-
8
-
-
4243423159
-
-
(1988)
Phys. Rev. Lett.
, vol.61
, pp. 1313
-
-
Thomas, G.A.1
Orenstein, J.2
Rapkine, D.H.3
Capizzi, M.4
Millis, A.J.5
Bhatt, R.N.6
Schneemeyer, L.F.7
Waszczak, J.V.8
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9
-
-
3342975864
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In a clean high-Tcsuperconductor you do not see the gap
-
(1990)
Physical Review Letters
, vol.64
, pp. 84
-
-
Kamaras, K.1
Herr, S.L.2
Porter, C.D.3
Tache, N.4
Tanner, D.B.5
Etemad, S.6
Venkatesan, T.7
Chase, E.8
Inam, A.9
Wu, X.D.10
Hegde, M.S.11
Dutta, B.12
-
10
-
-
33845734025
-
-
(1990)
Phys. Rev. Lett.
, vol.64
, pp. 1692E
-
-
Kamaras, K.1
Herr, S.L.2
Porter, C.D.3
Tache, N.4
Tanner, D.B.5
Etemad, S.6
Venkatesan, T.7
Chase, E.8
Inam, A.9
Wu, X.D.10
Hegde, M.S.11
Dutta, B.12
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21
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84927410728
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This relies on the assumption that the plane contribution to σ ( ω ) is isotropic, which is reasonable since the plane Cu-O bond lengths in the a bhat and b bhat directions are virtually identical (the 2% lattice constant difference is associated with buckling).
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22
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84927410727
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If one assumes that the chain and plane band masses are roughly equal (as would be the case if both are dominated by the oxygen bandwidth), then this result implies app 0.5 – 0.6 hole per chain Cu, and 0.25–0.2 hole per plane Cu (total of 1 hole per unit cell).
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