Abstract
The intensity of ultra-short pulse lasers has reached 10 W/cm owing to the advancements in laser technology. The large radiation from the electron behaves something like resistance in this ultrarelativistic laser–electron interaction. This effect is called the “radiation reaction”. The equation of motion with the radiation reaction is known as the Lorentz–Abraham–Dirac equation; however, this equation does not incorporate the spin property. In laser plasmas, classical physics descriptions are preferred for simulations. This paper discusses how to describe the radiation reaction of a spinning relativistic electron in classical dynamics. Subject Index A00, A01, G03, J25
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