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. 2013 Jun 13;3:1987. doi: 10.1038/srep01987

Figure 2. Mode profiles and frequency spectrum in the divided cavity.

Figure 2

(a) The mode profile of the lowest-energy cavity mode, calculated using Eq. (4), with a flux through the SQUIDs of (i) Φ = 0.35Φ0, (ii) Φ = 0.28Φ0, and (iii) Φ = 0.14Φ0. (b) The frequencies of the two lowest modes, calculated from Eq. (6), as functions of the bare left-cavity frequency to give the spectrum in the frequency range around the left-right cavity resonance. The first and second modes, for the flux values considered in (a), are marked with squares and circles, respectively. For the cavity parameters, we take a cavity of length L = 12 mm, and a capacitor positioned at xc = 0.45 L, with capacitance Cc = 0.5 fF. We introduce ns SQUIDs, each with a critical current Ic0 = 0.3 μA × ns, into the left side of the cavity. For the center conductor, c = 130 × 10−12 Fm−1, and we take the inductance per unit length of the right cavity region to be R = 3.25 × 10−7 Hm−1, resulting in a characteristic impedance Inline graphic. For these parameters, the bare right-cavity frequency has a value Inline graphic, and the interaction frequency is Inline graphic.