Abstract.
Cross-section, vector-polarization, and tensor-polarization distributions are calculated for the reactions \( e^{+}e^{-}\rightarrow\bar{p}p\) and \( e^{+}e^{-}\rightarrow \bar{\Lambda}\Lambda\). Each reaction requires six characteristic functions that are bilinear in the, possibly complex, electromagnetic form factors, denoted \( G_{E}(P^{2})\) and \( G_{M}(P^{2})\), of p and \( \Lambda\). For the hyperon reaction also the joint-decay distributions of \( \Lambda\) and \( \bar{\Lambda}\) are calculated. Their knowledge allows a complete determination of the hyperon electromagnetic form factors, without measuring hyperon spins. We explain how this is done in practice. For some tensor-polarization components our results are in conflict with previously repeatedly published distributions.
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Communicated by S.-L. Zhu
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Fäldt, G. Polarization observables in the \(e^{+}e^{-} \rightarrow \bar{\Lambda}\Lambda\) reaction. Eur. Phys. J. A 52, 141 (2016). https://doi.org/10.1140/epja/i2016-16141-y
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DOI: https://doi.org/10.1140/epja/i2016-16141-y