Fig. 4From: A supplemental device to return escaping particles to a magnetic mirror reactorThe gyration orbit of a relativistic electron. The conditions are the same with in Fig. 3, except for the following change of the initial velocity at ( t = 0): \( \widehat{z}\ {z}_0=\widehat{z}\ {10}^8 \) \( \to -\widehat{z}\ {10}^8 \) m/s. This figure is related with Fig. 1cBack to article page