2,033 research outputs found

    Individual leader to interdependent leadership: A case study in leadership development and tripartite evaluation

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    This article is available open access through the publisher’s website at the link below. Copyright @ 2013 Sage Publications.The Problem - In this case study we see a move away from orthodox views of school leadership as “headship” to a more contemporary model of educational leadership wherein we note a departure from functional, curricula-based school leadership toward more human resource development (HRD) approaches. The aim of this study was to consider the effectiveness of an educational development program for middle leaders within an educational establishment. The Solution - We examined the impact of a bespoke higher education leadership development intervention in Leadership (and Change) on the formation and cohesiveness of a newly formed innovative leadership structure. The Stakeholders - The leadership development intervention was designed through a tripartite collaboration including a university, senior school leaders, and staff. The intervention was designed to shift leadership from individual leader agency to interdependent human leadership agency. Through tripartite evaluation we uncover leadership development praxis that transcends the boundaries of conventional educational leadership and reemphasizes the benefits of bridging the academic/practitioner divide and the application of theory to praxis

    Rapid retreat of permafrost coastline observed with aerial drone photogrammetry

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    Permafrost landscapes are changing around the Arctic in response to climate warming, with coastal erosion being one of the most prominent and hazardous features. Using drone platforms, satellite images, and historic aerial photographs, we observed the rapid retreat of a permafrost coastline on Qikiqtaruk – Herschel Island, Yukon Territory, in the Canadian Beaufort Sea. This coastline is adjacent to a gravel spit accommodating several culturally significant sites and is the logistical base for the Qikiqtaruk – Herschel Island Territorial Park operations. In this study we sought to (i) assess short-term coastal erosion dynamics over fine temporal resolution, (ii) evaluate short-term shoreline change in the context of long-term observations, and (iii) demonstrate the potential of low-cost lightweight unmanned aerial vehicles (“drones”) to inform coastline studies and management decisions. We resurveyed a 500&thinsp;m permafrost coastal reach at high temporal frequency (seven surveys over 40&thinsp;d in 2017). Intra-seasonal shoreline changes were related to meteorological and oceanographic variables to understand controls on intra-seasonal erosion patterns. To put our short-term observations into historical context, we combined our analysis of shoreline positions in 2016 and 2017 with historical observations from 1952, 1970, 2000, and 2011. In just the summer of 2017, we observed coastal retreat of 14.5&thinsp;m, more than 6 times faster than the long-term average rate of 2.2±0.1&thinsp;m&thinsp;a−1 (1952–2017). Coastline retreat rates exceeded 1.0±0.1&thinsp;m&thinsp;d−1 over a single 4&thinsp;d period. Over 40&thinsp;d, we estimated removal of ca. 0.96&thinsp;m3&thinsp;m−1&thinsp;d−1. These findings highlight the episodic nature of shoreline change and the important role of storm events, which are poorly understood along permafrost coastlines. We found drone surveys combined with image-based modelling yield fine spatial resolution and accurately geolocated observations that are highly suitable to observe intra-seasonal erosion dynamics in rapidly changing Arctic landscapes.</p

    Dephosphorylation of YB-1 is Required for Nuclear Localisation During G2 Phase of the Cell Cycle

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    Elevated levels of nuclear Y-box binding protein 1 (YB-1) are linked to poor prognosis in cancer. It has been proposed that entry into the nucleus requires specific proteasomal cleavage. However, evidence for cleavage is contradictory and high YB-1 levels are prognostic regardless of cellular location. Here, using confocal microscopy and mass spectrometry, we find no evidence of specific proteolytic cleavage. Doxorubicin treatment, and the resultant G2 arrest, leads to a significant increase in the number of cells where YB-1 is not found in the cytoplasm, suggesting that its cellular localisation is variable during the cell cycle. Live cell imaging reveals that the location of YB-1 is linked to progression through the cell cycle. Primarily perinuclear during G1 and S phases, YB-1 enters the nucleus as cells transition through late G2/M and exits at the completion of mitosis. Atomistic modelling and molecular dynamics simulations show that dephosphorylation of YB-1 at serine residues 102, 165 and 176 increases the accessibility of the nuclear localisation signal (NLS). We propose that this conformational change facilitates nuclear entry during late G2/M. Thus, the phosphorylation status of YB-1 determines its cellular location

    Measurement of the Branching Fraction of the Decay B+π+π+ν\boldsymbol{B^{+}\to\pi^{+}\pi^{-}\ell^{+}\nu_\ell} in Fully Reconstructed Events at Belle

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    We present an analysis of the exclusive B+π+π+νB^{+}\to\pi^{+}\pi^{-}\ell^{+}\nu_{\ell} decay, where \ell represents an electron or a muon, with the assumption of charge-conjugation symmetry and lepton universality. The analysis uses the full Υ(4S)\Upsilon(4S) data sample collected by the Belle detector, corresponding to 711 fb1^{-1} of integrated luminosity. We select the events by fully reconstructing one BB meson in hadronic decay modes, subsequently determining the properties of the other BB meson. We extract the signal yields using a binned maximum-likelihood fit to the missing-mass squared distribution in bins of the invariant mass of the two pions or the momentum transfer squared. We measure a total branching fraction of B(B+π+π+ν)=[22.71.6+1.9(stat)±3.5(syst)]×105{{\cal B}(B^{+}\to \pi^{+}\pi^{-}\ell^{+}\nu_{\ell})= [22.7 ^{+1.9}_{-1.6} (\mathrm{stat}) \pm 3.5(\mathrm{syst}) ]\times 10^{-5}}, where the uncertainties are statistical and systematic, respectively. This result is the first reported measurement of this decay.Comment: 23 pages, 19 figure

    Measurement of the CKM Matrix Element Vcb|V_{cb}| from B0D+νB^{0} \to D^{*-} \ell^+ \nu_\ell at Belle

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    We present a new measurement of the CKM matrix element Vcb|V_{cb}| from B0D+νB^{0} \to D^{*-} \ell^+ \nu_\ell decays, reconstructed with the full Belle data set of 711fb1711 \, \rm fb^{-1} integrated luminosity. Two form factor parameterizations, originally conceived by the Caprini-Lellouch-Neubert (CLN) and the Boyd, Grinstein and Lebed (BGL) groups, are used to extract the product F(1)ηEWVcb\mathcal{F}(1)\eta_{\rm EW}|V_{cb}| and the decay form factors, where F(1)\mathcal{F}(1) is the normalization factor and ηEW\eta_{\rm EW} is a small electroweak correction. In the CLN parameterization we find F(1)ηEWVcb=(35.06±0.15±0.56)×103\mathcal{F}(1)\eta_{\rm EW}|V_{cb}| = (35.06 \pm 0.15 \pm 0.56) \times 10^{-3}, ρ2=1.106±0.031±0.007\rho^{2}=1.106 \pm 0.031 \pm 0.007, R1(1)=1.229±0.028±0.009R_{1}(1)=1.229 \pm 0.028 \pm 0.009, R2(1)=0.852±0.021±0.006R_{2}(1)=0.852 \pm 0.021 \pm 0.006. For the BGL parameterization we obtain F(1)ηEWVcb=(34.93±0.23±0.59)×103\mathcal{F}(1)\eta_{\rm EW}|V_{cb}|= (34.93 \pm 0.23 \pm 0.59)\times 10^{-3}, which is consistent with the World Average when correcting for F(1)ηEW\mathcal{F}(1)\eta_{\rm EW}. The branching fraction of B0D+νB^{0} \to D^{*-} \ell^+ \nu_\ell is measured to be B(B0D+ν)=(4.90±0.02±0.16)%\mathcal{B}(B^{0}\rightarrow D^{*-}\ell^{+}\nu_{\ell}) = (4.90 \pm 0.02 \pm 0.16)\%. We also present a new test of lepton flavor universality violation in semileptonic BB decays, B(B0De+ν)B(B0Dμ+ν)=1.01±0.01±0.03 \frac{{\cal B }(B^0 \to D^{*-} e^+ \nu)}{{\cal B }(B^0 \to D^{*-} \mu^+ \nu)} = 1.01 \pm 0.01 \pm 0.03~. The errors correspond to the statistical and systematic uncertainties respectively. This is the most precise measurement of F(1)ηEWVcb\mathcal{F}(1)\eta_{\rm EW}|V_{cb}| and form factors to date and the first experimental study of the BGL form factor parameterization in an experimental measurement

    Evidence for a vector charmonium-like state in e+eDs+Ds2(2573)+c.c.e^+e^- \to D^+_sD^*_{s2}(2573)^-+c.c.

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    We report the measurement of e+eDs+Ds2(2573)+c.c.e^+e^- \to D^+_sD^*_{s2}(2573)^-+c.c. via initial-state radiation using a data sample of an integrated luminosity of 921.9 fb1^{-1} collected with the Belle detector at the Υ(4S)\Upsilon(4S) and nearby. We find evidence for an enhancement with a 3.4σ\sigma significance in the invariant mass of Ds+Ds2(2573)+c.c.D^+_sD^*_{s2}(2573)^- +c.c. The measured mass and width are (4619.88.0+8.9(stat.)±2.3(syst.)) MeV/c2(4619.8^{+8.9}_{-8.0}({\rm stat.})\pm2.3({\rm syst.}))~{\rm MeV}/c^{2} and (47.014.8+31.3(stat.)±4.6(syst.)) MeV(47.0^{+31.3}_{-14.8}({\rm stat.})\pm4.6({\rm syst.}))~{\rm MeV}, respectively. The mass, width, and quantum numbers of this enhancement are consistent with the charmonium-like state at 4626 MeV/c2c^2 recently reported by Belle in e+eDs+Ds1(2536)+c.c.e^+e^-\to D^+_sD_{s1}(2536)^-+c.c. The product of the e+eDs+Ds2(2573)+c.c.e^+e^-\to D^+_sD^*_{s2}(2573)^-+c.c. cross section and the branching fraction of Ds2(2573)Dˉ0KD^*_{s2}(2573)^-\to{\bar D}^0K^- is measured from Ds+Ds2(2573)D^+_sD^*_{s2}(2573)^- threshold to 5.6 GeV.Comment: 9 pages, 4 figure

    Inclusive study of bottomonium production in association with an η\eta meson in e+ee^+e^- annihilations near Υ(5S)\Upsilon(5S)

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    We study bottomonium production in association with an η\eta meson in e+ee^+e^- annihilations near the Υ(5S)\Upsilon(5S), at a center of mass energy of s=10.866\sqrt{s}=10.866\,GeV. The results are based on the 121.4121.4\,fb1^{-1} data sample collected by the Belle experiment at the asymmetric energy KEKB collider. Only the η\eta meson is reconstructed and the missing-mass spectrum of η\eta candidates is investigated. We observe the e+eηΥJ(1D)e^+e^-\to\eta\Upsilon_J(1D) process and find evidence for the e+eηΥ(2S)e^+e^-\to\eta\Upsilon(2S) process, while no significant signals of Υ(1S)\Upsilon(1S), hb(1P)h_b(1P), nor hb(2P)h_b(2P) are found. Cross sections for the studied processes are reported.Comment: Submitted to EPJ-
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