Department of Applied Physics, School of Engineering, The University of Tokyo, 7-3-1 Hongo, Tokyo 113-8656, Japan.
Nature. 2013 Aug 15;500(7462):315-8. doi: 10.1038/nature12366.
Quantum teleportation allows for the transfer of arbitrary unknown quantum states from a sender to a spatially distant receiver, provided that the two parties share an entangled state and can communicate classically. It is the essence of many sophisticated protocols for quantum communication and computation. Photons are an optimal choice for carrying information in the form of 'flying qubits', but the teleportation of photonic quantum bits (qubits) has been limited by experimental inefficiencies and restrictions. Main disadvantages include the fundamentally probabilistic nature of linear-optics Bell measurements, as well as the need either to destroy the teleported qubit or attenuate the input qubit when the detectors do not resolve photon numbers. Here we experimentally realize fully deterministic quantum teleportation of photonic qubits without post-selection. The key step is to make use of a hybrid technique involving continuous-variable teleportation of a discrete-variable, photonic qubit. When the receiver's feedforward gain is optimally tuned, the continuous-variable teleporter acts as a pure loss channel, and the input dual-rail-encoded qubit, based on a single photon, represents a quantum error detection code against photon loss and hence remains completely intact for most teleportation events. This allows for a faithful qubit transfer even with imperfect continuous-variable entangled states: for four qubits the overall transfer fidelities range from 0.79 to 0.82 and all of them exceed the classical limit of teleportation. Furthermore, even for a relatively low level of the entanglement, qubits are teleported much more efficiently than in previous experiments, albeit post-selectively (taking into account only the qubit subspaces), and with a fidelity comparable to the previously reported values.
量子隐形传态允许发送方将任意未知的量子态从一个地方传输到空间上相隔很远的接收方,只要这两方共享一个纠缠态并且能够进行经典通信。它是许多复杂的量子通信和计算协议的本质。光子是携带“飞行量子位”信息的最佳选择,但光子量子位(qubit)的隐形传态受到实验效率低下和限制的限制。主要缺点包括线性光学贝尔测量的基本概率性质,以及当探测器无法解析光子数时,要么需要破坏传输的量子位,要么需要衰减输入量子位。在这里,我们实验实现了无后选择的光子量子位的完全确定性隐形传态。关键步骤是利用涉及连续变量对离散变量的量子隐形传态的混合技术。当接收器的前馈增益被最佳调谐时,连续变量传送器充当纯损耗通道,并且基于单个光子的输入双轨编码量子位表示针对光子损耗的量子错误检测码,并且对于大多数隐形传态事件仍然保持完整。即使对于不完美的连续变量纠缠态,这也允许进行忠实的量子位传输:对于四个量子位,整体传输保真度范围为 0.79 到 0.82,并且它们全部超过隐形传态的经典极限。此外,即使纠缠水平相对较低,与以前的实验相比,量子位的传输效率也更高,尽管是后选择(仅考虑量子位子空间),并且与以前报道的值相当。