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Supplementary Information: Difference between revisions
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===Graph states=== | ===Graph states=== | ||
The above operation can also be viewed as a graph state with two nodes and one edge. The qubit 1 is measured in a rotated basis <math>\mathrm{HZ}(\theta)</math>, thus leaving qubit 2 in desired state and Pauli Correction <math>\mathrm{X}^|\mathrm{s1}\rangle \mathrm{HZ}(\theta_1)|\psi\rangle</math>, where <math>\mathrm{s1}</math> is the measurement outcome of qubit 1. See | The above operation can also be viewed as a graph state with two nodes and one edge. The qubit 1 is measured in a rotated basis <math>\mathrm{HZ}(\theta)</math>, thus leaving qubit 2 in desired state and Pauli Correction <math>\mathrm{X}^|\mathrm{s1}\rangle \mathrm{HZ}(\theta_1)|\psi\rangle</math>, where <math>\mathrm{s1}</math> is the measurement outcome of qubit 1. See [[Supplementary Information#3|Figure 3]]<br/> | ||
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[[File:Graph States for Single Qubit States.jpg|center|thumb|1000px|Figure 3: Graph State for Single Qubit Gates]]</div> | [[File:Graph States for Single Qubit States.jpg|center|thumb|1000px|Figure 3: Graph State for Single Qubit Gates]]</div> | ||