Unconditional quantum teleportation

Quantum teleportation of optical coherent states was demonstrated experimentally using squeezed-state entanglement. The quantum nature of the achieved teleportation was verified by the experimentally determined fidelity Fexp = 0.58 +/- 0.02, which describes the match between input and output states. A fidelity greater than 0.5 is not possible for coherent states without the use of entanglement. This is the first realization of unconditional quantum teleportation where every state entering the device is actually teleported.

[1]  Albert Einstein,et al.  Can Quantum-Mechanical Description of Physical Reality Be Considered Complete? , 1935 .

[2]  Klauder,et al.  SU(2) and SU(1,1) interferometers. , 1986, Physical review. A, General physics.

[3]  Hall,et al.  Generation of squeezed states by parametric down conversion. , 1986, Physical review letters.

[4]  J. Bell,et al.  Speakable and Unspeakable in Quatum Mechanics , 1988 .

[5]  Reid,et al.  Quantum correlations of phase in nondegenerate parametric oscillation. , 1988, Physical review letters.

[6]  Rarity,et al.  Use of parametric down-conversion to generate sub-Poissonian light. , 1988, Physical review. A, General physics.

[7]  A. Zeilinger,et al.  Speakable and Unspeakable in Quantum Mechanics , 1989 .

[8]  Reid,et al.  Demonstration of the Einstein-Podolsky-Rosen paradox using nondegenerate parametric amplification. , 1989, Physical review. A, General physics.

[9]  Reynaud,et al.  Observation of high-intensity sub-Poissonian light using an optical parametric oscillator. , 1990, Physical review letters.

[10]  E S Polzik,et al.  Frequency doubling with KNbO(3) in an external cavity. , 1991, Optics letters.

[11]  Ou,et al.  Realization of the Einstein-Podolsky-Rosen paradox for continuous variables. , 1992, Physical review letters.

[12]  Silvania F. Pereira,et al.  Realization of the Einstein-Podolsky-Rosen paradox for continuous variables in nondegenerate parametric amplification , 1992 .

[13]  Kimble,et al.  Spectroscopy with squeezed light. , 1992, Physical review letters.

[14]  Charles H. Bennett,et al.  Teleporting an unknown quantum state via dual classical and Einstein-Podolsky-Rosen channels. , 1993, Physical review letters.

[15]  Davidovich,et al.  Teleportation of an atomic state between two cavities using nonlocal microwave fields. , 1994, Physical review. A, Atomic, molecular, and optical physics.

[16]  Vaidman Teleportation of quantum states. , 1993, Physical review. A, Atomic, molecular, and optical physics.

[17]  Harald Weinfurter,et al.  Quantum Teleportation and Quantum Computation Based on Cavity QED , 1995 .

[18]  Mann,et al.  Measurement of the Bell operator and quantum teleportation. , 1995, Physical review. A, Atomic, molecular, and optical physics.

[19]  Pérès,et al.  Quantum-state disturbance versus information gain: Uncertainty relations for quantum information. , 1995, Physical review. A, Atomic, molecular, and optical physics.

[20]  H. Weinfurter,et al.  Experimental quantum teleportation , 1997, Nature.

[21]  Samuel L. Braunstein,et al.  Quantum error correction for communication with linear optics , 1998, Nature.

[22]  F. Martini,et al.  Experimental Realization of Teleporting an Unknown Pure Quantum State via Dual Classical and Einstein-Podolsky-Rosen Channels , 1997, quant-ph/9710013.

[23]  Samuel L. Braunstein,et al.  A posteriori teleportation , 1998, Nature.

[24]  H. Kimble,et al.  Teleportation of continuous quantum variables , 1998, Technical Digest. Summaries of Papers Presented at the International Quantum Electronics Conference. Conference Edition. 1998 Technical Digest Series, Vol.7 (IEEE Cat. No.98CH36236).