5,322 research outputs found

    The disjuncture of learning and recognition: credential assessment from the standpoint of Chinese immigrant engineers in Canada

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    To better recognise foreign qualifications, many OECD countries have promoted liberal fairness epitomised by universal standards and institutional efficiency. This paper departs from such a managerial orientation towards recognition. Building on recognitive justice, it proposes an alternative anchoring point for recognition practices: the standpoint or everyday experiences of immigrants. This approach is illustrated with a qualitative study of the credential recognition practices of the engineering profession in Canada. From the standpoint of Chinese immigrants, the study identifies a disjuncture between credential recognition practices and immigrants’ career stage post-migration. Taking this disjuncture as problematic, it further pinpoints recognition issues such as redundancy and arbitrariness, a narrow focus on undergraduate education, and a deficit view of training from other countries. While some of these issues may be addressed by improving administrative procedures, others demand a participatory space allowing immigrants to become partners of assessment, rather than merely its objects. (DIPF/Orig.

    Three body radiative decay Bs→ϕKˉ0γB_s\to \phi \bar K^0 \gamma in the PQCD approach

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    We study the three body radiative decay Bs→ϕKˉ0γB_s\to \phi \bar K^0 \gamma by introducing the ϕK\phi K pair distribution amplitudes (DAs) in the perturbative QCD approach. This nonperturbative inputs, the two meson DAs, is very important to simplify the calculations. Besides the dominant electromagnetic penguin operator O7γO_{7\gamma}, the subleading contributions from chromomagnetic penguin operator O8gO_{8g}, quark-loop corrections and annihilation type amplitudes are also considered. We find that the branching ratio for the decay Bs→ϕKˉ0γB_s\to \phi \bar K^0 \gamma is about (9.26−1.61−3.86−0.49+1.79+3.12+0.64)×10−8(9.26^{+1.79+3.12+0.64}_{-1.61-3.86-0.49})\times10^{-8}, which is much smaller compared with that for the decay B0→ϕK0γB^0\to \phi K^0\gamma. It is mainly because that the former decay induces by b→dγb\to d\gamma with small CKM matrix element being proportional to λ3\lambda^3. The prediction for the direct CP asymmetry is ACPdir(Bs→ϕKˉ0γ)=(−4.1−0.6−1.2−0.1+0.4+1.7+0.2)%A^{dir}_{CP}(B_s\to \phi \bar K^0 \gamma)=(-4.1^{+0.4+1.7+0.2}_{-0.6-1.2-0.1})\%, which is well consistent with the result from the U-spin symmetry approach. we also predict the Bs→ϕKˉ0γB_s \to\phi \bar K^0\gamma decay spectrum, which exhibits a maximu at the ϕK\phi K invariant masss around 1.95 GeV.Comment: 17 pages,6 figures, Accepted for publication in EPJ
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