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A Way to Realize Controlled Nuclear Fusion by γ-Laser or γ-Ray

机译:一种通过& -Laser或& gamma-Ray实现受控核聚变的方式

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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.
机译:提出了一种以一定的频率和足够大的强度照射目标球的γ-激光或γ-射线与普通激光实现可控核聚变的方法。普通激光的功能是加热目标原子核并实现目标原子核的惯性约束。吸收γ-光子的目标核将处于一定的激发态。为了实现处于激发态的核的融合,与处于其基态的核的融合相比,散射截面将更大并且点火温度将更低。与常规聚变中使用的原子核(例如氘核和tri核)相反,按照这种方式,应用于聚变的原子核应具有以下特征:原子核具有激发态,其中一个激发态具有更高的能量和更长的寿命,原子核的质量较小。因此,可以更容易地实现劳森条件,从而可能实现可控的核聚变。

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