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• Codes, i.e. interesting subspaces of H ⊗n . To make quantum computing fault tolerant,<br />
these subspaces should have special properties. In particular, in a physical realization,<br />
the dynamics of the system should suppress errors.<br />
• Unitary operators acting on H ⊗n that preserve these subspaces.<br />
5.5.4 Quantum gates<br />
First let us discuss quantum gates: for quantum computation, we need unitary operators H ⊗n →<br />
H ⊗n to be realized by some time evolution. Unitarity implies reversibility.<br />
Definition 5.5.9<br />
1. A quantum gate on H ⊗n is a unitary map H ⊗n → H ⊗n that acts as the identity on at<br />
least n − 2 tensorands.<br />
2. Consider a fixed finite set {U i } i∈I of quantum gates, i.e. U i ∈ U(H) or U i ∈ U(H ⊗ H),<br />
called a library of quantum gates. Denote by U αβ<br />
i the gate U i acting on the α and β<br />
tensorand resp. Ui<br />
α acting on the α tensorand of H n . A quantum circuit based on this<br />
library is a finite product of Ui<br />
α and U αβ<br />
i . It is a unitary endomorphism of H ⊗n .<br />
3. A library of quantum gates is called universal, if for any n, the subgroup of U(H ⊗n )<br />
generated by all circuits is dense.<br />
Examples 5.5.10.<br />
1. An important examples of a gate is the CNOT gate (controlled not gate) which acts on<br />
two qubits: H ⊗2 → H ⊗2 . The CNOT gate flips the second qubit (the target qubit) if and<br />
only if the first qubit (the control qubit) is 1. Here we write 1 = | ↑〉 and 0 = | ↓〉.<br />
Before<br />
After<br />
Control Target Control Target<br />
0 0 0 0<br />
0 1 0 1<br />
1 0 1 1<br />
1 1 1 0<br />
The resulting value of the second qubit corresponds to the result of a classical XOR gate<br />
while the control qubit is unchanged.<br />
An experimental realization of the CNOT gate was afforded by a single Beryllium ion<br />
in a trap in 1995 with a reliability of 90%. The two qubits were encoded into an optical<br />
state and into the vibrational state of the ion.<br />
2. The relative phase gate H → H acting on one qubit, a popular choice of which is in the<br />
selected basis | ↑〉, | ↓〉: ( )<br />
1 0<br />
0 exp(2πi/5)<br />
Similarly, the three Pauli matrices give rise to so-called Pauli gates acting on a single<br />
qubit.<br />
3. The library consisting of the CNOT gate and the relative phase gate can be shown to be<br />
universal.<br />
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