Abstract
The Ξ hyperon is produced in a parity-conserving interaction involving only a proton and two spinless K mesons. Therefore, the Ξ beam in any direction consists of an equal, incoherent mixture of two pure spin states which go into each other under 180° rotation in the production plane. This condition implies a new restriction upon the angular distribution of the Ξ decay products. In particular, the distribution I(θ,φ)=1+Acosθ is impossible for A0 unless the Ξ spin is ½.

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