Abstract
The detailed knowledge of the experimental setup is of essential importance for the calculation of radiative corrections since the actual computation has to be fitted to the prevailing situation. Here we choose relatively simple experimental circumstances:
An extremely well-focused monoenergetic (E1) electron beam impinges on a proton target. We shall distinguish between two cases:
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I.
Detection of the outgoing electrons,
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II.
Detection of the recoil protons.
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Urban, P. (1970). Examples. In: Topics in Applied Quantumelectrodynamics. Springer, Vienna. https://doi.org/10.1007/978-3-7091-8247-5_9
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DOI: https://doi.org/10.1007/978-3-7091-8247-5_9
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