ABSTRACT
In Sections 1.4, 3.3, 4.3 and 6.3, we have briefly discussed the “secondary” quantum macroscopic effects arising in very small Josephson junctions at low temperatures. It has been shown that these effects can be observed if the energy quantum ℏωA corresponding to the attempt frequency (3.45) ()https://www.w3.org/1998/Math/MathML">ωA≈ min [ωp,ωc]https://s3-euw1-ap-pe-df-pch-content-public-p.s3.eu-west-1.amazonaws.com/9781315141572/0ba78ca1-05bc-4a29-bdf3-856e8fbc4b17/content/eq1736.tif" xmlns:xlink="https://www.w3.org/1999/xlink"/>
