Ginzburg-London superconductivity theory

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Ginzburg-London superconductivity theory [′ginz·bərg ′lən·dən ′sü·pər‚kän‚dək′tiv·əd·ē ‚thē·ə·rē]

(solid-state physics)

A modification of the London superconductivity theory to take into account the boundary energy.

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