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Some authors explicitly adopted the terminology "teleportation without Bell-state measurements." It should be noticed that when teleportation is achieved via local measurements, this typically occurs after some interaction process has taken place, which means that such measurements are actually effective indirect Bell-state measurements. This is is indeed the case of the protocol presented in this work.
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Some authors explicitly adopted the terminology "teleportation without Bell-state measurements." It should be noticed that when teleportation is achieved via local measurements, this typically occurs after some interaction process has taken place, which means that such measurements are actually effective indirect Bell-state measurements. This is is indeed the case of the protocol presented in this work.
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Clearly, due to J1=0 [J3=0] at step (b) [step (c)] E23 [E12] effectively acts over the spin space of centers 2 and 3 [1 and 2] and likewise V□23 V□[12].
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Clearly, due to J 1 = 0 [J 3 = 0] at step (b) [step (c)] E 23 [E 12] effectively acts over the spin space of centers 2 and 3 [1 and 2] and likewise V□ 23 V□ [12].
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For polarized electrons injected in |↑□ and postselected in |↑□ e the centers' fixed point other than the singlet is |↑□,↑□ 12. Concerning the present scheme, notice that in the photonic setup the coupling between e and the centers effectively vanishes for up-polarized photons when the centers' state is |↑□,↑□ 12, while it does not for down-polarized photons. Hence, in our protocol sending particles in a statistical mixture of |↑□ and |↓ □ e is crucial for its effectiveness in the photonic setting (see also Ref. [16]).
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For polarized electrons injected in |↑□ e and postselected in |↑□ e the centers' fixed point other than the singlet is |↑□,↑□ 12. Concerning the present scheme, notice that in the photonic setup the coupling between e and the centers effectively vanishes for up-polarized photons when the centers' state is |↑□,↑□ 12, while it does not for down-polarized photons. Hence, in our protocol sending particles in a statistical mixture of |↑□ and |↓ □ e is crucial for its effectiveness in the photonic setting (see also Ref. [16]).
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It should be pointed out that the scheme in Ref. [18] demands an additional detector able to record back-reflected particles along with the ability to inject, depending on the detector outcomes, either on- or off-resonance mediators.
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It should be pointed out that the scheme in Ref. [18] demands an additional detector able to record back-reflected particles along with the ability to inject, depending on the detector outcomes, either on- or off-resonance mediators.
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