ABSTRACT

We will start our consideration of the microwave signal influence upon the Josephson junction with the simplest case of a small signal. According to the discussion of Section 2.4, the signal is represented by an ac current Ĩ(t) with sufficiently small amplitude Iω (the exact conditions on the amplitude will be specified later). For the small signal, one can expand its effects to the Taylor series with respect to Iω and consider consequently the linear (∝ Iω), quadratic https://www.w3.org/1998/Math/MathML">(∝ Iω2)https://s3-euw1-ap-pe-df-pch-content-public-p.s3.eu-west-1.amazonaws.com/9781315141572/0ba78ca1-05bc-4a29-bdf3-856e8fbc4b17/content/eq920.tif" xmlns:xlink="https://www.w3.org/1999/xlink"/> and higher-order effects. The first-order (linear) effects are, of course, the most significant ones at Iω → 0.