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| author | Eugeniy Mikhailov <evgmik@gmail.com> | 2014-10-07 10:49:04 -0400 |
|---|---|---|
| committer | Eugeniy Mikhailov <evgmik@gmail.com> | 2014-10-07 10:54:29 -0400 |
| commit | fd5f7a7cc884041111bd9b88803a136672020802 (patch) | |
| tree | bc842e21de94da85c94a3904db0d69f2d2d2bd49 /supcon.tex | |
| parent | bad17babb14116b702c87e967b067bca973a92c5 (diff) | |
| download | manual_for_Experimental_Atomic_Physics-fd5f7a7cc884041111bd9b88803a136672020802.tar.gz manual_for_Experimental_Atomic_Physics-fd5f7a7cc884041111bd9b88803a136672020802.zip | |
quotation typo fixed
Diffstat (limited to 'supcon.tex')
| -rw-r--r-- | supcon.tex | 2 |
1 files changed, 1 insertions, 1 deletions
@@ -25,7 +25,7 @@ between a metal and insulator: while it has a full band (the valence band), the next band (the conduction band) is close enough in energy and so that the electrons can easily reach it. Superconductors are in a class by themselves. They can be metals or insulators at room temperature. Below a certain -temperature, called the critical temperature, the electrons "pair" together (in +temperature, called the critical temperature, the electrons ``pair'' together (in Cooper pairs) and travel through the solid without resistance. Current in a superconductor below the critical temperature will travel indefinitely without dissipation. |