Skip to main content

Full text of "USPTO Patents Application 08479810"

See other formats


Best Available Copy 

Theory of 
Superconductivity 

By 

M. von LAUE 

Kaiser- Wilhelm-Institut fur physikalische und Elektro-Chemie 
Berlin — Dahlem ' 

Translated by 

LOTHAR METER 

University of Chicago, Chicago, Illinois 

and 

WILLIAM BAND 

The State College of Washington, Pullman, Washington 




ACADEMIC PRESS INC., PUBLISHERS 
New York, 1952 



r 



Best Available Copy 



Chapter i 



aiso 



am 



aw 



am 



Fundamental Facts 

(a) Superconductivity was discovered in 1911 by Kamerlingh-Onnes. 1 
He was the first to liquefy helium and so to produce temperatures below 
10° K. With this new technique he was able to observe the continued 
decrease of the electrical resistance of metals with decreasing temperature. 
With mercury, in contrast to other metals, he was astonished to find that 
the resistance completely vanished, almost discontinuously, at about 4.2° K 
(Fig. 1-1); Today superconductivity is 
.. known in 18 other metals (see Table 
1— 1) whereas in others, e. g.; gold and 
bismuth, the conductivity remains nor- 
mal far below even 1° K. Many alloys 
and compounds ' can also become super- 
conducting, in particular the frequently 
/ \used niobium nitride which has a tran- 
sition temperature as high as 20° K. 
However, among these latter substances 
^ hysteresis phenomena mentioned in the 
% "Introduction*' are so much more strongly 
v evident that in testing the present theory 
we prefer to employ only the "good" 
. superconductors, i. e., the pure elements. 

: ? n tne ^eal case * ne resistance vanishes 

^ completely and discontinuously at a tran- 
sition temperature T $ . Actually the resi- 
stance-temperature curve does fall more 
sharply the more the specimen is like a 
single crystal and the smaller the mea- 
suring current used. < Because the drop 
. always occurs in a measurable tempera - 

^ture* range, the experimental definition 

v:- of the transition temperature is to some 
^extent arbitrary. The temperature at 

; / r which the direct-current resistance reaches one half of the value; it had 

* just before the drop is generally given as the transition temperature, because 
this can be measured accurately. However, a high-frequency investigation 
to be described in Chap. 16 (f) indicates that the foot of the curve where 



aaso 



aozs 



R 9 -i 

















































Fig. 1 — 1. Appearance of supercon- 
ductivity in mercury according to 
H. Kamerlingh-Onnes (1911). The 
ordinate is the resistance R; 
the resistance of solid mercury 
extrapolated to 0° C, is 60 ohms. 



*H. Kamerlingh-Onncs. Commun. Leiden, 120b, J22h, 124c, (1911).