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Lecture 5
Josephson Effects
•Quasi-particle Tunneling
•Pair Tunneling and weak Links
•SIS Josephson Junctions
•Superconducting Quantum
Interference Devices (SQUIDS)
Lecture 5 josephson effects
Lecture 5 josephson effects
Quasi-Particle Tunneling
Lecture 5 josephson effects
Lecture 5 josephson effects
Lecture 5 josephson effects
Lecture 5 josephson effects
Lecture 5 josephson effects
Lecture 5 josephson effects
Lecture 5 josephson effects
Lecture 5 josephson effects
Lecture 5 josephson effects
Lecture 5 josephson effects
Lecture 5 josephson effects
Lecture 5 josephson effects
Lecture 5 josephson effects
Lecture 5 josephson effects
Lecture 5 josephson effects
Lecture 5 josephson effects
Lecture 5 josephson effects
Lecture 5 josephson effects
Lecture 5 josephson effects
Lecture 5 josephson effects
Josephson effect
(see also hand-out)
In 1962 Josephson predicted Cooper-pairs can tunnel
through a weak link at zero voltage difference. Current in
junction (called Josephson junction – Jj) is then equal to:
 21sin   cJJ
Electrical current flows between two SC
materials - even when they are separated by
a non-SC or insulator. Electrons "tunnel"
through this non-SC region, and SC current
flows.
Lecture 5 josephson effects
Lecture 5 josephson effects
Lecture 5 josephson effects
Lecture 5 josephson effects
Lecture 5 josephson effects
Lecture 5 josephson effects
Lecture 5 josephson effects
Lecture 5 josephson effects
Lecture 5 josephson effects
Superconducting Quantum
Interference Devices-
SQUIDS
Lecture 5 josephson effects
Lecture 5 josephson effects
Lecture 5 josephson effects
Lecture 5 josephson effects
Lecture 5 josephson effects
Lecture 5 josephson effects

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Lecture 5 josephson effects