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IEEE International Conference on Quantum Computing and Engineering (QCE)

Quantum Teleportation Using a Genuinely Classical Communication Channel Must Fail

Maria Violaris, Simone Rijavec, Charles Alexandre Bédard

Published Sep 15, 2024• 0 citations
Publisher

Abstract

During the quantum teleportation protocol, Alice sends two bits of classical information to Bob, which somehow transports quantum information from Alice's location to Bob's location. The local account of teleportation from Deutsch and Hayden reveals that these bits are actually qubits instantiating locally inaccessible information, and appear classical because they carry information in a form that is robust to decoherence. If the classical bits have absolutely no underlying quantum properties, teleportation will fail - challenging all current and future variants of quantum theory that explain teleportation using only classical properties of the physical bits being transported. A successful teleportation via apparently classical bits therefore indicates that either: (1) the fundamental principle of locality, which says that isolated systems are independent from each other, is false, or (2) the apparently classical bits actually have some quantum properties. We propose using existing models for quantum-classical dynamics, such as Sudarshan's, and the dynamics-independent Constructor Theory, to determine exactly what features a system with unknown dynamics needs to carry information for teleportation. Our proposal may characterise a new form of non-classicality, giving novel insights into hybrid quantum-classical systems. This could lead to new experimental proposals to test the properties of systems with unknown dynamics.

DOI
10.1109/qce60285.2024.10383

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During the quantum teleportation protocol, Alice sends two bits of classical information to Bob, which somehow transports quantum information from Alice's location to Bob's location. The local account of teleportation from Deutsch and Hayden reveals that these bits are actually qubits instantiating locally inaccessible information, and appear classical because they carry information in a form that is robust to decoherence. If the classical bits have absolutely no underlying quantum properties, teleportation will fail - challenging all current and future variants of quantum theory that explain teleportation using only classical properties of the physical bits being transported. A successful teleportation via apparently classical bits therefore indicates that either: (1) the fundamental principle of locality, which says that isolated systems are independent from each other, is false, or (2) the apparently classical bits actually have some quantum properties. We propose using existing models for quantum-classical dynamics, such as Sudarshan's, and the dynamics-independent Constructor Theory, to determine exactly what features a system with unknown dynamics needs to carry information for teleportation. Our proposal may characterise a new form of non-classicality, giving novel insights into hybrid quantum-classical systems. This could lead to new experimental proposals to test the properties of systems with unknown dynamics.
Quantum teleportation is the name of a problem: How can the real-valued parameters encoding the state at Alice’s location make their way to Bob’s location via shared entanglement and only two bits of classical communication? Without an explanation, teleportation appears to be a conjuring trick. Investigating the phenomenon with Schrödinger states and reduced density matrices shall always leave loose ends because they are not local and complete descriptions of quantum systems. Upon demonstrating that the Heisenberg picture admits a local and complete description, Deutsch and Hayden rendered its explanatory power manifest by revealing the trick behind teleportation, namely, by providing an entirely local account. Their analysis is re-exposed and further developed.
In this work, we consider the following teleportation protocol: There is an arbitrary two-qubit resource state, shared between two spatially separated parties, Alice and Bob. Applying local unitary operators, they transform the resource state into the canonical form. To teleport an unknown qubit, Alice now measures her qubits in the Bell basis. Then, the measurement outcome is communicated by Alice to Bob via noisy classical channel(s). Finally, after receiving the classical message, Bob applies the necessary unitary operator to his qubit. Under this protocol, we find the exact formulae of teleportation fidelity and its deviation. We further find conditions for non-classical fidelity within this protocol. If the classical communication is noiseless in the above protocol then there are resource states which can lead to zero fidelity deviation. However, we show that such states may not lead to zero fidelity deviation when the classical communication is noisy in the same protocol. We also explore the opposite case, i.e., the states, which cannot lead to zero fidelity deviation in the above protocol when the classical communication is noiseless, may lead to zero fidelity deviation when the classical communication is noisy in the same protocol without compromising the non-classical fidelity. Moreover, we exhibit scenarios within the present protocol, where the fidelity deviation increases if the entanglement of the resource state is increased.
What is proposed here is a simple modication in the quantum protocol [1] for achieving instantaneous teleportation of arbitrary quantum state from Alice to Bob even when Bob is several light years away. This modied quantum protocol is constructed by adding a step the in the celebrated quantum teleportation protocol [1]. It consists of the action of a unitary operator to be performed by Alice on the qubits in her possession before she does the Bell basis measurement. It is important to note that the existing quantum teleportation protocol [1] requires certain classical communication between the participants, Alice and Bob, and we are going to eliminate this classical communication through our modification. In the existing protocol [1] Alice requires sending the classical bits generated during her Bell basis measurement over a classical channel to Bob for Bob to use these classical bits to determine the exact recovery operation to be performed on the qubit(s) in his possession for creating the exactly identical copy of unknown quantum state that was with Alice and got destroyed during her Bell basis measurement. Alice cannot send the classical bits she obtained to Bob with the speed faster than that of light since it is the well known experimentally veried universal upper limit on the speed. We show that by incorporating suitable unitary operation to be performed by Alice on her qubits before the Bell basis measurement the requirement of the transmission of classical bits by Alice to Bob for the creation of the unknown quantum state by Bob at his place can be completely eliminated. Our modification in the teleportation protocols [1], [2] thus clearly demonstrates the enormous advantage of remaining in the quantum regime and avoiding the requirement of any classical communication for the teleportation of the quantum states.
We investigate whether it is possible to teleport the coherence of an unknown quantum state from Alice to Bob by communicating a lesser number of classical bits in comparison to what is required for teleporting an unknown quantum state. We find that we cannot achieve perfect teleportation of coherence with one bit of classical communication for an arbitrary qubit. However, we find that if the qubit is partially known, i.e., chosen from the equatorial and polar circles of the Bloch sphere, then teleportation of coherence is possible with the transfer of one cbit of information when we have maximally entangled states as a shared resource. In the case of the resource being a non-maximally entangled state, we can teleport the coherence with a certain probability of success. In a general teleportation protocol for coherence, we derive a compact formula for the final state at Bob's lab in terms of the composition of the completely positive maps corresponding to the shared resource state and joint POVM performed by Alice on her qubit and the unknown state. Using this formula, we show that teleportation of the coherence of a partially known state with real matrix elements is possible perfectly with the help of a maximally entangled state as a resource. Furthermore, we explore the teleportation of coherence with the Werner states and show that even when the Werner states become separable, the amount of teleported coherence is non-zero, implying the possibility of teleportation of coherence without entanglement.
FINDING: Quantum teleportation transfers quantum *state* (information), not matter — no particle traverses the channel; only a classical 2-bit message plus a pre-shared entangled pair is required. | MATH: Protocol (Bennett et al. 1993): Alice holds unknown state |ψ⟩ = α|0⟩ + β|1⟩ (|α|²+|β|²=1) and one qubit of a Bell pair |Φ⁺⟩ = (|00⟩+|11⟩)/√2. Joint Bell-basis measurement yields one of 4 outcomes {|Φ±⟩,|Ψ±⟩}, each probability 1/4. Alice sends 2 classical bits (log₂4 = 2). Bob applies one of {I, X, Z, XZ} to recover |ψ⟩ exactly. Fidelity F=1; no-cloning preserved (state destroyed at Alice). | CONNECTION: The 4 Bell states form an orthonormal basis of the 2-qubit Hilbert space ℂ²⊗ℂ² ≅ ℂ⁴ — a complete measurement basis. The 1/4 uniform outcome probability is the maximally-mixed (maximally-entangled) reference state ρ = I/4. This is the qubit analogue of a 4-fold symmetric point group (C₂ᵥ-like), and the Pauli group {I,X,Y,Z} is the order-4 operator set closing under multiplication. The √ Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com