167 research outputs found

    Educating and training in an Ideological vacuum: A critical explanation of the dilemma of education in Zimbabwe

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    This paper is a philosophical study on ideology and its indispensable relationship to education policy making and implementation and its didactical dimension with a special reference to Zimbabwe. The paper points out that successive colonial governments and religious organisations of that era established and worked, planned and implemented their policies within the bounds of liberal-cum-capitalist ideological framework. Hence all their education and training institutions were built and meant to fulfill that cause. Post-independent Africa inherited that framework and found herself giving her citizens education that created useless school leavers. This paper will advance an argument that educating and training in an ideological vacuum stifles critical and creative thinking which is the sources and foundation of potential invention and innovation. It therefore calls for Africa to come up with an ideological framework that defines their contextual social, political, and economic condition(s) resulting in crafting policies that are relevant to their needs than repeating tired ideologies. Key words: Ideology, education, training, vacuum, Zimbabwe, society

    An exploration of ebook selection behavior in academic library collections

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    Academic libraries have offered ebooks for some time, however little is known about how readers interact with them while making relevance decisions. In this paper we seek to address that gap by analyzing ebook transaction logs for books in a university library

    Sum rules and energy scales in the high-temperature superconductor YBa2Cu3O6+x

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    The Ferrell-Glover-Tinkham (FGT) sum rule has been applied to the temperature dependence of the in-plane optical conductivity of optimally-doped YBa_2Cu_3O_{6.95} and underdoped YBa_2Cu_3O_{6.60}. Within the accuracy of the experiment, the sum rule is obeyed in both materials. However, the energy scale \omega_c required to recover the full strength of the superfluid \rho_s in the two materials is dramatically different; \omega_c \simeq 800 cm^{-1} in the optimally doped system (close to twice the maximum of the superconducting gap, 2\Delta_0), but \omega_c \gtrsim 5000 cm^{-1} in the underdoped system. In both materials, the normal-state scattering rate close to the critical temperature is small, \Gamma < 2\Delta_0, so that the materials are not in the dirty limit and the relevant energy scale for \rho_s in a BCS material should be twice the energy gap. The FGT sum rule in the optimally-doped material suggests that the majority of the spectral weight of the condensate comes from energies below 2\Delta_0, which is consistent with a BCS material in which the condensate originates from a Fermi liquid normal state. In the underdoped material the larger energy scale may be a result of the non-Fermi liquid nature of the normal state. The dramatically different energy scales suggest that the nature of the normal state creates specific conditions for observing the different aspects of what is presumably a central mechanism for superconductivity in these materials.Comment: RevTeX 4 file, 9 pages with 7 embedded eps figure

    S and D Wave Mixing in High TcT_c Superconductors

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    For a tight binding model with nearest neighbour attraction and a small orthorhombic distortion, we find a phase diagram for the gap at zero temperature which includes three distinct regions as a function of filling. In the first, the gap is a mixture of mainly dd-wave with a smaller extended ss-wave part. This is followed by a region in which there is a rapid increase in the ss-wave part accompanied by a rapid increase in relative phase between ss and dd from 0 to π\pi. Finally, there is a region of dominant ss with a mixture of dd and zero phase. In the mixed region with a finite phase, the ss-wave part of the gap can show a sudden increase with decreasing temperature accompanied with a rapid increase in phase which shows many of the characteristics measured in the angular resolved photoemission experiments of Ma {\em et al.} in Bi2Sr2CaCu2O8\rm Bi_2Sr_2CaCu_2O_8Comment: 12 pages, RevTeX 3.0, 3 PostScript figures uuencoded and compresse

    Glimpses of the Octonions and Quaternions History and Todays Applications in Quantum Physics

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    Before we dive into the accessibility stream of nowadays indicatory applications of octonions to computer and other sciences and to quantum physics let us focus for a while on the crucially relevant events for todays revival on interest to nonassociativity. Our reflections keep wandering back to the BrahmaguptaBrahmagupta FibonaccFibonacc two square identity and then via the EulerEuler four square identity up to the DegenDegen GgravesGgraves CayleyCayley eight square identity. These glimpses of history incline and invite us to retell the story on how about one month after quaternions have been carved on the BroughamianBroughamian bridge octonions were discovered by JohnJohn ThomasThomas GgravesGgraves, jurist and mathematician, a friend of WilliamWilliam RowanRowan HamiltonHamilton. As for today we just mention en passant quaternionic and octonionic quantum mechanics, generalization of CauchyCauchy RiemannRiemann equations for octonions and triality principle and G2G_2 group in spinor language in a descriptive way in order not to daunt non specialists. Relation to finite geometries is recalled and the links to the 7stones of seven sphere, seven imaginary octonions units in out of the PlatoPlato cave reality applications are appointed . This way we are welcomed back to primary ideas of HeisenbergHeisenberg, WheelerWheeler and other distinguished fathers of quantum mechanics and quantum gravity foundations.Comment: 26 pages, 7 figure

    Dynamic generation of maximally entangled photon multiplets by adiabatic passage

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    The adiabatic passage scheme for quantum state synthesis, in which atomic Zeeman coherences are mapped to photon states in an optical cavity, is extended to the general case of two degenerate cavity modes with orthogonal polarization. Analytical calculations of the dressed-state structure and Monte Carlo wave-function simulations of the system dynamics show that, for a suitably chosen cavity detuning, it is possible to generate states of photon multiplets that are maximally entangled in polarization. These states display nonclassical correlations of the type described by Greenberger, Horne, and Zeilinger (GHZ). An experimental scheme to realize a GHZ measurement using coincidence detection of the photons escaping from the cavity is proposed. The correlations are found to originate in the dynamics of the adiabatic passage and persist even if cavity decay and GHZ state synthesis compete on the same time scale. Beyond entangled field states, it is also possible to generate entanglement between photons and the atom by using a different atomic transition and initial Zeeman state.Comment: 22 pages (RevTeX), including 23 postscript figures. To be published in Physical Review

    Identification of the bulk pairing symmetry in high-temperature superconductors: Evidence for an extended s-wave with eight line nodes

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    we identify the intrinsic bulk pairing symmetry for both electron and hole-doped cuprates from the existing bulk- and nearly bulk-sensitive experimental results such as magnetic penetration depth, Raman scattering, single-particle tunneling, Andreev reflection, nonlinear Meissner effect, neutron scattering, thermal conductivity, specific heat, and angle-resolved photoemission spectroscopy. These experiments consistently show that the dominant bulk pairing symmetry in hole-doped cuprates is of extended s-wave with eight line nodes, and of anisotropic s-wave in electron-doped cuprates. The proposed pairing symmetries do not contradict some surface- and phase-sensitive experiments which show a predominant d-wave pairing symmetry at the degraded surfaces. We also quantitatively explain the phase-sensitive experiments along the c-axis for both Bi_{2}Sr_{2}CaCu_{2}O_{8+y} and YBa_{2}Cu_{3}O_{7-y}.Comment: 11 pages, 9 figure

    Coupling between planes and chains in YBa2Cu3O7 : a possible solution for the order parameter controversy

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    We propose to explain the contradictory experimental evidence about the symmetry of the order parameter in YBa2Cu3O7YBa_{2}Cu_{3}O_{7} by taking into account the coupling between planes and chains. This leads to an anticrossing of the plane and chain band. We include an attractive pairing interaction within the planes and a repulsive one between planes and chains, leading to opposite signs for the order parameter on planes and chains, and to nodes of the gap because of the anticrossing. Our model blends s-wave and d-wave features, and provides a natural explanation for all the contradictory experimentsComment: 13 pages, revtex, 2 uucoded figure

    Single-particle nonlocality and entanglement with the vacuum

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    We propose a single-particle experiment that is equivalent to the conventional two-particle experiment used to demonstrate a violation of Bell's inequalities. Hence, we argue that quantum mechanical nonlocality can be demonstrated by single-particle states. The validity of such a claim has been discussed in the literature, but without reaching a clear consensus. We show that the disagreement can be traced to what part of the total state of the experiment one assigns to the (macroscopic) measurement apparatus. However, with a conventional and legitimate interpretation of the measurement process one is led to the conclusion that even a single particle can show nonlocal properties.Comment: 6 pages, 5 figure

    Anisotropic superconductivity mediated by phonons in layered compounds with weak screening effect

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    Anisotropic pairing interactions mediated by phonons are examined in layer systems. It is shown that the screening effects become weaker when the layer spacing increases. Then the anisotropic components of the pairing interactions increase with the screening length since the momentum dependence changes. As a result, various types of anisotropic superconductivity occur depending on the parameter region. For example, p-wave superconductivity occurs when the short-range part of Coulomb repulsion is strong and the layer spacing is large. Two kinds of inter-layer pairing may occur when the layer spacing is not too large. Although the phonon contribution to the d-wave pairing interaction is weaker than the p-wave interaction, it increases with the layer spacing. Relevance of the present results to organic superconductors, high-T_c cuprates, and Sr_2RuO_4 is discussed.Comment: 8 pages, 5 figures, (Latex, revtex.sty, epsf.sty
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