Table 9 The exchanges of the input basis vectors for the measurement of the other correlation pairs. The meanings of parentheses and square brackets are same as Table 8.

From: State-independent contextuality in classical light

 

Observables

PD1

PD2

PD3

HWP5

HWP6

\(|{\overrightarrow{{\rm{e}}}}_{0})\,\leftrightarrow \,|{\overrightarrow{{\rm{e}}}}_{2})\)

\({A^{\prime} }_{3}{A^{\prime} }_{5}\)

(\({a^{\prime} }_{5}\))

(\({a^{\prime} }_{3}\))

[\({A^{\prime} }_{3hc}\)]

22.5°

17.6°

\({A^{\prime} }_{2}{A^{\prime} }_{5}\)

(\({a^{\prime} }_{5}\))

(\({a^{\prime} }_{2}\))

[\({A^{\prime} }_{2hc}\)]

22.5°

−17.6°

\({A^{\prime} }_{1}{A^{\prime} }_{6}\)

(\({a^{\prime} }_{6}\))

(\({a^{\prime} }_{1}\))

[\({A^{\prime} }_{1hc}\)]

67.5°

17.6°

\({A^{\prime} }_{4}{A^{\prime} }_{6}\)

(\({a^{\prime} }_{6}\))

(\({a^{\prime} }_{4}\))

[\({A^{\prime} }_{4hc}\)]

−22.5°

17.6°

\(|{\overrightarrow{{\rm{e}}}}_{1})\,\leftrightarrow \,|{\overrightarrow{{\rm{e}}}}_{2})\)

\({A^{\prime} }_{1}{A^{\prime} }_{7}\)

(\({a^{\prime} }_{7}\))

(\({a^{\prime} }_{1}\))

[\({A^{\prime} }_{1hd}\)]

22.5°

17.6°

\({A^{\prime} }_{3}{A^{\prime} }_{7}\)

(\({a^{\prime} }_{7}\))

(\({a^{\prime} }_{3}\))

[\({A^{\prime} }_{3hd}\)]

22.5°

−17.6°

\({A^{\prime} }_{2}{A^{\prime} }_{8}\)

(\({a^{\prime} }_{8}\))

(\({a^{\prime} }_{2}\))

[\({A^{\prime} }_{2hd}\)]

67.5°

17.6°

\({A^{\prime} }_{4}{A^{\prime} }_{8}\)

(\({a^{\prime} }_{8}\))

(\({a^{\prime} }_{4}\))

[\({A^{\prime} }_{4hd}\)]

−22.5°

17.6°