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PDF (double-sided) - Physics Department, UCSB - University of ...

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Figure 9.3: Spectroscopy <strong>of</strong> Coupled Qubits – a) Far <strong>of</strong>f: Initially the flux bias<br />

crosstalk will probably place the qubits <strong>of</strong>f resonance. b) Closer: As the flux bias<br />

is corrected, the resonance peaks move closer. c) Splitting: When the qubits are<br />

on resonance, the coupling causes them to split.<br />

one-dimensional spectroscopy scan introduced above. If it is run on all qubits<br />

simultaneously, it will show each qubit’s resonance peak in the presence <strong>of</strong> all<br />

other qubits’ biases. If the operating biases <strong>of</strong> all qubits are then adjusted to set<br />

the resonance frequency <strong>of</strong> all qubits to the same value, the qubits will begin to<br />

couple. This can sometimes be seen in a splitting <strong>of</strong> the response peak in the<br />

spectroscopy sweep, as shown in Figure 9.3c.<br />

9.2.3 Swaps<br />

The next step is to examine the time dynamics from the qubits’ interaction.<br />

This can be achieved with a sweep that is essentially a multi-qubit T 1 experiment,<br />

except that only one <strong>of</strong> the involved qubits is prepared in the | 1 〉-state with a<br />

π-pulse, while all other qubits remain in the ground state.<br />

In addition to the<br />

209

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