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首页> 外文期刊>International journal of modern physics, D. Gravitation, astrophysics, cosmology >Induced vacuum bosonic current by magnetic flux in a higher dimensional compactified cosmic string spacetime
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Induced vacuum bosonic current by magnetic flux in a higher dimensional compactified cosmic string spacetime

机译:高维压缩宇宙弦时空中的磁通感应产生的真空硼电流。

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In this paper, we analyze the bosonic current densities induced by a magnetic flux running along an idealized cosmic string in a high-dimensional spacetime, admitting that the coordinate along the string's axis is compactified. Additionally we admit the presence of a magnetic flux enclosed by the compactification axis. In order to develop this analysis we calculate the complete set of normalized bosonic wave functions obeying a quasiperiodicity condition, with arbitrary phase beta, along the compactified dimension. In this context, only azimuthal and axial currents densities take place. As to the azimuthal current, two contributions appear. The first contribution corresponds to the standard azimuthal current in a cosmic string spacetime without compactification, while the second contribution is a new one, induced by the compactification itself. The latter is an even function of the magnetic flux enclosed by the string axis and is an odd function of the magnetic flux along its core with period equal to quantum flux, Phi(0) = 2 pi/e. On the other hand, the nonzero axial current density is an even function of the magnetic flux along the core of the string and an odd function of the magnetic flux enclosed by it. We also find that the axial current density vanishes for untwisted and twisted bosonic fields in the absence of the magnetic flux enclosed by the string axis. Some asymptotic expressions for the current density are provided for specific limiting cases of the physical parameter of the model.
机译:在本文中,我们分析了在高维时空中沿着理想化宇宙线传播的磁通量所感应的玻色子电流密度,并承认沿线轴的坐标已被压缩。另外,我们承认存在由压实轴包围的磁通量。为了进行此分析,我们沿压缩维数计算了服从准周期条件且具有任意相位β的归一化正弦波函数的完整集合。在这种情况下,仅发生方位和轴向电流密度。关于方位电流,出现了两个贡献。第一个贡献对应于未压缩的宇宙弦时空中的标准方位电流,而第二个贡献是由压缩本身引起的新贡献。后者是由弦轴包围的磁通量的偶数函数,并且是沿着其磁芯且周期等于量子通量Phi(0)= 2 pi / e的磁通量的奇数函数。另一方面,非零轴向电流密度是沿着弦线芯的磁通量的偶数函数,并且是由其包围的磁通量的奇数函数。我们还发现,在不存在弦轴包围的磁通量的情况下,未扭曲和扭曲的玻色子场的轴向电流密度消失了。对于模型的物理参数的特定极限情况,提供了一些电流密度的渐近表达式。

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