Magic state distillation
Magic state distillation is a method for creating more accurate quantum states from multiple noisy ones, which is important[1] for building fault tolerant quantum computers. It has also been linked[2] to quantum contextuality, a concept thought to contribute to quantum computers' power.[3]
The technique was first proposed by Emanuel Knill in 2004,[4] and further analyzed by Sergey Bravyi and Alexei Kitaev the same year.[5]
Thanks to the Gottesman–Knill theorem, it is known that some quantum operations (operations in the Clifford algebra) can be perfectly simulated in polynomial time on a probabilistic classical computer. In order to achieve universal quantum computation, a quantum computer must be able to perform operations outside this set. Magic state distillation achieves this, in principle, by concentrating the usefulness of imperfect resources, represented by mixed states, into states that are conducive for performing operations that are difficult to simulate classically.
A variety of qubit magic state distillation routines[6][7] and distillation routines for qubits[8][9][10] with various advantages have been proposed.
Stabilizer formalism
The Clifford group consists of a set of [math]\displaystyle{ n }[/math]-qubit operations generated by the gates {H, S, CNOT} (where H is Hadamard and S is [math]\displaystyle{ \begin{bmatrix} 1 & 0 \\ 0 & i \end{bmatrix} }[/math]) called Clifford gates. The Clifford group generates stabilizer states which can be efficiently simulated classically, as shown by the Gottesman–Knill theorem. This set of gates with a non-Clifford operation is universal for quantum computation.[5]
Magic states
Magic states are purified from [math]\displaystyle{ n }[/math] copies of a mixed state [math]\displaystyle{ \rho }[/math].[6] These states are typically provided via an ancilla to the circuit. A magic state for the [math]\displaystyle{ T }[/math] gate is [math]\displaystyle{ |M\rangle = \cos(\beta/2)|0\rangle + e^{i\frac{\pi}{4}}\sin(\beta/2)|1\rangle }[/math] where [math]\displaystyle{ \beta = \arccos\left(\frac{1}{\sqrt 3}\right) }[/math]. By combining (copies of) magic states with Clifford gates, can be used to make a non-Clifford gate.[5] Since Clifford gates combined with a non-Clifford gate are universal for quantum computation, magic states combined with Clifford gates are also universal.
Purification algorithm for distilling |M〉
The first magic state distillation algorithm, invented by Sergey Bravyi and Alexei Kitaev, is a follows.[5]
- Input: Prepare 5 imperfect states.
- Output: An almost pure state having a small error probability.
- repeat
- Apply the decoding operation of the five-qubit error correcting code and measure the syndrome.
- If the measured syndrome is [math]\displaystyle{ |0000\rangle }[/math], the distillation attempt is successful.
- else Get rid of the resulting state and restart the algorithm.
- until The states have been distilled to the desired purity.
References
- ↑ Campbell, Earl T.; Terhal, Barbara M.; Vuillot, Christophe (14 September 2017). "Roads towards fault-tolerant universal quantum computation". Nature 549 (7671): 172–179. doi:10.1038/nature23460. PMID 28905902. Bibcode: 2017Natur.549..172C. http://eprints.whiterose.ac.uk/121343/1/1612.07330.pdf.
- ↑ Howard, Mark; Wallman, Joel; Veitch, Victor; Emerson, Joseph (11 June 2014). "Contextuality supplies the 'magic' for quantum computation". Nature 510 (7505): 351–355. doi:10.1038/nature13460. PMID 24919152. Bibcode: 2014Natur.510..351H.
- ↑ Bartlett, Stephen D. (11 June 2014). "Powered by magic". Nature 510 (7505): 345–347. doi:10.1038/nature13504. PMID 24919151.
- ↑ Knill, E. (2004). Fault-Tolerant Postselected Quantum Computation: Schemes. Bibcode: 2004quant.ph..2171K.
- ↑ 5.0 5.1 5.2 5.3 Bravyi, Sergey; Kitaev, Alexei (2005). "Universal quantum computation with ideal Clifford gates and noisy ancillas". Physical Review A 71 (2): 022316. doi:10.1103/PhysRevA.71.022316. Bibcode: 2005PhRvA..71b2316B.
- ↑ 6.0 6.1 Bravyi, Sergey; Haah, Jeongwan (2012). "Magic state distillation with low overhead". Physical Review A 86 (5): 052329. doi:10.1103/PhysRevA.86.052329. Bibcode: 2012PhRvA..86e2329B.
- ↑ Meier, Adam; Eastin, Bryan; Knill, Emanuel (2013). "Magic-state distillation with the four-qubit code". Quantum Information & Computation 13 (3–4): 195–209. doi:10.26421/QIC13.3-4-2.
- ↑ Campbell, Earl T.; Anwar, Hussain; Browne, Dan E. (27 December 2012). "Magic-State Distillation in All Prime Dimensions Using Quantum Reed-Muller Codes". Physical Review X 2 (4): 041021. doi:10.1103/PhysRevX.2.041021. Bibcode: 2012PhRvX...2d1021C.
- ↑ Campbell, Earl T. (3 December 2014). "Enhanced Fault-Tolerant Quantum Computing in d -Level Systems". Physical Review Letters 113 (23): 230501. doi:10.1103/PhysRevLett.113.230501. PMID 25526106. Bibcode: 2014PhRvL.113w0501C. https://refubium.fu-berlin.de/handle/fub188/17541.
- ↑ Prakash, Shiroman (September 2020). "Magic state distillation with the ternary Golay code". Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences 476 (2241): 20200187. doi:10.1098/rspa.2020.0187. PMID 33071576. Bibcode: 2020RSPSA.47600187P.
Original source: https://en.wikipedia.org/wiki/Magic state distillation.
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