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    Perceptual balance, stability, and aesthetic appreciation

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    This repository contains the full datasets and calculated objective measures related to the article "Perceptual balance, stability, and aesthetic appreciation: Their relations depend on the picture type" (Huebner & Fillinger, 2019)
    OSF Preprints

    On the relation between perceived stability and aesthetic appreciation

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    This repository contains the full datasets with calculated objective measures and the stimulus material related to the article "On the relation between perceived stability and aesthetic appreciation"
    OSF Preprints

    Relations between balance, prototypicality, and aesthetic appreciation for Japanese calligraphy

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    OSF Preprints

    Clinical outcome of biomarker-guided therapies in adult patients with tumors of the nervous system

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    Publikationsserver der Universität Tübingen

    Evidence of the P_ccbars(4459)0 in Upsilon(1S, 2S) inclusive decays at Belle

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    International audienceUsing data samples of 102 million Upsilon(1S) events and 158 million Upsilon(2S) events collected by the Belle detector at the KEKB asymmetric-energy e+e−e^+e^- collider, we search for [udsccbar] pentaquark states decaying to Jpsi Lambda. Using the first observations of Upsilon(1S, 2S) inclusive decays to Jpsi Lambda, we find evidence of the P_ccbars(4459)0 state with a significance of 3.3 standard deviations, including statistical and systematic uncertainties. We measure the mass and width of the Pccbars(4459)0 to be (4471.7 +- 4.8 +- 0.6) MeV/c2 and (21.9 +- 13.1 +- 2.7) MeV, respectively. The branching fractions for P_ccbars(4459)0 production are measured to be B[Upsilon(1S) -> P_ccbars(4459)0/ Pbar_ccbars(4459)0 + anything] = (3.5 +- 2.0 +- 0.2)*10-6 and B[Upsilin(2S) -> P_ccbars(4459)0/ Pbar_ccbars(4459)0 +anything] = (2.9 +- 1.7 +- 0.4)*10-6. The inclusive branching fractions of Upsilon(1S, 2S) -> Jpsi Lambda/Lambdabar are measured to be B[Upsilin(1S) -> Jpsi Lambda/Lambdabar + anything] = (36.9 +- 5.3 +- 2.4)*10-6 and B[Upsilon(2S) -> Jpsi Lambda/Lambdabar + anything] = (22.3 +- 5.7 +- 3.1)*10-6. We measure the visible cross section σ(e+e−→J/psiΛ/Λˉ\sigma(e^+e^- \to J/psi \Lambda/\bar\Lambda + anything) = (90 +- 14 +- 6) fb for the continuum production at s=10.52\sqrt{s} = 10.52 GeV. In all cases, the first uncertainties are statistical and the second are systematic
    HAL AMU

    Evidence of the Pccˉs_{c\bar{c}s}(4459)0^0 in Upsilon(1S, 2S) inclusive decays at Belle

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    Using data samples of 102 million Upsilon(1S) events and 158 million Upsilon(2S) events collected by the Belle detector at the KEKB asymmetric-energy e+e−e^+e^- collider, we search for [udsccbar] pentaquark states decaying to Jpsi Lambda. Using the first observations of Upsilon(1S, 2S) inclusive decays to Jpsi Lambda, we find evidence of the Pccsˉ(4459)0P_{cc\bar{s}}(4459)^0 state with a significance of 3.3 standard deviations, including statistical and systematic uncertainties. We measure the mass and width of the Pccsˉ(4459)0P_{cc\bar{s}}(4459)^0 to be (4471.7 +- 4.8 +- 0.6) MeV/c2 and (21.9 +- 13.1 +- 2.7) MeV, respectively. The branching fractions for Pccsˉ(4459)0P_{cc\bar{s}}(4459)^0 production are measured to be B[Upsilon(1S) -> Pccsˉ(4459)0P_{cc\bar{s}}(4459)^0/ Pbar_ccbars(4459)0 + anything] = (3.5 +- 2.0 +- 0.2)*10−6^{-6} and B[Upsilin(2S) -> Pccsˉ(4459)0P_{cc\bar{s}}(4459)^0/ Pbar_ccbars(4459)0 +anything] = (2.9 +- 1.7 +- 0.4)*10−6^{-6}. The inclusive branching fractions of Upsilon(1S, 2S) -> Jpsi Lambda/Lambdabar are measured to be B[Upsilin(1S) -> Jpsi Lambda/Lambdabar + anything] = (36.9 +- 5.3 +- 2.4)*10-6 and B[Upsilon(2S) -> Jpsi Lambda/Lambdabar + anything] = (22.3 +- 5.7 +- 3.1)*10-6. We measure the visible cross section σ(e+e−→J/psiΛ/Λˉ\sigma(e^+e^- \to J/psi \Lambda/\bar\Lambda + anything) = (90 +- 14 +- 6) fb for the continuum production at s=10.52\sqrt{s} = 10.52 GeV. In all cases, the first uncertainties are statistical and the second are systematic
    DESY

    Measurement of the branching fraction and CP\it CP-violating asymmetry of the decay B0→π0π0B^{0} \rightarrow \pi^{0} \pi^{0} using 387387 million bottom-antibottom meson pairs in Belle II data

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    We measure the branching fraction and CP\it CP-violating flavor-dependent rate asymmetry of B0→π0π0B^{0} \to \pi^{0} \pi^{0} decays reconstructed using the Belle II detector in an electron-positron collision sample containing 387×106387 \times 10^{6}BB‾B\overline{B} pairs. Using an optimized event selection, we find 126±20126\pm 20 signal decays in a fit to background-discriminating and flavor-sensitive distributions. The resulting branching fraction is (1.25±0.23)×10−6(1.25 \pm 0.23)\times 10^{-6} and the CP\it CP-violating asymmetry is 0.03±0.300.03 \pm 0.30
    DESY

    Measurement of the branching fractions of B‾ \overline{B} → D(∗)^{(*)}K−K(S)(∗)0^{−} {K}_{(S)}^{\left(\ast \right)0} and B‾ \overline{B} → D(∗)Ds−^{(*)} {D}_s^{-} decays at Belle II

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    We present measurements of the branching fractions of eight B‾0 {\overline{B}}^0 → D(∗)+^{(*)+}K−K(S)(∗)0^{−} {K}_{(S)}^{\left(\ast \right)0} , B−^{−} → D(∗)0^{(*)0}K−K(S)(∗)0^{−} {K}_{(S)}^{\left(\ast \right)0} decay channels. The results are based on data from SuperKEKB electron-positron collisions at the Υ(4S) resonance collected with the Belle II detector, corresponding to an integrated luminosity of 362 fb−1^{−1}. The event yields are extracted from fits to the distributions of the difference between expected and observed B meson energy, and are efficiency-corrected as a function of m(K−K(S)(∗)0^{−} {K}_{(S)}^{\left(\ast \right)0} ) and m(D(∗)K(S)(∗)0^{(*)} {K}_{(S)}^{\left(\ast \right)0} ) in order to avoid dependence on the decay model. These results include the first observation of B‾0 {\overline{B}}^0 → D+^{+}K−KS0^{−} {K}_S^0 , B−^{−} → D*0^{0}K−KS0^{−} {K}_S^0 , and B‾0 {\overline{B}}^0 → D*+^{+}K−KS0^{−} {K}_S^0 decays and a significant improvement in the precision of the other channels compared to previous measurements. The helicity-angle distributions and the invariant mass distributions of the K−K(S)(∗)0^{−} {K}_{(S)}^{\left(\ast \right)0} systems are compatible with quasi-two-body decays via a resonant transition with spin-parity JP^{P} = 1−^{−} for the K−KS0^{−} {K}_S^0 systems and JP^{P} = 1+^{+} for the K−^{−}K*0^{0} systems. We also present measurements of the branching fractions of four B‾0 {\overline{B}}^0 → D(∗)+Ds−^{(*)+} {D}_s^{-} , B−^{−} → D(∗)0Ds−^{(*)0} {D}_s^{-} decay channels with a precision compatible to the current world averages.[graphic not available: see fulltext
    DESY

    Measurement of the branching fractions of Bˉ→D(∗)K−K(S)(∗)0\bar{B}\to D^{(*)} K^- K^{(*)0}_{(S)} and Bˉ→D(∗)Ds−\bar{B}\to D^{(*)}D_s^{-} decays at Belle II

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    International audienceWe present measurements of the branching fractions of eight B‾0→D(∗)+K−K(S)(∗)0\overline B{}^0\to D^{(*)+} K^- K^{(*)0}_{(S)}, B−→D(∗)0K−K(S)(∗)0B^{-}\to D^{(*)0} K^- K^{(*)0}_{(S)} decay channels. The results are based on data from SuperKEKB electron-positron collisions at the Υ(4S)\Upsilon(4S) resonance collected with the Belle II detector, corresponding to an integrated luminosity of 362 fb−1362~\text{fb}^{-1}. The event yields are extracted from fits to the distributions of the difference between expected and observed BB meson energy, and are efficiency-corrected as a function of m(K−K(S)(∗)0)m(K^-K^{(*)0}_{(S)}) and m(D(∗)K(S)(∗)0)m(D^{(*)}K^{(*)0}_{(S)}) in order to avoid dependence on the decay model. These results include the first observation of B‾0→D+K−KS0\overline B{}^0\to D^+K^-K_S^0, B−→D∗0K−KS0B^-\to D^{*0}K^-K_S^0, and B‾0→D∗+K−KS0\overline B{}^0\to D^{*+}K^-K_S^0 decays and a significant improvement in the precision of the other channels compared to previous measurements. The helicity-angle distributions and the invariant mass distributions of the K−K(S)(∗)0K^- K^{(*)0}_{(S)} systems are compatible with quasi-two-body decays via a resonant transition with spin-parity JP=1−J^P=1^- for the K−KS0K^-K_S^0 systems and JP=1+J^P= 1^+ for the K−K∗0K^-K^{*0} systems. We also present measurements of the branching fractions of four B‾0→D(∗)+Ds−\overline B{}^0\to D^{(*)+} D_s^-, B−→D(∗)0Ds−B^{-}\to D^{(*)0} D_s^- decay channels with a precision compatible to the current world averages
    Archives ouvertes de Paris-Saclay
    HAL-IN2P3
    HAL AMU
    DESY
    HAL

    Measurement of the branching fraction and CP\it CP-violating asymmetry of the decay B0→π0π0B^{0} \rightarrow \pi^{0} \pi^{0} using 387387 million bottom-antibottom meson pairs in Belle II data

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    Field of study
    No full text
    We measure the branching fraction and CP\it CP-violating flavor-dependent rate asymmetry of B0→π0π0B^{0} \to \pi^{0} \pi^{0} decays reconstructed using the Belle II detector in an electron-positron collision sample containing 387×106387 \times 10^{6}BB‾B\overline{B} pairs. Using an optimized event selection, we find 126±20126\pm 20 signal decays in a fit to background-discriminating and flavor-sensitive distributions. The resulting branching fraction is (1.25±0.23)×10−6(1.25 \pm 0.23)\times 10^{-6} and the CP\it CP-violating asymmetry is 0.03±0.300.03 \pm 0.30
    DESY
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