28.04.2014 Views

pdf file

pdf file

pdf file

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

• 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 />

143

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!