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The fission barrier is a concept in nuclear physics that describes the energy required to split an atomic nucleus. Nuclei, composed of neutrons and protons, are held together by the strong nuclear force. However, the repulsive Coulomb force between positively charged protons can destabilize the nucleus.

When a nucleus is excited, it can deform. The fission barrier arises from the interplay between the surface tension (which favors a spherical shape) and the Coulomb repulsion (which increases with deformation). If the nucleus gains enough energy to overcome this barrier, it can split into two smaller nuclei, releasing a significant amount of energy. This process, known as nuclear fission, can be induced by particles like neutrons. The height and shape of this barrier vary for different nuclei.123

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