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Table 11.1: Entangled State Density Matrix – Raw<br />

ρ raw | 00 〉 | 01 〉 | 10 〉 | 11 〉<br />

| 00 〉 0.151 −0.005 + 0.034i 0.041 + 0.034i −0.003 + 0.005i<br />

| 01 〉 −0.005 − 0.034i 0.369 −0.380 − 0.000i −0.030 − 0.012i<br />

| 10 〉 0.041 − 0.034i −0.380 + 0.000i 0.428 −0.004 − 0.054i<br />

| 11 〉 −0.003 − 0.005i −0.030 + 0.012i −0.004 + 0.054i 0.051<br />

Table 11.2: Entangled State Density Matrix – Corrected for Visibilities<br />

ρ corr | 00 〉 | 01 〉 | 10 〉 | 11 〉<br />

| 00 〉 0.135 −0.006 + 0.040i 0.046 + 0.037i −0.003 + 0.006i<br />

| 01 〉 −0.006 − 0.040i 0.387 −0.431 + 0.000i −0.034 − 0.015i<br />

| 10 〉 0.046 − 0.037i −0.431 − 0.000i 0.449 −0.004 − 0.061i<br />

| 11 〉 −0.003 − 0.006i −0.034 + 0.015i −0.004 + 0.061i 0.029<br />

the fact that the pulses that sweep the first qubit <strong>of</strong>f and the second qubit on<br />

resonance also cause Z-rotations.<br />

11.1.4 Verifying Entanglement – State Tomography<br />

At this point, for either coupling scheme, the qubit pair should be prepared<br />

in a highly entangled state similar to the Bell singlet. To verify the quality <strong>of</strong> the<br />

created state, one can employ a technique called “Quantum State Tomography”<br />

244

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