Can Anyone Simplify the BCS Theory of Superconductivity?

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BCS theory of superconductivity explains how electrons, which are fermions, can pair up and behave like bosons under certain conditions. This pairing occurs through indirect coupling with lattice phonons, allowing two electrons to attract each other despite their like charges. As a result, these paired electrons form a new entity that follows Bose-Einstein statistics, enabling them to flow without resistance. The process is facilitated by low temperatures, where lattice vibrations create dipoles that help couple the electrons. Overall, BCS theory illustrates the transition to superconductivity through electron pairing and lattice interactions.
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I just don't get it, would anyone care to simplify the BCS theory for me? Please?
 
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electrons are fermions (spin 1/2), they don't like to be in the same state as each other. Boson (spin 1,2...) on the other hand, like to be with each other. The whole point of BCS is that electrons couple with each other indirectly through coupling with the lattice phonon (vibration of lattice). What you have are (effectively) two electron trying to "attract" each other even though they have like charges. Since each has 1/2 spin, the coupled particle has spin 1 (or 0). Now the new e-e "particle" obeys Bose-Einstein statistic, and flow like an ideal fluid, hence superconductivity.

I'd like to imagine this coupling as following: When you don't have much lattice kinetic energy (hence low temp), a vibrating lattice site (positive ion) pulls away from its electron, forming a dipole, and the positive end of this dipole attracts the electron of the next side, which effectively couple the two electrons together.

This is my 2 cents about BCS.
 
Thread 'Unexpected irregular reflection signal from a high-finesse cavity'

Thread 'Unexpected irregular reflection signal from a high-finesse cavity'

I am observing an irregular, aperiodic noise pattern in the reflection signal of a high-finesse optical cavity (finesse ≈ 20,000). The cavity is normally operated using a standard Pound–Drever–Hall (PDH) locking configuration, where an EOM provides phase modulation. The signals shown in the attached figures were recorded with the modulation turned off. Under these conditions, when scanning the laser frequency across a cavity resonance, I expected to observe a simple reflection dip. Instead...
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