875 research outputs found

    Contextual barriers to mobile health technology in African countries: a perspective piece

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    On a global scale, healthcare practitioners are now beginning to move from traditional desktop-based computer technologies towards mobile computing environments[1]. Consequently, such environments have received immense attention from both academia and industry, in order to explore these promising opportunities, apparent limitations, and implications for both theory and practice[2]. The application of mobile IT within a medical context, referred to as mobile health or mHealth, has revolutionised the delivery of healthcare services as mobile technologies offer the potential of retrieving, modifying and entering patient-related data/information at the point-of-care. As a component of the larger health informatics domain mHealth may be referred as all portable computing devices (e.g. mobile phones, mobile clinical assistants and medical sensors) used in a healthcare context to support the delivery of healthcare services

    TO EXAMINE THE DIFFERENCES IN REARFOOT KINEMATICS DURING TREADMILL AND OVERGROUND RUNNING

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    This study examined the differences between the kinematics of rearfoot motion in overground (OG) and treadmill (TM) running. Two subjects ran at various speeds under both conditions and a three-dimensional analysis was performed using the Peak Motus Analysis system. TM running produced repeatable and consistent measures of rearfoot motion across all speeds however OG running was more variable. While there are some differences between the two modes, this can be explained by TM mechanics and TM testing cannot be dismissed based on this. Speed was found to influence most variables making speed control critical in obtaining reliable measures of rearfoot motion. The TM easily and accurately provides this, which advocates its use in locomotion studies. It was concluded that speed control is more important than the mode of runnin

    Absorptive part of meson--baryon scattering amplitude and baryon polarization in chiral perturbation theory

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    We compute the spin asymmetry and polarization of the final-state baryon in its rest frame in two-body meson--baryon low-energy scattering with unpolarized initial state, to lowest non-trivial order in BChPT. The required absorptive amplitudes are obtained analytically at one-loop level. We discuss the polarization results numerically for several meson--baryon processes. Even at low energies above threshold, where BChPT can reasonably be expected to be applicable, sizable values of polarization are found for some processes

    Fermion masses in noncommutative geometry

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    Recent indications of neutrino oscillations raise the question of the possibility of incorporating massive neutrinos in the formulation of the Standard Model (SM) within noncommutative geometry (NCG). We find that the NCG requirement of Poincare duality constrains the numbers of massless quarks and neutrinos to be unequal unless new fermions are introduced. Possible scenarios in which this constraint is satisfied are discussed.Comment: 4 pages, REVTeX; typos are corrected in (19), "Possible Solutions" and "Conclusion" are modified; additional calculational details are included; references are update

    On the Ultraviolet Behaviour of Newton's constant

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    We clarify a point concerning the ultraviolet behaviour of the Quantum Field Theory of gravity, under the assumption of the existence of an ultraviolet Fixed Point. We explain why Newton's constant should to scale like the inverse of the square of the cutoff, even though it is technically inessential. As a consequence of this behaviour, the existence of an UV Fixed Point would seem to imply that gravity has a built-in UV cutoff when described in Planck units, but not necessarily in other units.Comment: 8 pages; CQG class; minor changes and rearrangement

    Strangeness spin, magnetic moment and strangeness configurations of the proton

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    The implications of the empirical signatures for the positivity of the strangeness magnetic moment μs\mu_s, and the negativity of the strangeness contribution to the proton spin Δs\Delta_s, on the possible uudssˉuuds\bar s configurations of five quarks in the proton are analyzed. The empirical signs for the values of these two observables can only be obtained in configurations where the uudsuuds system is orbitally excited and the sˉ\bar s quark is in the ground state. The configurations, in which the sˉ\bar s is orbitally excited, which include the conventional K+Λ0K^+\Lambda^0 congfiguration, with the exception of that, in which the uudsuuds component has spin 2, yield negative values for μs\mu_s. Here the strangeness spin Δs\Delta_s, the strangeness magnetic moment μs\mu_s and the axial coupling constant GAsG_A^s are calculated for all possible configurations of the uudssˉuuds\bar s component of the proton. In the configuration with [4]FS[22]F[22]S[4]_{FS}[22]_F[22]_S flavor-spin symmetry, which is likely to have the lowest energy, μs\mu_s is positive and Δs≃GAs≃−1/3μs\Delta_s\simeq G_A^s\simeq -1/3\mu_s.Comment: 17 page

    Weak Hyperon Decays: Quark Sea and SU(3) Symmetry Breaking

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    An explanation of the difference in the values of the apparent f/df/d ratios for the S- and P- wave amplitudes of nonleptonic hyperon decays is proposed. The argument is formulated in the framework of the standard pole model with (56,0+)(56,0^{+}) ground-state and (70,1−)(70,1^{-}) excited baryons as intermediate states for the P- and S- waves respectively. Under the assumption that the dominant part of the deviation of (f/d)P−wave(f/d)_{P-wave} from −1-1 is due to large quark sea effects, SU(3)SU(3) symmetry breaking in energy denominators is shown to lead to a prediction for (f/d)S−wave(f/d)_{S-wave} which is in excellent agreement with experiment. This corroborates our previous unitarity calculations which indicated that the matrix elements of the parity conserving weak Hamiltonian between the ground-state baryons are characterized by f0/d0≈−1.6f_{0}/d_{0} \approx -1.6 or more. A brief discussion of the problem of the relative size of S- and P- wave amplitudes is given. Finally, implications for weak radiative hyperon decays are also discussed.Comment: 26 pages, LATEX, 1647/PH IFJ Krako
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