Category:Few-Qubits Fault Tolerant Quantum Computing Network Stage: Difference between revisions

From Quantum Protocol Zoo
Jump to navigation Jump to search
No edit summary
No edit summary
Line 1: Line 1:
The fifth network stage differs from the earlier ([[:Category:Quantum Memory Network Stage|Quantum Memory]]) stage by demanding that the local operations can be performed fault-tolerantly (without any error), which is considerably more challenging. The devices on the
The fifth network stage differs from the earlier ([[:Category:Quantum Memory Network Stage|Quantum Memory]]) stage by demanding that the local operations can be performed fault-tolerantly (without any error), which is considerably more challenging.The devices on the end nodes are not full fedged quantum computers but a smaller version of the same with fewer qubits than what is required to show quantum supremacy or efficiently do better than a classical computer. Fault tolerance implies that all error parameters of a quantum memory network can be made negligible by adding more resources. Here the number of qubits available is small enough such that the end nodes can be simulated effectively on a classical computer. Here, the main interest is the performance of the fault-
network are full  
tolerant scheme. However, this does not imply that the entire network can be simulated efficiently or that there would exist equivalent classical protocols; the effect of entanglement cannot generally be replicated classically.<br/>
edged quantum computers and able to carry out error cor-
==Application==
rection on data transfers.
Having access to fault-tolerant gates allows higher-accuracy clock synchronization (3) and protocols that require many rounds of communication and high circuit depth to be useful. This includes distributed quantum computing as well as applications for full-scale quantum computing networks, restricted to few qubits. This could be of great practical interest, especially for applica-
Fault-tolerant operations being available would allow the execution of local
tions in the domain of distributed systems.
quantum computation of high circuit depth as well as an arbitrary extension
==Relevant Parameters==
of storage times to execute protocols with an arbitrary number of rounds of
communication. Fault tolerance implies that all error parameters of a quantum
memory network can be made negligible by adding more resources.
The term few qubits here refers to the fact that the number of qubits avail-
able is small enough so that the end nodes can be simulated e�ectively on a
classical computer. Here, the main interest is the performance of the fault-
tolerant scheme, This does not imply that the entire network can be simulated
e�ciently or that there would exist equivalent classical protocols; the e�ects
of entanglement cannot generally be replicated classically.
Applications:
Having access to fault-tolerant gates allows higher-accuracy clock synchro-
nization (3) and protocols that require many rounds of communication and
high circuit depth to be useful. This includes distributed quantum computing
as well as applications for full-scale quantum computing networks, restricted
to few qubits. This could be of great practical interest, especially for applica-
tions in the domain of distributed systems, but as with the implementation of
quantum algorithms on quantum computers, the power of having only a lim-
ited number of qubits at our disposal is an important subject of investigation
 
[[Category:Network Stages]]
[[Category:Network Stages]]

Revision as of 01:00, 11 July 2019

The fifth network stage differs from the earlier (Quantum Memory) stage by demanding that the local operations can be performed fault-tolerantly (without any error), which is considerably more challenging.The devices on the end nodes are not full fedged quantum computers but a smaller version of the same with fewer qubits than what is required to show quantum supremacy or efficiently do better than a classical computer. Fault tolerance implies that all error parameters of a quantum memory network can be made negligible by adding more resources. Here the number of qubits available is small enough such that the end nodes can be simulated effectively on a classical computer. Here, the main interest is the performance of the fault- tolerant scheme. However, this does not imply that the entire network can be simulated efficiently or that there would exist equivalent classical protocols; the effect of entanglement cannot generally be replicated classically.

Application

Having access to fault-tolerant gates allows higher-accuracy clock synchronization (3) and protocols that require many rounds of communication and high circuit depth to be useful. This includes distributed quantum computing as well as applications for full-scale quantum computing networks, restricted to few qubits. This could be of great practical interest, especially for applica- tions in the domain of distributed systems.

Relevant Parameters

This category currently contains no pages or media.