March 10, 2015 feature
Traveling without moving: Quantum communication scheme transfers quantum states without transmitting physical particles
Prof. Shou Zhang discussed the paper that he and his colleagues published in Scientific Reports. "There's a long-held assumption in the classical information field that information transfer requires physical particles to travel between sender and receiver – an assumption first challenged in 2013 by Hatim Salih and his colleagues1," Zhang tells Phys.org. By using the so-called chained quantum Zeno effect, the 2013 paper showed how information can in fact be transferred between two locations without any physical particles traveling between them. (In the quantum Zeno effect, time evolution caused by quantum decoherence in quantum systems is suppressed by, for example, continuous observation or measurement, interaction with the environment, or stochastic fields. In a chained quantum Zeno effect, a series of secondary splitter/detector loops ensure that there is never a significant probability of decoherence.) "This mind-boggling and highly counterintuitive communication protocol inspired us to think whether quantum information can be transferred counterfactually," Zhang adds, "so in fact, our present scheme can be considered as an incremental extension of Salih's work from classical bit to quantum bit."
"In quantum information science," Zhang continues, "the minimum information unit is quantum state-encoded qubit. However, to date, schemes for the transfer of an unknown quantum state required physical particles to travel – for example, quantum teleportation needs prior entanglement sharing and classical communication, and both entanglement sharing and classical communication cannot be done without transmitting physical particles. In our scheme, entanglement sharing and classical communication are not needed."
In short, existing quantum-information transfer schemes require a physical medium, and it was unclear if quantum information can be transferred without transmitting any physical particles – but this paper suggests that it can. To achieve this counterfactual scheme by entangling two nonlocal qubits with each other without interaction, Zhang says that their main challenge was determining how to place the obstructing object in Salih's scheme in an unknown quantum superposition state of presence and absence. "Entanglement is basic resource for many nonlocal quantum information tasks," Zhang notes. "However, it's well known that distant separable states cannot be entangled only by means of local operations and classical communication. Generally, people introduce nonlocal interaction by entanglement swapping or transmitting a mediating particle between distant quantum nodes. Interaction-free measurement provides a new way to create entanglement, and so, albeit inconceivably, two qubits can be entangled without interaction."
Zhang notes that there were also several challenges in the experiment in realizing the scheme by using a photon and a Rydberg atom assisted by a mesoscopic atomic ensemble, such as trapping atoms and the ensemble's coherent time. (A Rydberg atom is an excited atom with one or more electrons that have a very high principal quantum number, meaning that the electron has higher potential energy and is therefore less tightly bound to the nucleus.) "Given that this paper is a theoretical work, and these technical challenges have been well researched in the existing literature, we only consider the ideal case in the paper."
The key component in this work, Zhang tells Phys.org, is the quantum version of the obstructing object. "In fact, any atom with two energy levels resonant with the photon's frequency can be used to act as the quantum obstructing object to control the passing or absorption of the photon, but the coupling between a single atom and a photon is so weak that the scheme cannot be achieved with high probability. The present scheme uses a single Rydberg atom to control the atomic ensemble via Rydberg dipole blockade." A Rydberg dipole blockade, which results from the interactions shifting the energy levels of the atoms, can be used to inhibit transitions into all but singly excited collective states – and thereby to manipulate quantum information stored in collective states of mesoscopic ensembles.
What's key is that during the entire process, the photon did not enter the channel between sender and receiver: As long as the photon passes through the channel, it will be absorbed by the ensemble if the control atom is in the ground state – but if the atom is in the Rydberg state, the photon will be absorbed by the detector. In this way, an unknown quantum state can be transferred between two distant participants without any physical particles traveling between them.
"The advantages of using the combined system," Zhang explains, are twofold: the coupling strength of the photon with the quantum obstructing object is greatly enhanced; and the individual addressing of an atom is not required. In principle, as long as the quantum obstructing object can be implemented, this scheme is universal for other physical systems of quantum information processing, such as trapped ion systems, superconducting quantum systems and quantum dot systems."
Unlike typical teleportation, the present scheme can transport an unknown qubit between two distant participants in a nondeterministic manner. "Typical teleportation can teleport an unknown quantum state perfectly by using subsequent local operations. However," Zhang points out, "in the last step of the present scheme, the sender will obtain two measurement results of the single atom state, and the recipient can obtain the teleported state perfectly only if the sender's measurement result is a Rydberg state. If the sender's measurement result is ground state, the quantum state the recipient receives has a phase flip error compared with the teleported state. Hence, the success probability is 50%. On the other hand, if the recipient wants to obtain the quantum information deterministically, the sender only needs to send one bit of information – that is, single-qubit detection results – to the recipient for the transfer of one qubit. However, in the one-qubit teleportation procedure, two bits of classical communication – that is, Bell-state measurement results – are required."
Regarding the implications and limits of their approach, Zhang says that the present scheme requires the single photon go through a large number of cycles in the nested interferometer, so the main limits of the scheme are the distance of the two parties and the coherent time of the Rydberg atom. "In principle, however, quantum information can be transferred without entanglement sharing or classical communication between the two parties regardless of the physical distance separating them." However, he emphasizes that since the coherent time of the atom is finite in practice, the counterfactual quantum-information transfer can be only implemented over a limited distance.
Despite the effect of the imperfections mentioned in the paper, Zhang tells Phys.org that the key component in the experimental system indicating that their scheme may be feasible using current technology is the combined system of a single atom and a mesoscopic atomic ensemble – specifically, the development of the cold Rydberg gas with alkali-metal vapor. "Moreover," he adds, "the remaining elements in the scheme are the most common optical elements found in the laboratory."
Moving forward, Zhang notes that the scientists are now researching the deeper mechanism behind the counterfactual quantum-information transfer, which he says may involve the foundation of quantum mechanics. "In addition, using the basic idea of the scheme, many nonlocal quantum information tasks could be achieved. We may develop other counterfactual quantum information protocols, such as quantum cloning or quantum algorithms."
In closing, Zhang says that the present scheme provides a new way for nonlocal quantum information processing, so it may lead to a quantum network that does not require physical particle transmission. "We also hope the present scheme can be realized in a physical experiment. On the other hand, the deeper mechanism behind the counterfactual scheme has not been revealed, which may well excite people's interest in the fundamental of quantum mechanics, such as quantum interference and wave-particle duality."
1Protocol for direct counterfactual quantum communication, Physical Review Letters (2013) 110:170502, doi:10.1103/PhysRevLett.110.170502
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