Quantum theory Quantum computation and error correction Theorem
Quantum threshold theorem
Builds on Quantum circuitQuantum error correctionStabilizer code
Statement
Consider quantum circuits built from four kinds of operations: one- and two-qubit gates, preparations of fresh qubits in , measurements and idle steps. Any number of operations may act in parallel, and fast classical computation is free. Assume local stochastic noise of strength : each operation fails independently with probability at most . A failed operation is replaced by an arbitrary quantum operation on the same qubits. Then there is a constant , the threshold, with the following property. If , then for every ideal circuit with operations and every there is a circuit with operations. Under the noise, the output distribution of is within total variation distance of the output distribution of without noise.
Remarks
Proof idea: encode each qubit in a quantum error-correcting code and replace each operation by a fault-tolerant gadget that does not spread a single fault into an uncorrectable error. Then a level- logical operation fails with probability at most for a constant . Concatenating the code times gives logical failure probability at most with . So the error falls doubly exponentially in while the size grows only exponentially in , which gives the polylogarithmic overhead.
The hypothesis of fresh qubits is needed: error correction removes entropy from the computer, and without a supply of fresh qubits the entropy builds up and long computations fail. The parallelism is needed so that errors can be corrected on all qubits at every time step.
Example: with stabilizer codes such as surface codes, numerical studies estimate thresholds of the order of for some noise models.
Going deeper
For a student
The theorem was proved independently in the late 1990s by Aharonov and Ben-Or, by Kitaev, and by Knill, Laflamme and Zurek. It is the quantum analogue of von Neumann's theorem on reliable computation with unreliable components. The value of depends on the noise model, the code and the gadgets, and the rigorous lower bounds are far below the numerical estimates. The theorem also holds for some correlated noise models with suitably decaying correlations.
Reading path
To understand this page from the ground up, read these 4 pages in order. The foundations come first.
Show the path as a graph
- no evidence level
- Quantum circuit concept
- Quantum error correction concept
- Stabilizer code concept
- Quantum threshold theorem statement
Further reading
About this page
| Tag | QSXW37V7XV |
|---|---|
| URI | m2://QSXW37V7XV |
| Kind | statement, theorem |
| Writing | W0 stub |
| MSC | 81P73, 68Q12, 81P68 |
| Status | This copy of the site has no build data. Run m2 status QSXW37V7XV. |
| About | Quantum error correction, Quantum circuit |
| Uses | Quantum circuit, Quantum error correction, Stabilizer code |
| Same as | |
| Changed | 3 November 2026 |
Markdown · JSON · Edit on GitHub
What this page needs for W1
- an inventory row: the row of the inventory that the node accounts for (0 of 1)
- a source with a locator (0 of 1)
The writing levels say how complete the text of a page is. They do not measure its truth.
What links here
No page links to this page yet.