在φ^4$模型中通过激发振子产生 "磕碰"-"反磕碰 "对

Fabiano C. Simas, E. da Hora
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引用次数: 0

摘要

我们研究了一个具有单一标量场和两个不对称基态的模型中的振子衰变。具体来说,我们验证了初始激发振子的演化如何导致在中心长寿命脉冲存在的情况下形成反激变对。在这种情况下,原始扰动的大小是影响这一过程的最重要因素。对于这个幅度的中间值,我们发现了一种过渡行为,表明平移和振动模式之间的能量交换开始在整个演化过程中发挥重要作用。随着幅度的增大,中心脉冲在构成对的内部结构之间产生了相互作用,其行为类似于标准的反激-扭结碰撞,因此加强了能量转移机制的作用。对于不同的宽度值,一个几乎纯粹的反扭结-扭结对在多次反弹后会逃逸到无穷远处。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Generation of kink-antikink pairs through the excitation of an oscillon in the $φ^4$ model
We examine the oscillon decay in a model with a single scalar field and two asymmetric fundamental states. Specifically, we verify how the evolution of an initially excited oscillon leads to the formation of antikink-kink pairs in the presence of a centered long-lived pulse. In such a context, the magnitude of the original perturbation stands for the most important factor influencing the process. For intermediary values of this magnitude, we find a transitory behavior which suggests that the energy exchange between translational and vibrational modes begins to play an important role in the overall evolution. As the magnitude increases, the centered pulse intermediates an interaction between the inner structures which compose the pairs whose behavior mimics that of a standard antikink-kink collision and therefore reinforces the role played by the energy transfer mechanism. For different values of width, an almost pure antikink-kink pair escapes to the infinity after multiple bounces.
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