Quantum entanglement swapping

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Quantum entanglement swapping is an essential idea in quantum mechanics. It involves entanglement from one pair of particles to another, even if those new particles have never interacted before. This process is very important for building quantum communication networks, enabling quantum teleportation and advancing quantum computing.

Contents

History

The idea of quantum entanglement swapping came from physicists Marek Żukowski, Anton Zeilinger, Michael A. Horne, and Artur K. Ekert in 1993. Their paper in Physical Review Letters introduced that one can extend entanglement from one particle pair to another using a method called Bell state measurement. [1]

Anton Zeilinger, key contributor to the experimental realization of entanglement swapping A. Zeilinger (cropped).jpg
Anton Zeilinger, key contributor to the experimental realization of entanglement swapping
Artur K. Ekert, key concept of entanglement swapping in 1993, contributing significantly to quantum cryptography and quantum communication Professor Artur Ekert FRS (cropped).jpg
Artur K. Ekert, key concept of entanglement swapping in 1993, contributing significantly to quantum cryptography and quantum communication

Key historical milestones

Concept

Basic principles

Quantum entanglement swapping has three pairs of entangled particles: (A, B), (C, D), & (E, F). Particles A & B are initially entangled, just like C & D. By applying a process called Bell state measurement to one particle from each pair (like B and C), the unmeasured particles (A and D) can become entangled. This happens without any direct interaction between them. [2]

The measurement collapses the states of B and C into one of four Bell states. Due to the laws of quantum mechanics, this instantly determines the state of A and D.

Mathematical representation

In quantum mechanics, a Bell state can be used to represent two particles in an entangled system. The mathematical expression for the swapping process is:

In this expression, refers to the state of X & Y particles while BSM indicates Bell state measurement.

Development and expansions

Quantum repeaters and long-distance communication

One main use of quantum entanglement swapping is for creating quantum repeaters. These devices help stretch out quantum communication networks by allowing entanglement to be shared over long regions. Performing entanglement swapping at certain points acts like relaying information without loss. [3]

Multi-particle entanglement

The idea of quantum entanglement swapping can be developed further into multi-particle setups. They can lead to discovering ways to create complex entangled states known as GHZ states (Greenberger–Horne–Zeilinger states). These states are crucial for quantum error correction and making fault-tolerant quantum computers. [4]

Satellite-based quantum communication

Experiments on satellite-based quantum communication showed how entanglement can link ground stations via satellites while using entanglement swapping to increase range. This marks a huge leap toward building a global quantum internet.

Applications

Quantum teleportation

Entanglement swapping plays an essential role in quantum teleportation, where the state of a particle can be sent from one spot to another without moving the particle itself. This relies on using entangled pairs through the swapping process. [5]

Quantum cryptography

In the field of quantum cryptography, it helps secure communication channels better. By utilizing swapped entangtlements between particles' pairs, it is possible to generate secure encryption keys that should be protected against eavesdropping.

Quantum networks

Quantum entanglement swapping also serves as a core technology for designing quantum networks, where many nodes-like quantum computers or communication points-link through these special connections made by entangled links. These networks support safely transferring quantum information over long routes and contribute significantly to building the emerging quantum internet.

Related Research Articles

In physics, the no-cloning theorem states that it is impossible to create an independent and identical copy of an arbitrary unknown quantum state, a statement which has profound implications in the field of quantum computing among others. The theorem is an evolution of the 1970 no-go theorem authored by James Park, in which he demonstrates that a non-disturbing measurement scheme which is both simple and perfect cannot exist. The aforementioned theorems do not preclude the state of one system becoming entangled with the state of another as cloning specifically refers to the creation of a separable state with identical factors. For example, one might use the controlled NOT gate and the Walsh–Hadamard gate to entangle two qubits without violating the no-cloning theorem as no well-defined state may be defined in terms of a subsystem of an entangled state. The no-cloning theorem concerns only pure states whereas the generalized statement regarding mixed states is known as the no-broadcast theorem.

<span class="mw-page-title-main">Quantum teleportation</span> Physical phenomenon

Quantum teleportation is a technique for transferring quantum information from a sender at one location to a receiver some distance away. While teleportation is commonly portrayed in science fiction as a means to transfer physical objects from one location to the next, quantum teleportation only transfers quantum information. The sender does not have to know the particular quantum state being transferred. Moreover, the location of the recipient can be unknown, but to complete the quantum teleportation, classical information needs to be sent from sender to receiver. Because classical information needs to be sent, quantum teleportation cannot occur faster than the speed of light.

<span class="mw-page-title-main">Quantum entanglement</span> Correlation between quantum systems

Quantum entanglement is the phenomenon of a group of particles being generated, interacting, or sharing spatial proximity in such a way that the quantum state of each particle of the group cannot be described independently of the state of the others, including when the particles are separated by a large distance. The topic of quantum entanglement is at the heart of the disparity between classical and quantum physics: entanglement is a primary feature of quantum mechanics not present in classical mechanics.

Bell's theorem is a term encompassing a number of closely related results in physics, all of which determine that quantum mechanics is incompatible with local hidden-variable theories, given some basic assumptions about the nature of measurement. "Local" here refers to the principle of locality, the idea that a particle can only be influenced by its immediate surroundings, and that interactions mediated by physical fields cannot propagate faster than the speed of light. "Hidden variables" are supposed properties of quantum particles that are not included in quantum theory but nevertheless affect the outcome of experiments. In the words of physicist John Stewart Bell, for whom this family of results is named, "If [a hidden-variable theory] is local it will not agree with quantum mechanics, and if it agrees with quantum mechanics it will not be local."

A Bell test, also known as Bell inequality test or Bell experiment, is a real-world physics experiment designed to test the theory of quantum mechanics in relation to Albert Einstein's concept of local realism. Named for John Stewart Bell, the experiments test whether or not the real world satisfies local realism, which requires the presence of some additional local variables to explain the behavior of particles like photons and electrons. The test empirically evaluates the implications of Bell's theorem. As of 2015, all Bell tests have found that the hypothesis of local hidden variables is inconsistent with the way that physical systems behave.

In the interpretation of quantum mechanics, a local hidden-variable theory is a hidden-variable theory that satisfies the principle of locality. These models attempt to account for the probabilistic features of quantum mechanics via the mechanism of underlying, but inaccessible variables, with the additional requirement that distant events be statistically independent.

<span class="mw-page-title-main">Anton Zeilinger</span> Austrian quantum physicist

Anton Zeilinger is an Austrian quantum physicist and Nobel laureate in physics of 2022. Zeilinger is professor of physics emeritus at the University of Vienna and senior scientist at the Institute for Quantum Optics and Quantum Information of the Austrian Academy of Sciences. Most of his research concerns the fundamental aspects and applications of quantum entanglement.

In quantum information science, the Bell's states or EPR pairs are specific quantum states of two qubits that represent the simplest examples of quantum entanglement. The Bell's states are a form of entangled and normalized basis vectors. This normalization implies that the overall probability of the particle being in one of the mentioned states is 1: . Entanglement is a basis-independent result of superposition. Due to this superposition, measurement of the qubit will "collapse" it into one of its basis states with a given probability. Because of the entanglement, measurement of one qubit will "collapse" the other qubit to a state whose measurement will yield one of two possible values, where the value depends on which Bell's state the two qubits are in initially. Bell's states can be generalized to certain quantum states of multi-qubit systems, such as the GHZ state for three or more subsystems.

Quantum networks form an important element of quantum computing and quantum communication systems. Quantum networks facilitate the transmission of information in the form of quantum bits, also called qubits, between physically separated quantum processors. A quantum processor is a machine able to perform quantum circuits on a certain number of qubits. Quantum networks work in a similar way to classical networks. The main difference is that quantum networking, like quantum computing, is better at solving certain problems, such as modeling quantum systems.

<span class="mw-page-title-main">LOCC</span> Method in quantum computation and communication

LOCC, or local operations and classical communication, is a method in quantum information theory where a local (product) operation is performed on part of the system, and where the result of that operation is "communicated" classically to another part where usually another local operation is performed conditioned on the information received.

<span class="mw-page-title-main">Greenberger–Horne–Zeilinger state</span> "Highly entangled" quantum state of 3 or more qubits

In physics, in the area of quantum information theory, a Greenberger–Horne–Zeilinger state is a certain type of entangled quantum state that involves at least three subsystems. The four-particle version was first studied by Daniel Greenberger, Michael Horne and Anton Zeilinger in 1989, and the three-particle version was introduced by N. David Mermin in 1990. Extremely non-classical properties of the state have been observed, contradicting intuitive notions of locality and causality. GHZ states for large numbers of qubits are theorized to give enhanced performance for metrology compared to other qubit superposition states.

The W state is an entangled quantum state of three qubits which in the bra-ket notation has the following shape

In theoretical physics, quantum nonlocality refers to the phenomenon by which the measurement statistics of a multipartite quantum system do not allow an interpretation with local realism. Quantum nonlocality has been experimentally verified under a variety of physical assumptions. Any physical theory that aims at superseding or replacing quantum theory should account for such experiments and therefore cannot fulfill local realism; quantum nonlocality is a property of the universe that is independent of our description of nature.

<span class="mw-page-title-main">One-way quantum computer</span> Method of quantum computing

The one-way quantum computer, also known as measurement-based quantum computer (MBQC), is a method of quantum computing that first prepares an entangled resource state, usually a cluster state or graph state, then performs single qubit measurements on it. It is "one-way" because the resource state is destroyed by the measurements.

In quantum information and quantum computing, a cluster state is a type of highly entangled state of multiple qubits. Cluster states are generated in lattices of qubits with Ising type interactions. A cluster C is a connected subset of a d-dimensional lattice, and a cluster state is a pure state of the qubits located on C. They are different from other types of entangled states such as GHZ states or W states in that it is more difficult to eliminate quantum entanglement in the case of cluster states. Another way of thinking of cluster states is as a particular instance of graph states, where the underlying graph is a connected subset of a d-dimensional lattice. Cluster states are especially useful in the context of the one-way quantum computer. For a comprehensible introduction to the topic see.

Entanglement distillation is the transformation of N copies of an arbitrary entangled state into some number of approximately pure Bell pairs, using only local operations and classical communication.

<span class="mw-page-title-main">Quantum complex network</span> Notion in network science of quantum information networks

Quantum complex networks are complex networks whose nodes are quantum computing devices. Quantum mechanics has been used to create secure quantum communications channels that are protected from hacking. Quantum communications offer the potential for secure enterprise-scale solutions.

Marek Żukowski is a Polish theoretical physicist and lecturer at the University of Gdańsk. He specializes in quantum mechanics, his area of interest in particular concerns the Bell's theorem and quantum interferometry.

In quantum physics, the "monogamy" of quantum entanglement refers to the fundamental property that it cannot be freely shared between arbitrarily many parties.

Quantum secret sharing (QSS) is a quantum cryptographic scheme for secure communication that extends beyond simple quantum key distribution. It modifies the classical secret sharing (CSS) scheme by using quantum information and the no-cloning theorem to attain the ultimate security for communications.

References

  1. Żukowski, M.; Zeilinger, A.; Horne, M. A.; Ekert, A. K. (27 December 1993). ""Event-ready-detectors" Bell experiment via entanglement swapping". Phys. Rev. Lett. 71: 4287. doi:10.1103/PhysRevLett.71.4287 . Retrieved 1 September 2024.
  2. Ji, Zhaoxu; Fan, Peiru; Zhang, Huanguo. "Entanglement swapping theory and beyond". arxiv.org. Retrieved 1 September 2024.
  3. Shchukin, Evgeny; van Loock, Peter (13 April 2022). "Optimal Entanglement Swapping in Quantum Repeaters". Phys. Rev. Lett. 128: 150502. doi:10.1103/PhysRevLett.128.150502 . Retrieved 1 September 2024.
  4. Lu, Chao-Yang; Yang, Tao; Pan, Jian-Wei (10 July 2009). "Experimental Multiparticle Entanglement Swapping for Quantum Networking". Phys. Rev. Lett. 103 (020501): 1–4. doi:10.1103/PhysRevLett.103.020501 . Retrieved 1 September 2024.
  5. Hu, Xiao-Min; Guo, Yu; Liu, Bi-Heng; Li, Chuan-Feng; Guo, Guang-Can (2023). "Progress in quantum teleportation". Nat. Rev. Phys. 5: 339–353. doi:10.1038/s42254-023-00588-x . Retrieved 1 September 2024.

Further reading