| 释义 |
Ginzburg-London superconductivity theory 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. |