1,108 research outputs found

    The role of the international patent system in the transfer of technology to West Africa : case studies : Ghana and Nigeria

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    The principal aim of this thesis is to undertake a critical examination of the role of the international patent system in the transfer of technology to West Africa, particularly Ghana and Nigeria. It focuses mainly on the patent systans and technology regulatory regimes of the two countries. The study is intended to identify and evaluate the impact of the international patent system on the transfer and development of technology in this area. The first chapter provides a theoretical foundation to some of the more practical issues to be discussed in the subsequent chapters. The Paris Convention and the diplomatic revision exercise thereof, as well as other efforts and policies regarding patents and technology transfer at various levels are discussed in Chapter Two. Chapters Three to Eight consider the two case-studies undertaken in this thesis. Chapter Three begins with the historical development of the patent system in both Ghana and Nigeria, and the remaining chapters continue with a discussion of the present patent and technology regulatory regimes of both countries. Based on facts and figures the two case-studies examine critically the patent law and systems and technology transfer laws of these two countries including other related institutional measures highlighting their strengths and weaknesses. The study argues that if the patent systems of both countries are to play a meaningful role in the transfer and developnent of technology they nust be utilized as a tool of economic policy and also be related to the technology transfer regimes which nust necessarily be integrated into the national technology policy which should, in turn, be made an integral part of the entire national developnent plan. It is concluded that it is only in this way that the patent system can effectively contribute to the transfer of technology and the development of indigenous technological capabilities in the two countries

    Interior penalty discontinuous galerkin methods for electromagnetic and acoustic wave equations

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    Introduction: In this thesis we present and analyze the numerical approximation of the second order electromagnetic and acoustic wave equation by the interior penalty (IP) discontinuous Galerkin (DG) finite element method (FEM). In Part I we focus on time-harmonic Maxwell source problems in the high-frequency regime. Part II is devoted to the study of the IP DG FEM for time-dependent acoustic and electromagnetic wave equations. We begin by stating Maxwell's equations in time and frequency domain. We proceed by a variational formulation of Maxwell's equations, and describe the key challenges that are faced in the analysis of the Maxwell operator. Then, we review conforming finite element methods to discretize the second order Maxwell operator. We end this general introduction with some numerical results to highlight the performance and feasibility of conforming FEM for Maxwell's equations. Chapter 2: In this chapter, we introduce and analyze the interior penalty discontinuous Galerkin method for the numerical discretization of the indefinite time-harmonic Maxwell equations in high-frequency regime. Based on suitable duality arguments, we derive a-priori error bounds in the energy norm and the L2-norm. In particular, the error in the energy norm is shown to converge with the optimal order O(hminfs;`g) with respect to the mesh size h, the polynomial degree `, and the regularity exponent s of the analytical solution. Under additional regularity assumptions, the L2-error is shown to converge with the optimal order O(h`+1). The theoretical results are confirmed in a series of numerical experiments on triangular meshes. The thesis' author's principal contributions are the proof of the L2-error bound in Section 2.6, and the proof of Lemma 2.4.1. Chapter 3: We present and analyze an interior penalty method for the numerical discretization of the indefinite time-harmonic Maxwell equations in mixed form. The method is based on the mixed discretization of the curl-curl operator developed in [44] and can be understood as a non-stabilized variant of the approach proposed in [63]. We show the well-posedness of this approach and derive optimal a-priori error estimates in the energy-norm as well as the L2-norm. The theoretical results are confirmed in a series of numerical experiments. The thesis' author's principal contribution is the proof of the L2-error bound in Section 3.6. Chapter 4: The symmetric interior penalty discontinuous Galerkin finite element method is presented for the numerical discretization of the second-order scalar wave equation. The resulting stiffness matrix is symmetric positive definite and the mass matrix is essentially diagonal; hence, the method is inherently parallel and, leads to fully explicit time integration when coupled with an explicit timestepping scheme. Optimal a priori error bounds are derived in the energy norm and the L2-norm for the semi-discrete formulation. In particular, the error in the energy norm is shown to converge with the optimal order O(hminfs;`g) with respect to the mesh size h, the polynomial degree `, and the regularity exponent s of the continuous solution. Under additional regularity assumptions, the L2-error is shown to converge with the optimal order O(h`+1). Numerical results confirm the expected convergence rates and illustrate the versatility of the method. Chapter 5: We develop the symmetric interior penalty discontinuous Galerkin (DG) method for the spatial discretization in the method of lines approach of the timedependent Maxwell equations in second-order form. We derive optimal a-priori estimates for the semi-discrete error in the energy norm. For smooth solutions, these estimates hold for DG discretizations on general finite element meshes. For low-regularity solutions that have singularities in space, the theoretical estimates hold on conforming, affine meshes. Moreover, on conforming triangular meshes, we derive optimal error estimates in the L2-norm. Finally, we valuate our theoretical results by a series of numerical experiments

    KN and KN two-body physics: 2-5 GeV/c

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    The author reviews KN and KN induced reactions in the intermediate energy region to sketch present theoretical understanding and to high- light promising avenues for the future. He emphasizes several experiments that should advance or consolidate understanding: polarization for K/sup 0/p to K/sup +/n, K/sup -/p to K/sup 0/n, K/sub L//sup 0/p to K/sub s//sup 0/p; R parameter data for K/sup +/p to K /sup +/p and KN to Lambda pi and Sigma /sup +/ pi . A determination of precise cross section differences between K/sup +or-/p and K/sup +or- /n elastic scattering; between K and K charge exchange and between KN to pi Y and pi N to KY is described. (20 refs)

    Analytic study of the Maxwell electromagnetic invariant in spinning and charged Kerr-Newman black-hole spacetimes

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    Abstract The Maxwell invariant plays a fundamental role in the mathematical description of electromagnetic fields in charged spacetimes. In particular, it has recently been proved that spatially regular scalar fields which are non-minimally coupled to the Maxwell electromagnetic invariant can be supported by spinning and charged Kerr-Newman black holes. Motivated by this physically intriguing property of asymptotically flat black holes in composed Einstein-Maxwell-scalar field theories, we present a detailed analytical study of the physical and mathematical properties of the Maxwell electromagnetic invariant F KN r θ M a Q FKN(r,θ;M,a,Q) {\mathcal{F}}_{\textrm{KN}}\left(r,\theta; M,a,Q\right) which characterizes the Kerr-Newman black-hole spacetime [here {r, θ} are respectively the radial and polar coordinates of the curved spacetime and {M, J = M a, Q} are respectively the mass, angular momentum, and electric charge parameters of the black hole]. It is proved that, for all Kerr-Newman black-hole spacetimes, the spin and charge dependent minimum value of the Maxwell electromagnetic invariant is attained on the equator of the black-hole surface. Interestingly, we reveal the physically important fact that Kerr-Newman spacetimes are characterized by two critical values of the dimensionless rotation parameter a ̂ ≡ a / r + a^a/r+ \hat{a}\equiv a/{r}_{+} [here r + (M, a, Q) is the black-hole horizon radius], a ̂ crit − = 3 − 2 2 a^crit=322 {\hat{a}}_{\textrm{crit}}^{-}=\sqrt{3-2\sqrt{2}} and a ̂ crit + = 5 − 2 5 a^crit+=525 {\hat{a}}_{\textrm{crit}}^{+}=\sqrt{5-2\sqrt{5}} , which mark the boundaries between three qualitatively different spatial functional behaviors of the Maxwell electromagnetic invariant: (i) Kerr-Newman black holes in the slow-rotation a ̂ < a ̂ crit − a^<a^crit \hat{a}<{\hat{a}}_{\textrm{crit}}^{-} regime are characterized by negative definite Maxwell electromagnetic invariants that increase monotonically towards spatial infinity, (ii) for black holes in the intermediate spin regime a ̂ crit − ≤ a ̂ ≤ a ̂ crit + a^crita^a^crit+ {\hat{a}}_{\textrm{crit}}^{-}\le \hat{a}\le {\hat{a}}_{\textrm{crit}}^{+} , the positive global maximum of the Kerr-Newman Maxwell electromagnetic invariant is located at the black-hole poles, and (iii) Kerr-Newman black holes in the super-critical regime a ̂ < a ̂ crit + a^<a^crit+ \hat{a}<{\hat{a}}_{\textrm{crit}}^{+} are characterized by a non-monotonic spatial behavior of the Maxwell electromagnetic invariant F KN r = r + θ M a Q FKN(r=r+,θ;M,a,Q) {\mathcal{F}}_{\textrm{KN}}\left(r={r}_{+},\theta; M,a,Q\right) along the black-hole horizon with a spin and charge dependent global maximum whose polar angular location is characterized by the dimensionless functional relation a ̂ 2 a^2 {\hat{a}}^2 · (cos2 θ)max = 5 – 2 5 25 2\sqrt{5}

    Triangular embeddings of Kn−Km with unboundedly large m

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    AbstractThe author has proposed methods of constructing index 2 and 3 current graphs generating triangular embeddings of graphs Kn−Km with unboundedly large m (asn increases). As a result, triangular embeddings of graphs of many families of graphs Kn−Km with unboundedly large m were constructed. The paper gives a survey of these results and a short explanation of the methods

    Slowly rotating black holes in the novel Einstein–Maxwell-scalar theory

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    We investigate a slowly rotating black hole solution in a novel Einstein–Maxwell-scalar theory, which is prompted by the classification of general Einstein–Maxwell-scalar theory. The gyromagnetic ratio of this black hole is calculated, and it increases as the second free parameter β\beta increases, but decreases with the increasing parameter γ2α21+α2\gamma \equiv \frac{2 \alpha ^{2}}{1+\alpha ^2}. In the Einstein–Maxwell-dilaton (EMD) theory, the parameter β\beta vanishes but the free parameter α\alpha governing the strength of the coupling between the dilaton and the Maxwell field remains. The gyromagnetic ratio is always less than 2, the well-known value for a Kerr–Newman (KN) black hole as well as for a Dirac electron. Scalar hairs reduce the magnetic dipole moment in dilaton theory, resulting in a drop in the gyromagnetic ratio. However, we find that the gyromagnetic ratio of two can be realized in this Einstein–Maxwell-scalar theory by increasing β\beta and the charge-to-mass ratio Q/M simultaneously (recall that the gyromagnetic ratio of KN black holes is independent of Q/M). The same situation also applies to the angular velocity of a locally non-rotating observer. Moreover, we analyze the period correction for circular orbits in terms of charge-to-mass ratio, as well as the correction of the radius of the innermost stable circular orbits. It is found the correction increases with β\beta but decreases with Q/M. Finally, the total radiative efficiency is investigated, and it can vanish once the effect of rotation is considered

    Einige extremale Aufgaben für die Klassen Kn(E) und P(E)

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    The abstracts (in two languages) can be found in the pdf file of the article. Original author name(s) and title in Russian and Lithuanian: Г. Кирьяцкий. Некоторые экстремальные задачи в классах Kn(E) и Р(Е) E. G. Kirjackis. Kai kurie ekstremaliniai uždaviniai Kn(E) ir P(E) klasės

    Ausdehnung einiger Sätze von Aksentjeff und Tshakaloff auf die Klassen Kn(D)

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    The abstracts (in two languages) can be found in the pdf file of the article. Original author name(s) and title in Russian and Lithuanian: Э. Г. Кирьяцкий. Распространение некоторых теорем Аксентьева и Чакалова на класс Kn(D) E. G. Kirjackis. Kai kurios Aksentjevo ir Čakalovo teoremos Kn(D) klasėj

    Superradiation of Dirac particles in KN black hole

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    In this article, we process the approximate wave function of the Dirac particle outside the horizon of the KN ds black hole to effective potential V, and then derive V (including real and imaginary parts). We know that fermions cannot produce superradiation, but we can prove that Dirac particles in the KN black hole background can have a special solution through a certain operation, forming a Cooper pair, thus producing superradiation.We deal with the real and imaginary parts separately. When V (real part or imaginary part) has a maximum value, there may be a potential barrier outside the field of view to have a chance to produce superradiation.Comment: 12 pages. arXiv admin note: text overlap with arXiv:2103.04239; text overlap with arXiv:1501.06570 by other author
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