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This state is an entangled state and is already quite adjustable. Further modifications can be made with ordinary optical components. For example, if θl=πlA and ø=π, then a half-wave plate in the signal beam could be used to switch the signal polarization |>s↔|V>s to produce |ψ′ DC>, V>s|H>i, H>s|V>i)√2. This polarization state is analogous to the singlet state for two spin-1/2 particles |ψ single>et>, ↑>|↓>-|↓>|>/√2
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