Continuous-Variable Quantum Teleportation with a Conventional Laser (Rev. Ver.)

Details Continuous-Variable Quantum Teleportation with a Conventional Laser (Rev. Ver.) Continuous-Variable Quantum Teleportation with a Conventional Laser (Rev. Ver.)

2003-04-23

arxiv.org/abs/quant-ph/0304148v1

Phys. Rev. A 68, 050302(R) (2003)

Physics

Quantum Physics

5 pages, 2 figures. This is a revised version of quant-ph/0301045. I have not replaced that original version with this revised

Scientific paper

10.1103/PhysRevA.68.050302

We give a description of balanced homodyne detection (BHD) using a conventional laser as a local oscillator (LO), where the laser field outside the cavity is a mixed state whose phase is completely unknown. Our description is based on the standard interpretation of the quantum theory for measurement, and accords with the experimental result in the squeezed state generation scheme. We apply our description of BHD to continuous-variable quantum teleportation (CVQT) with a conventional laser to analyze the CVQT experiment [A. Furusawa et al., Science 282, 706 (1998)], whose validity has been questioned on the ground of intrinsic phase indeterminacy of the laser field [T. Rudolph and B.C. Sanders, Phys. Rev. Lett. 87, 077903 (2001)]. We show that CVQT with a laser is valid only if the unknown phase of the laser field is shared among sender's LOs, the EPR state, and receiver's LO. The CVQT experiment is considered valid with the aid of an optical path other than the EPR channel and a classical channel, directly linking between a sender and a receiver. We also propose a method to probabilistically generate a strongly phase-correlated quantum state via continuous measurement of independent lasers, which is applicable to realizing CVQT without the additional optical path.

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