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Cited in the paper.
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Cited in the paper.
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Cited in the paper.
The maximum quantum value can be obtained preparing the state ⟨ ψ | = ( 0 , 0 , 1 ) \langle\psi|=(0,0,1) and with the tests i = 2 | v i ⟩ ⟨ v i | − 𝟙 i=2|v_{i}\rangle\langle v_{i}|-\openone with ⟨ v 0 | = N 0 ( 1 , 0 , r ) \langle v_{0}|=N_{0}\left(1,0,r\right) , ⟨ v 1 , 4 | = N 1 ( c , ± s , r ) \langle v_{1,4}|=N_{1}\left(c,\pm s,r\right) , ⟨ v 2 , 3 | = N 2 ( C , ∓ S , r ) \langle v_{2,3}|=N_{2}\left(C,\mp S,r\right) , where r = cos ( π 5 ) r=\sqrt{\cos{\left(\frac{\pi}{5}\right)}} , c = cos ( 4 π 5 ) c=\cos{\left(\frac{4\pi}{5}\right)} , s = sin ( 4 π 5 ) s=\sin{\left(\frac{4\pi}{5}\right)} , C = cos ( 2 π 5 ) C=\cos{\left(\frac{2\pi}{5}\right)} , S = sin ( 2 π 5 ) S=\sin{\left(\frac{2\pi}{5}\right)} , and N i N_{i} are suitable normalization factors
Cited in the paper.