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An explanation for a universality of transition temperatures in families of copper oxide superconductors
A remarkable mystery of the copper oxide high-transition-temperature ( T c ) superconductors is the dependence of T c on the number of CuO 2 layers, n , in the unit cell of a crystal. In a given family of these superconductors, T c rises with the number of layers, reaching a peak at n = 3, and then...
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Published in: | Nature (London) 2004-03, Vol.428 (6978), p.53-55 |
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Main Authors: | , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | A remarkable mystery of the copper oxide high-transition-temperature (
T
c
) superconductors is the dependence of
T
c
on the number of CuO
2
layers,
n
, in the unit cell of a crystal. In a given family of these superconductors,
T
c
rises with the number of layers, reaching a peak at
n
= 3, and then declines
1
: the result is a bell-shaped curve. Despite the ubiquity of this phenomenon, it is still poorly understood and attention has instead been mainly focused on the properties of a single CuO
2
plane. Here we show that the quantum tunnelling of Cooper pairs between the layers
2
simply and naturally explains the experimental results, when combined with the recently quantified charge imbalance of the layers
3
and the latest notion of a competing order
4
,
5
,
6
,
7
,
8
,
9
nucleated by this charge imbalance that suppresses superconductivity. We calculate the bell-shaped curve and show that, if materials can be engineered so as to minimize the charge imbalance as
n
increases,
T
c
can be raised further. |
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ISSN: | 0028-0836 1476-4687 |
DOI: | 10.1038/nature02348 |