369 research outputs found

    Linking variation in planktonic primary production to coral reef fish growth and condition

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    Within low-nutrient tropical oceans, islands and atolls with higher primary production support higher fish biomass and reef organism abundance. External energy subsidies can be delivered onto reefs via a range of physical mechanisms. However, the influence of spatial variation in primary production on reef fish growth and condition is largely unknown. It is not yet dear how energy subsidies interact with reef depth and slope. Here we test the hypothesis that with increased proximity to deep-water oceanic nutrient sources, or at sites with shallower reef slopes, parameters of fish growth and condition will be higher. Contrary to expectations, we found no association between fish growth rate and sites with higher mean chlorophyll-a values. There were no differences in fish delta N-15 or delta C-13 values between depths. The relationship between fish condition and primary production was influenced by depth, driven by increased fish condition at shallow depths within a primary production 'hotspot' site. Carbon delta C-13 was depleted with increasing primary production, and interacted with reef slope. Our results indicate that variable primary production did not influence growth rates in planktivorous Chromis fieldi within 10-17.5 m depth, but show site-specific variation in reef physical characteristics influencing fish carbon isotopic composition

    Spatial quantification of dynamic inter and intra particle crystallographic heterogeneities within lithium ion electrodes

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    The performance of lithium ion electrodes is hindered by unfavorable chemical heterogeneities that pre-exist or develop during operation. Time-resolved spatial descriptions are needed to understand the link between such heterogeneities and a cell’s performance. Here, operando high-resolution X-ray diffraction-computed tomography is used to spatially and temporally quantify crystallographic heterogeneities within and between particles throughout both fresh and degraded Li_{x}Mn_{2)O_{4} electrodes. This imaging technique facilitates identification of stoichiometric differences between particles and stoichiometric gradients and phase heterogeneities within particles. Through radial quantification of phase fractions, the response of distinct particles to lithiation is found to vary; most particles contain localized regions that transition to rock salt LiMnO_{2} within the first cycle. Other particles contain monoclinic Li_{2}MnO_{3}near the surface and almost pure spinel Li_{x}Mn_{2}O_{4} near the core. Following 150 cycles, concentrations of LiMnO_{2} and Li_{2}MnO_{3} significantly increase and widely vary between particles

    High speed 4D neutron computed tomography for quantifying water dynamics in polymer electrolyte fuel cells

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    In recent years, low temperature polymer electrolyte fuel cells have become an increasingly important pillar in a zero carbon strategy for curbing climate change, with their potential to power multiscale stationary and mobile applications. The performance improvement is a particular focus of research and engineering roadmaps, with water management being one of the major areas of interest for development. Appropriate characterisation tools for mapping the evolution, motion and removal of water are of high importance to tackle shortcomings. This article demonstrates the development of a 4D high speed neutron imaging technique, which enables a quantitative analysis of the local water evolution. 4D visualisation allows the time resolved studies of droplet formation in the flow fields and water quantification in various cell parts. Performance parameters for water management are identified that offer a method of cell classification, which will, in turn, support computer modelling and the engineering of next generation flow field design

    Observation of B+- -> omega K+- Decay

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    We report the first observation of the charmless two-body mode B±ωK±B^{\pm} \to \omega K^{\pm} decay, and a new measurement of the branching fraction for the B±ωπ±B^{\pm} \to \omega \pi^{\pm} decay. The measured branching fractions are B(B±ωK±)=(9.22.3+2.6±1.0)×106{\cal B} (B^{\pm} \to \omega K^{\pm}) = (9.2{}^{+2.6}_{-2.3}\pm 1.0) \times 10^{-6} and B(B±ωπ±)=(4.21.8+2.0±0.5)×106{\cal B} (B^{\pm} \to \omega \pi^{\pm}) = (4.2{}^{+2.0}_{-1.8}\pm 0.5) \times 10^{-6}. %and we set 90% confidence level upper limits of %B(Bωπ)<8.1×106{\cal B} (B^- \to \omega \pi^-) < 8.1\times 10^{-6}. We also measure the partial rate asymmetry of B±ωK±B^{\pm}\to\omega K^{\pm} decays and obtain ACP=0.21±0.28±0.03{\cal A}_{CP} = -0.21 \pm 0.28 \pm 0.03. The results are based on a data sample of 29.4 fb1^{-1} collected on the Υ(4S)\Upsilon(4S) resonance by the Belle detector at the KEKB e+ee^{+} e^{-} collider.Comment: 5 pages, 4 figures, resubmitted to Phys. Rev. Let

    Mesurement of the B0 - anti-B0 Mixing Parameter Delta m_d using Semileptonic B0 Decays

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    We present a measurement of the B^0-B^0bar mixing parameter Delta m_d using neutral B meson pairs in a 29.1 fb^{-1} data sample collected at the Upsilon(4S) resonance with the Belle detector at the KEKB asymmetric-energy e^+e^- collider. We exclusively reconstruct one neutral B meson in the semileptonic B^0 \to D^{*-}\ell^+\nu decay mode and identify the flavor of the accompanying B meson from its decay products. From the distribution of the time intervals between the two flavor-tagged B meson decay points, we obtain Delta m_d = (0.494 +- 0.012 +- 0.015) ps^{-1}, where the first error is statistical and the second error is systematic.Comment: 10 pages, 3 figures, Published in Phys.Rev.Lett. 89, 251803 (2002

    Measurement of the B0Bˉ0B^0 -\bar{B}^0 mixing rate with B0(Bˉ0)Dπ±B^0(\bar{B}^0) \to D^{*\mp} \pi^{\pm} partial reconstruction

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    We report a measurement of the B0Bˉ0B^0-\bar{B}^0 mixing parameter Δmd\Delta m_d based on a 29.1 fb1\rm 29.1~fb^{-1} sample of Υ(4S)\Upsilon (4S) resonance decays collected by the Belle detector at the KEKB asymmetric e+ee^+ e^- collider. We use events with a partially reconstructed B0(Bˉ0)Dπ±B^0(\bar{B}^0) \to D^{*\mp} \pi^{\pm} candidate and where the flavor of the accompanying BB meson is identified by the charge of the lepton from a B0(Bˉ0)X±νB^0(\bar{B}^0) \to X^{\mp} \ell^{\pm} \nu decay. The proper-time difference between the two BB mesons is determined from the distance between the two decay vertices. From a simultaneous fit to the proper-time distributions for the same-flavor (B0(Bˉ0)B^0(\bar{B}^0), ±\ell^{\pm}) and opposite-flavor (B0(Bˉ0)B^0(\bar{B}^0), \ell^{\mp}) event samples, we measure the mass difference between the two mass eigenstates of the neutral BB meson to be Δmd\Delta m_d= (0.509±0.017 (stat)±0.020 (syst)) ps1(0.509 \pm 0.017~(\rm stat) \pm 0.020~(\rm syst))~ps^{-1}.Comment: 16 pages, 14 figure

    Evidence for Direct CP Violation in B0 -> K+- pi-+ Decays

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    We report evidence for direct CP violation in the decay B0 -> K+-pi-+ with 253/fb of data collected with the Belle detector at the KEKB e+e- collider. Using 275 million B B_bar pairs we observe a B -> K+-pi-+ signal with 2140+-53 events. The measured CP violating asymmetry is Acp(K+-pi-+) = -0.101+-0.025 (stat)+-0.005 (syst), corresponding to a significance of 3.9 sigma including systematics. We also search for CP violation in the decays B+- -> K+-pi0 and B+- -> pi+-pi0. The measured CP violating asymmetries are Acp(K+-pi0) = 0.04+-0.05(stat)+-0.02(syst) and Acp(pi+-pi0) = -0.02+-0.10(stat)+-0.01(syst), corresponding to the intervals -0.05 < Acp(K+-pi0) < 0.13 and -0.18<Acp(pi+-pi0)<0.14 at 90% confidence level.Comment: 9 pages, 3 figures. submitted to Physical Review Letter

    Search for Charmless Two-body Baryonic Decays of B Mesons

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    We report the results of a search for the rare baryonic decays B0ppˉB^0 \to p\bar{p}, ΛΛˉ\Lambda\bar{\Lambda}, and B+pΛˉB^+ \to p\bar{\Lambda}. The analysis is based on a data set of 31.7×106BBˉ31.7\times 10^6 B\bar{B} events collected by the Belle detector at the KEKB e+ee^+e^- collider. No statistically significant signals are found, and we set branching fraction upper limits B(B0ppˉ)<1.2×106{\mathcal B}(B^0 \to p\bar{p}) < 1.2 \times 10^{-6}, B(B0ΛΛˉ)<1.0×106{\mathcal B}(B^0 \to \Lambda\bar{\Lambda}) < 1.0 \times 10^{-6}, and B(B+pΛˉ)<2.2×106{\mathcal B}(B^+ \to p\bar{\Lambda}) < 2.2 \times 10^{-6} at the 90% confidence level.Comment: 6 pages, 4 figures and 1 table. Submitted to Phys. Rev. D Rapid Communication

    Structure and flexibility of the endosomal Vps34 complex reveals the basis of its function on membranes

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    Phosphatidylinositol 3-kinase Vps34 complexes regulate intracellular membrane trafficking in endocytic sorting, cytokinesis and autophagy. We present the 4.4 Å crystal structure of the 385 kDa endosomal complex II (PIK3C3-CII), consisting of Vps34, Vps15 (p150), Vps30/Atg6 (Beclin 1) and Vps38 (UVRAG). The subunits form a Y-shaped complex, centered on the Vps34 C2 domain. Vps34 and Vps15 intertwine in one arm where the Vps15 kinase domain engages the Vps34 activation loop to regulate its activity. Vps30 and Vps38 form the other arm that brackets the Vps15/Vps34 heterodimer, suggesting a path for complex assembly. Hydrogen-Deuterium Exchange Mass Spectrometry (HDX-MS) revealed conformational changes accompanying membrane binding and identified a Vps30 loop that is critical for the ability of complex II to phosphorylate giant liposomes on which complex I is inactive

    Measurement of B0d - B0d-bar mixing rate from the time evolution of dilepton events at the Upsilon(4S)

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    We report a determination of the B0d - B0d-bar mixing parameter Delta-m_d based on the time evolution of dilepton yields in Upsilon(4S) decays. The measurement is based on a 5.9 /fb data sample collected by the Belle detector at KEKB. The proper-time difference distributions for same-sign and opposite-sign dilepton events are simultaneously fitted to an expression containing Delta-m_d as a free parameter. Using both muons and electrons, we obtain Delta-m_d = 0.463 +- 0.008(stat.) +- 0.016(sys.) ps^{-1} This is the first determination of Delta-m_d from time evolution measurements at the Upsilon(4S). We also place limits on possible CPT violations.Comment: 12 pages, 2 figure
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