Clifford gates

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. ^[1] Quantum circuits that consist of only Clifford gates can be efficiently simulated with a classical computer due to the Gottesman–Knill theorem.

The Clifford group is generated by three gates: Hadamard, phase gate S, and CNOT. ^{[2] [3] [4]} This set of gates is minimal in the sense that discarding any one gate results in the inability to implement some Clifford operations; removing the Hadamard gate disallows powers of ${\displaystyle {1}/{\sqrt {2}}}$ in the unitary matrix representation, removing the phase gate S disallows ${\displaystyle i}$ in the unitary matrix, and removing the CNOT gate reduces the set of implementable operations from ${\displaystyle \mathbf {C} _{n}}$ to ${\displaystyle \mathbf {C} _{1}^{n}}$. Since all Pauli matrices can be constructed from the phase and Hadamard gates, each Pauli gate is also trivially an element of the Clifford group.

The ${\displaystyle Y}$ gate is equal to the product of ${\displaystyle X}$ and ${\displaystyle Z}$ gates. To show that a unitary ${\displaystyle U}$ is a member of the Clifford group, it suffices to show that for all ${\displaystyle P\in \mathbf {P} _{n}}$ that consist only of the tensor products of ${\displaystyle X}$ and ${\displaystyle Z}$, we have ${\displaystyle UPU^{\dagger }\in \mathbf {P} _{n}}$.

Common generating gates

Hadamard gate

The Hadamard gate

${\displaystyle H={\frac {1}{\sqrt {2}}}{\begin{bmatrix}1&1\\1&-1\end{bmatrix}}}$

is a member of the Clifford group as ${\displaystyle HXH^{\dagger }=Z}$ and ${\displaystyle HZH^{\dagger }=X}$.

S gate

The phase gate

${\displaystyle S={\begin{bmatrix}1&0\\0&e^{i{\frac {\pi }{2}}}\end{bmatrix}}={\begin{bmatrix}1&0\\0&i\end{bmatrix}}={\sqrt {Z}}}$

is a Clifford gate as ${\displaystyle SXS^{\dagger }=Y}$ and ${\displaystyle SZS^{\dagger }=Z}$.

CNOT gate

The CNOT gate applies to two qubits. It is a (C)ontrolled NOT gate, where a NOT gate is performed on qubit 2 if and only if qubit 1 is in the 1 state.

${\displaystyle \mathrm {CNOT} ={\begin{bmatrix}1&0&0&0\\0&1&0&0\\0&0&0&1\\0&0&1&0\end{bmatrix}}.}$

Between ${\displaystyle X}$ and ${\displaystyle Z}$ there are four options:

CNOT combinations

${\displaystyle P}$	CNOT ${\displaystyle P}$ CNOT${\displaystyle ^{\dagger }}$
${\displaystyle X\otimes I}$	${\displaystyle X\otimes X}$
${\displaystyle I\otimes X}$	${\displaystyle I\otimes X}$
${\displaystyle Z\otimes I}$	${\displaystyle Z\otimes I}$
${\displaystyle I\otimes Z}$	${\displaystyle Z\otimes Z}$

Building a universal set of quantum gates

The Clifford gates do not form a universal set of quantum gates as some gates outside the Clifford group cannot be arbitrarily approximated with a finite set of operations. An example is the phase shift gate (historically known as the ${\displaystyle \pi /8}$ gate):

${\displaystyle T={\begin{bmatrix}1&0\\0&e^{i{\frac {\pi }{4}}}\end{bmatrix}}={\sqrt {S}}={\sqrt[{4}]{Z}}}$.

The following shows that the ${\displaystyle T}$ gate does not map the Pauli-${\displaystyle X}$ gate to another Pauli matrix:

${\displaystyle TX{T^{\dagger }}=\left[{\begin{array}{*{20}{c}}1&0\\0&{e^{i{\frac {\pi }{4}}}}\end{array}}\right]\left[{\begin{array}{*{20}{c}}0&1\\1&0\end{array}}\right]\left[{\begin{array}{*{20}{c}}1&0\\0&{e^{-i{\frac {\pi }{4}}}}\end{array}}\right]=\left[{\begin{array}{*{20}{c}}0&{e^{-i{\frac {\pi }{4}}}}\\{e^{i{\frac {\pi }{4}}}}&0\end{array}}\right]\not \in {{\mathbf {P} }_{1}}}$

However, the Clifford group, when augmented with the ${\displaystyle T}$ gate, forms a universal quantum gate set for quantum computation. ^[5] Moreover, exact, optimal circuit implementations of the single-qubit ${\displaystyle Z}$-angle rotations are known. ^{[6] [7]}

See also

• Magic state distillation
• Clifford algebra

References

1. Gottesman, Daniel (1998-01-01). "Theory of fault-tolerant quantum computation" (PDF). Physical Review A . 57 (1): 127–137. arXiv: quant-ph/9702029 . Bibcode:1998PhRvA..57..127G. doi:10.1103/physreva.57.127. ISSN   1050-2947. S2CID   8391036.
2. Nielsen, Michael A.; Chuang, Isaac L. (2010-12-09). Quantum Computation and Quantum Information: 10th Anniversary Edition. Cambridge University Press. ISBN   978-1-107-00217-3.
3. Gottesman, Daniel (1998-01-01). "Theory of fault-tolerant quantum computation". Physical Review A. 57 (1): 127–137. arXiv: quant-ph/9702029 . Bibcode:1998PhRvA..57..127G. doi:10.1103/PhysRevA.57.127. ISSN   1050-2947. S2CID   8391036.
4. Gottesman, Daniel (1997-05-28). Stabilizer Codes and Quantum Error Correction (PhD thesis). Caltech. arXiv: quant-ph/9705052 . Bibcode:1997PhDT.......232G.
5. Forest, Simon; Gosset, David; Kliuchnikov, Vadym; McKinnon, David. "Exact Synthesis of Single-Qubit Unitaries Over Clifford-Cyclotomic Gate Sets". Journal of Mathematical Physics .
6. Ross, Neil J.; Selinger, Peter (2014). "Optimal ancilla-free Clifford+ T approximation of z-rotations". arXiv: 1403.2975 .
7. Kliuchnikov, Vadym; Maslov, Dmitri; Mosca, Michele (2013). "Fast and efficient exact synthesis of single qubit unitaries generated by Clifford and T gates". Quantum Information and Computation. 13 (7–8): 607–630. arXiv: 1206.5236 . doi:10.26421/QIC13.7-8-4. S2CID   12885769.