Quantum gate teleportation

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Applying a CNOT gate by using gate teleportation. Uses Bell basis measurement (decomposed here into a CNOT, an H, and two measurements), Bell basis initialization (decomposed here into two resets, an H, and a CNOT), and classical feedback in the form of Pauli operations controlled by the measurement results. Cnot-teleportation.png
Applying a CNOT gate by using gate teleportation. Uses Bell basis measurement (decomposed here into a CNOT, an H, and two measurements), Bell basis initialization (decomposed here into two resets, an H, and a CNOT), and classical feedback in the form of Pauli operations controlled by the measurement results.

Quantum gate teleportation is a quantum circuit construction where a gate is applied to target qubits by first applying the gate to an entangled state and then teleporting the target qubits through that entangled state. [1] [2]

This separation of the physical application of the gate from the target qubit can be useful in cases where applying the gate directly to the target qubit may be more likely to destroy it than to apply the desired operation. For example, the KLM protocol can be used to implement a Controlled NOT gate on a photonic quantum computer, but the process can be prone to errors that destroy the target qubits. By using gate teleportation, the CNOT operation can be applied to a state that can be easily recreated if it is destroyed, allowing the KLM CNOT to be used in long-running quantum computations without risking the rest of the computation. Additionally, gate teleportation is a key component of magic state distillation, a technique that can be used to overcome the limitations of the Eastin-Knill theorem. [3]

Quantum gate teleportation has been demonstrated in various types of quantum computers, including linear optical, [4] superconducting quantum computing, [5] and trapped ion quantum computing. [6]

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

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<span class="mw-page-title-main">Trapped-ion quantum computer</span> Proposed quantum computer implementation

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<span class="mw-page-title-main">Controlled NOT gate</span> Quantum logic gate

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The KLM scheme or KLM protocol is an implementation of linear optical quantum computing (LOQC), developed in 2000 by Emanuel Knill, Raymond Laflamme and Gerard J. Milburn. This protocol makes it possible to create universal quantum computers solely with linear optical tools. The KLM protocol uses linear optical elements, single-photon sources and photon detectors as resources to construct a quantum computation scheme involving only ancilla resources, quantum teleportations and error corrections.

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Optical cluster states are a proposed tool to achieve quantum computational universality in linear optical quantum computing (LOQC). As direct entangling operations with photons often require nonlinear effects, probabilistic generation of entangled resource states has been proposed as an alternative path to the direct approach.

In quantum computing, a qubit is a unit of information analogous to a bit in classical computing, but it is affected by quantum mechanical properties such as superposition and entanglement which allow qubits to be in some ways more powerful than classical bits for some tasks. Qubits are used in quantum circuits and quantum algorithms composed of quantum logic gates to solve computational problems, where they are used for input/output and intermediate computations.

Magic state distillation is a method for creating more accurate quantum states from multiple noisy ones, which is important for building fault tolerant quantum computers. It has also been linked to quantum contextuality, a concept thought to contribute to quantum computers' power.

In quantum computing and quantum information theory, the Clifford gates are the elements of the Clifford group, a set of mathematical transformations which normalize the n-qubit Pauli group, i.e., map tensor products of Pauli matrices to tensor products of Pauli matrices through conjugation. The notion was introduced by Daniel Gottesman and is named after the mathematician William Kingdon Clifford. Quantum circuits that consist of only Clifford gates can be efficiently simulated with a classical computer due to the Gottesman–Knill theorem.

The Eastin–Knill theorem is a no-go theorem that states: "No quantum error correcting code can have a continuous symmetry which acts transversely on physical qubits". In other words, no quantum error correcting code can transversely implement a universal gate set, where a transversal logical gate is one that can be implemented on a logical qubit by the independent action of separate physical gates on corresponding physical qubits.

This glossary of quantum computing is a list of definitions of terms and concepts used in quantum computing, its sub-disciplines, and related fields.

References

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