200,794 research outputs found

    Magnetization reversal through synchronization with a microwave

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    Based on the Landau-Lifshitz-Gilbert equation, it can be shown that a circularly-polarized microwave can reverse the magnetization of a Stoner particle through synchronization. In comparison with magnetization reversal induced by a static magnetic field, it can be shown that when a proper microwave frequency is used the minimal switching field is much smaller than that of precessional magnetization reversal. A microwave needs only to overcome the energy dissipation of a Stoner particle in order to reverse magnetization unlike the conventional method with a static magnetic field where the switching field must be of the order of magnetic anisotropy.Comment: 4 pages, 5 figure

    The Relativistic Rotation

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    The classical rotation is not self-consistent in the framework of the special theory of relativity. the Relativistic rotation is obtained, which takes the relativistic effect into account. It is demonstrated that the angular frequency of classical rotation is only valid in local approximation. The properties of the relativistic rotation and the relativistic transverse Doppler shift are discussed in this work

    On the momentum-dependence of K−K^{-}-nuclear potentials

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    The momentum dependent K−K^{-}-nucleus optical potentials are obtained based on the relativistic mean-field theory. By considering the quarks coordinates of K−K^- meson, we introduced a momentum-dependent "form factor" to modify the coupling vertexes. The parameters in the form factors are determined by fitting the experimental K−K^{-}-nucleus scattering data. It is found that the real part of the optical potentials decrease with increasing K−K^- momenta, however the imaginary potentials increase at first with increasing momenta up to Pk=450∼550P_k=450\sim 550 MeV and then decrease. By comparing the calculated K−K^- mean free paths with those from K−nK^-n/K−pK^-p scattering data, we suggested that the real potential depth is V0∼80V_0\sim 80 MeV, and the imaginary potential parameter is W0∼65W_0\sim 65 MeV.Comment: 9 pages, 4 figure
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