一种利用γ激光或γ射线实现可控核聚变的方法

Shihao Chen, Ziwei Chen
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引用次数: 2

摘要

提出了一种利用γ激光或γ射线与普通激光实现可控核聚变的方法,这些激光具有一定的频率和足够大的强度来照射目标球。普通激光的作用是加热靶核,实现对靶核的惯性约束。吸收γ光子的靶核将处于一定的激发态。散射截面将更大,点火温度将更低,以实现处于激发态的原子核比处于基态的原子核的聚变。与传统聚变中应用的原子核,如双原子核和三原子核相比,根据方法,应用于聚变的原子核应具有以下特征:原子核有其激发态,其中一个激发态具有更高的能量和更长的寿命,原子核的质量更小。因此,可以更容易地实现劳森条件,从而有可能实现可控核聚变。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
A Way to Realize Controlled Nuclear Fusion by γ-Laser or γ-Ray
A way is proposed to realize controllable-nuclear fusion by γ-laser or γ-ray and ordinary laser with their certain frequencies and large enough intensities to irradiate a target ball. The function of ordinary laser is to heat the target nuclei and to realize the inertial confinement for the target nuclei. The target nuclei absorbing γ-photons will be in a certain excited state. The scattering cross-sections will be larger and the ignition temperature will be lower to realize fusion of the nuclei in their excited states than those of the nuclei in their ground states. In contrast with the nuclei applied in conventional fusion, e.g., deutons and tritons, according to the way, the nuclei applied to fusion should have the following characters: the nuclei have their excited states, one of the excited states has higher energy and longer lifetime, and the masses of the nuclei are lesser. Thus, the Lawson conditions can more easily be realized so that the controllable nuclear fusion is possibly realized by the way.
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