi K--(-)pi(+) and K+pi K--(+)pi(-) final states. The results are obtained from a data sample containing 657 x 10(6) B (B) over bar pairs collected with the Belle detector at the KEKB asymmetric- energy e(+)e(-) collider. We set upper limits on the branching fractions for B-0 -> K*(0)(K) over bar*(0) and B-0 -> K*K-0*(0) of 0: 81 x 10(-6) and 0.20 x 10(-6), respectively, at the 90% confidence level.LPH

    Measurement of B0DsKS0π+B^0 \to D_s^- K^0_S\pi^+ and B+DsK+K+B^+ \to D_s^- K^+K^+ branching fractions

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    We report a measurement of the B0{B}^{0} and B+{B}^{+} meson decays to the DsKS0π+{D}_{s}^{-}{K}_{S}^{0}{\pi }^{+} and DsK+K+{D}_{s}^{-}{K}^{+}{K}^{+} final states, respectively, using 657×106BB657×1{0}^{6}B\overline{B} pairs collected at the Υ(4S)\mathrm{Υ}\left(4S\right) resonance with the Belle detector at the KEKB asymmetric-energy e+e{e}^{+}{e}^{-} collider. Using the Dsφπ{D}_{s}^{-}\to \varphi {\pi }^{-}, {K}^{*}\left(892{\right)}^{0}{K}^{-} and KS0K{K}_{S}^{0}{K}^{-} decay modes for the Ds{D}_{s} reconstruction, we measure the following branching fractions: B(B0DsKS0π+)=[0.47±0.06(stat)±0.05(syst)]×104\mathcal{B}\left({B}^{0}\to {D}_{s}^{-}{K}_{S}^{0}{\pi }^{+}\right)=\left[0.47±0.06\left(\text{stat}\right)±0.05\left(\text{syst}\right)\right]×1{0}^{-4} and B(B+DsK+K+)=[0.93±0.22(stat)±0.10(syst)]×105\mathcal{B}\left({B}^{+}\to {D}_{s}^{-}{K}^{+}{K}^{+}\right)=\left[0.93±0.22\left(\text{stat}\right)±0.10\left(\text{syst}\right)\right]×1{0}^{-5}. We find the ratio of the branching fraction of B+DsK+K+{B}^{+}\to {D}_{s}^{-}{K}^{+}{K}^{+} to that of the analogous Cabibbo-favored B+DsK+π+{B}^{+}\to {D}_{s}^{-}{K}^{+}{\pi }^{+} decay to be RB=0.054±0.013(stat)±0.006(syst){\mathcal{R}}_{\mathcal{B}}=0.054±0.013\left(\text{stat}\right)±0.006\left(\text{syst}\right), which is consistent with the naive factorization model. We also observe a deviation of the DsK{D}_{s}K invariant-mass distribution from the three-body phase-space model for both studied decays

    Proper Names in Polish Proverbs

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    U članku se određuju značenjske sastavnice u definiranju poslovica te se klasificiraju poslovice s algoremom vlastitih imena prema korpusu iz poljsko-ruskog rječnika poslovica što ga je sastavio Ryszard Stypula. Prema značenjskom kriteriju poslovice s algoremom vlastitog imena podijeljene su u tri grupe: 1) antroponimne poslovice (imena i prezimena); 2) etnonimne poslovice (nazivi naroda i rasa); 3) toponimne poslovice (nazivi gradova). Svaka poslovica analizirana je s obzirom na njeno opće značenje i uspoređivana s hrvatskim ekvivalentima. U zaključku se pokazuje da se poslovice mogu promatrati kao etnolingvističke jedinice govora. Poslovice s algoremom vlastitih imena pokazuju u doslovnom značenju poljski kulturni krug koji se vidi u poljskim imenima ljudi, naroda i gradova, a u prenesenom značenju ta vlastita imena označuju omnipersonalnost koja je u obliku "svak, svaki čovjek" prisutnija u hrvatskim ekvivalentima.The paper deals with the elements of meaning in defining proverbs, as well as with the classifica¬tion of proverbs containing a proper name. The author uses the proverbs from the Polish-Russian Dictionary of Proverbs compiled by Ryszard Stypula. The proverbs containing a proper name are classified according to the criterium of meaning into three groups: (1) anthroponymic proverbs (first and family names); (2) ethnonymic proverbs (names of nations and races) and (3) toponymic proverbs (names of places). Each proverb has been analysed in accordance with its general meaning and in comparison with its Croatian counterpart. The concluding part of the paper shows that proverbs can be observed as ethnolinguistic units of speech. The proverbs containing a proper name show — in their denotative meaning — Polish cul¬tural environment which can be observed through the Polish names of people, nations and places, and —in their connotative meaning—these proper names show the omnipersonality which is also present in their Croatian counterparts in the form "everyone; everybody"

    Study of charmless decays B±KS0KS0h±B^{\pm} \to K^{0}_{S} K^{0}_{S} h^{\pm} (h=K,πh=K,\pi) at Belle

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    International audienceWe report a search for charmless hadronic decays of charged BB mesons to the final states KS0KS0K±K^{0}_{S} K^{0}_{S} K^{\pm} and KS0KS0π±K^{0}_{S} K^{0}_{S} \pi^{\pm} . The results are based on a 711fb1711 {fb}^{-1} data sample that contains 772×106772 \times 10^6 BBˉB \bar{B} pairs, and was collected at the Υ(4S)\Upsilon(4S) resonance with the Belle detector at the KEKB asymmetric-energy e+ee^{+}e^{-} collider. For B±KS0KS0K±B^{\pm} \to K^{0}_{S} K^{0}_{S} K^{\pm} decays, the measured branching fraction and direct CPCP asymmetry are [10.64±0.49(stat)±0.44(syst)]×106[10.64\pm0.49(stat)\pm 0.44(syst)]\times10^{-6} and [0.6±3.9(stat)±3.4(syst)-0.6\pm3.9(stat)\pm 3.4(syst)] %, respectively. In the absence of a statistically significant signal for B±KS0KS0π±B^{\pm}\to K^{0}_{S} K^{0}_{S} \pi^{\pm}, we set the 90 % confidence-level upper limit on its branching fraction at 1.14×1061.14 \times 10^{-6}
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