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This effect is most likely attributed to a power-dependent shift of the cavity resonance medicine 8 capital rocka trusted haldol 10mg. The increased Stark drive treatment eating disorders cheap haldol 1.5 mg, despite being off-resonant from the cavity medications hyperkalemia quality 5mg haldol, will at large enough powers begin to Stark shift the cavity frequency medications zoloft proven 5 mg haldol, such that the transmission of the measurement drive which is locked to the starting cavity frequency is reduced during the experiment. The interaction is coherent and effectively switchable, as evidenced by the avoided crossing in spectroscopy and the ability to coherently swap in the time-domain. Furthermore, the coupling is long range and could possibly be extended to non-nearest neighbors. The direct improvements which are necessary to take a leap ahead towards generating and detecting entangled states are improved coherence times and an improved method of turning on and off the interaction. The coherence times of the sample studied in this experiment were multi-mode Purcell limited []. By reducing the cavity linewidth, the loss of polarization via spontaneous emission would be reduced. Furthermore, although the Stark shift is a creative way of turning the qubit-qubit interaction on and off, a better option would be to directly tune the flux, which we can hope to achieve with high-bandwidth on-chip flux bias. In the previous chapter (chapter 7), we demonstrated the first steps towards entangling two superconducting qubits via a cavity bus. Furthermore, we could see the possibility to employ the same bus which provides the interaction to act as a multiplexed readout of the two qubit quantum state. However, the accurate and reliable detection of such quantum states and their degree of entanglement is itself a major necessity and nontrivial problem for quantum information systems. In any experiment one obtains information about the quantum system only through 187 entanglement and joint readout the observation of the output from a detector, whose classical imperfections can introduce bias and noise. As a result, to make precise statements about intrinsic properties of quantum states, such as entanglement or purity (section 2. In traditional quantum information processing architectures, such as those employing photons or trapped ions, the relationship between a quantum state and the quantities measured has been well established. In addition, the fidelity of single-shot measurements can in such cases be very high (. However, in the context of solid-state systems, the details of the measurement process itself are not fully understood and are an area of active research and recent progress. Single-shot individual qubit measurements have been technically challenging, and the readout fidelity is not yet as high as the fidelity of qubit operations (- % for single-qubit gates [,]). Each individual readout channel can provide an additional path for decoherence and must also be calibrated. An example of the need for calibration is measurement cross-talk, which can be significant in circuit-based architectures [], but has now been suppressed to the. Recently, the single-shot fidelity of independent readouts of superconducting qubits has also been improved [,] to %. In the last chapter (chapter 7) we observed the first steps towards using the cavity as a joint qubit state detector. The coherence times in that experiment were unfortunately too low for the generating high purity separable and entangled states. In this chapter, we will show the full calibration and characterization of our joint detector and place bounds of % on systematic deviations from the ideal joint measurement (section 8. This is similar to determining the systematic errors, such as cross-talk [], in individual readouts. We then employ the joint detector for two qubits to perform quantum state tomography for both separable states as well as highly entangled states, generated using the cavity bus two transmon interaction (section 8. Furthermore, we demonstrate a high degree of entanglement by measuring a large violation of a Clauser-Horne-Shimony-Holt inequality [] in a solid-state system, with a value of. The cavity, normally off-resonance with the qubit transition frequencies fL and fR, couples the qubits by virtual photon exchange and shields them from the electromagnetic continuum. As previously discussed in chapter 7, microwave pulses resonant with fL or fR applied to the cavity input port provide frequency-multiplexed single-qubit x- and y-rotations with high fidelity [] and selectivity []. The remaining two ports create local magnetic fields that tune the qubit transition frequencies. Each qubit has a split-pair of Josephson junctions, so its frequency is flux-tunable. Static tuning of qubit transitions using the flux-bias lines is demonstrated in figure 8.

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