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arXiv:0806.1679

Is Teleportation a (quantum) mystery?

Berry Groisman

Published Jun 10, 2008• 0 citations
arXivHTMLPDF

Abstract

Since its discovery quantum teleportation has often been seen as a manifestation, indeed the epitome, of the very paradoxical and mysterious nature of quantum theory itself. It is commonly regarded as genuinely quantum and essentially paradoxical. Although a common approach to teleportation amongst physicists nowadays is a somewhat operational one, some researchers are making an effort to deflate the above views. On the one hand, it was recently argued that the paradox of information transfer taking place in teleportation is dissolved (Timpson, 2006) by appealing the very notion of information. On the other hand, it was demonstrated that some classical versions of teleportation retain its important features, which hitherto were considered genuinely quantum (Cohen, 2003; Collins&Popescu, 2002; Hardy, 1999; Mor, 2006; Spekkens, 2007). I will present a special version of a quantum teleportation protocol which is in a sense split into classical and quantum steps. This description provides us with a unified picture of teleportation in both domains. It will be explicitly shown how classical teleportation is embedded in the quantum protocol. Moreover, the classical step can be successfully accomplished even if the state shared by the parties is completely disentangled [this is consistent with the result obtained in (Wang, 2005)]. Yet, all the (apparent) paradoxical features usually associated with quantum teleportation are clearly present in this step. In particular, this demonstrates that entanglement cannot be ultimately responsible and not necessary for the (paradoxical?) information transfer. Thus, even if one considers teleportation as mysterious, all its mysteries are shifted from quantum domain into purely classical one.

DOI
10.48550/arxiv.0806.1679

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Since its discovery quantum teleportation has often been seen as a manifestation, indeed the epitome, of the very paradoxical and mysterious nature of quantum theory itself. It is commonly regarded as genuinely quantum and essentially paradoxical. Although a common approach to teleportation amongst physicists nowadays is a somewhat operational one, some researchers are making an effort to deflate the above views. On the one hand, it was recently argued that the paradox of information transfer taking place in teleportation is dissolved (Timpson, 2006) by appealing the very notion of information. On the other hand, it was demonstrated that some classical versions of teleportation retain its important features, which hitherto were considered genuinely quantum (Cohen, 2003; Collins&Popescu, 2002; Hardy, 1999; Mor, 2006; Spekkens, 2007). I will present a special version of a quantum teleportation protocol which is in a sense split into classical and quantum steps. This description provides us with a unified picture of teleportation in both domains. It will be explicitly shown how classical teleportation is embedded in the quantum protocol. Moreover, the classical step can be successfully accomplished even if the state shared by the parties is completely disentangled [this is consistent with the result obtained in (Wang, 2005)]. Yet, all the (apparent) paradoxical features usually associated with quantum teleportation are clearly present in this step. In particular, this demonstrates that entanglement cannot be ultimately responsible and not necessary for the (paradoxical?) information transfer. Thus, even if one considers teleportation as mysterious, all its mysteries are shifted from quantum domain into purely classical one.
Quantum teleportation is a transfer protocol of quantum states, which cannot be realized only with classical physics. The essence of this protocol is quantum entanglement, which was proposed by Einstein as a counter example for quantum mechanics. In terms of quantum information processing, quantum teleportation can be regarded as an “Identity” operation. So one can modify the quantum circuit to make an arbitrary operation and universal quantum computing. One of the application of the quantum computing is “quantum version of coherent communication”, which enables us to get the channel capacity beyond the classical limit (Shannon limit).
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With the advent of quantum technology, the exploration of quantum teleportation has become increasingly important, and it has provided a glimpse of the potential of quantum information science. The current research delves into the background of quantum teleportation, emphasizing its key role in advancing quantum communication and computation. Implications of this research are that it has the potential to revolutionize data transmission and processing, providing a secure and efficient means of exchanging quantum information. This paper is structured to provide a comprehensive study of quantum teleportation, starting with a literature review that lays the foundation for our work. Afterward, the details of our research are presented, including the theoretical framework and the proposed methodology for realizing the quantum teleportation protocol. We provide a careful overview of the technical details, demonstrating the complexity of quantum state preparation, entanglement distribution, and Bell state measurements. Our empirical section demonstrates the practical application of these protocols, providing empirical evidence of successful teleportation of quantum states. The theoretical predictions are confirmed by the experimental results, which validate the feasibility and reliability of our approach. Conclusions drawn from the experiments emphasize the robustness of quantum teleportation as a viable technology for future quantum networks.
Monogamy of entanglement states that quantum correlations cannot be freely shared: if two parties are maximally entangled, neither can be entangled with a third. The Fano plane PG(2,2)\mathrm{PG}(2,2)PG(2,2) appears to violate this principle — its Hamiltonian ground state simultaneously correlates all seven directed triples. Hardy's paradox is a complementary phenomenon: four conditions on a multi-qubit state force the classically impossible conclusion P(Z+,…,Z+)=0P(Z_+,\ldots,Z_+) = 0P(Z+​,…,Z+​)=0, yet quantum mechanics permits P(Z+,…,Z+)>0P(Z_+,\ldots,Z_+) > 0P(Z+​,…,Z+​)>0. Both are well-understood within standard quantum mechanics; neither was ever mysterious to quantum theory itself. This paper identifies a single necessary condition that unifies both phenomena: irreducible three-body entanglement, as measured by the Coffman–Kundu–Wootters three-tangle τ3\tau_3τ3​. The Fano monogamy apparent paradox dissolves once one observes that C(i,j)<1C(i,j) < 1C(i,j)<1 for all pairs and τ3>0\tau_3 > 0τ3​>0 for Fano-line triples — the correlations are triangular, not pairwise. For the tripartite Hardy impossible event (N=3N=3N=3), we show numerically that τ3>0\tau_3 > 0τ3​>0 is a necessary condition: no W-class or product state (τ3=0\tau_3 = 0τ3​=0) satisfies all four Hardy conditions simultaneously, confirmed across 54 independent free-state optimisations (JAX/Adam, A100 GPU). The open question — whether this is provable algebraically — is stated explicitly. The novel contribution is the connection between the Dür–Vidal–Cirac entanglement classification and Hardy-type nonlocality: GHZ-class states (τ3>0\tau_3 > 0τ3​>0) can exhibit the tripartite impossible event; W-class states cannot. Within the Adelic Simplicial Architecture (ASA), both phenomena share a further geometric explanation: the octonion associator ∣A(ei,ej,ek)∣=0|\mathcal{A}(e_i,e_j,e_k)| = 0∣A(ei​,ej​,ek​)∣=0 on Fano-line triples and ∣A∣=2|\mathcal{A}| = 2∣A∣=2 elsewhere is the algebraic signature of the same triangular irreducibility, connecting the monogamy resolution and the Hardy condition to the associator firewall of the companion papers on the Spacelike Associator Paradox and Hardy's Paradox and the Fano Associator.
The standard quantum teleportation scheme is deconstructed, and those aspects of it that appear remarkable and "non-classical" are identified. An alternative teleportation scheme, involving only classical states and classical information, is then formulated, and it is shown that the classical scheme reproduces all of these remarkable aspects, despite the fact that they had seemed non-classical. This leads to a re-examination of quantum teleportation, which suggests that its significance depends on the interpretation of quantum states.