Verification of Nodeless Superconducting Pairing in Single-Crystal YBa2Cu3O7

2003 ◽  
Vol 17 (18n20) ◽  
pp. 3582-3593 ◽  
Author(s):  
Dale R. Harshman ◽  
W. J. Kossler ◽  
X. Wan ◽  
A. T. Fiory ◽  
A. J. Greer ◽  
...  

The temperature and field dependence of the penetration depth was determined from muon spin rotation (μ+ SR ) measurements on a single crystal of YBa 2 Cu 3 O 7 having a superconducting transition at Tc ≈ 91.3 K . Data were acquired at applied magnetic fields of 0.05, 1.0, 3.0, and 6.0 Tesla, yielding results inconsistent with any pairing state requiring nodes, including d-wave pairing. These data are, however, completely consistent with s-wave (or extended s-wave) superconductivity, with clear evidence of field-dependent, temperature-activated vortex pinning. Our results confirm the s-wave character originally observed in 1989, and show that the features of μ+ SR (and microwave) data used by other authors as evidence for d-wave superconductivity are instead due to temperature- and field-dependent vortex pinning/reordering, resulting in significant distortion of the flux lattice.

2020 ◽  
Vol 5 (3) ◽  
pp. 50
Author(s):  
Rustem Khasanov ◽  
Alexander Shengelaya ◽  
Roland Brütsch ◽  
Hugo Keller

The temperature dependencies of the in-plane (λab) and out-of-plane (λc) components of the magnetic field penetration depth were investigated near the surface and in the bulk of the electron-doped superconductor Sr0.9La0.1CuO2 by means of magnetization measurements. The measured λab(T) and λc(T) were analyzed in terms of a two-gap model with mixed s+d-wave symmetry of the order parameter. λab(T) is well described by an almost pure anisotropic d-wave symmetry component (≃96%), mainly reflecting the surface properties of the sample. In contrast, λc(T) exhibits a mixed s+d-wave order parameter with a substantial s-wave component of more than 50%. The comparison of λab−2(T) measured near the surface with that determined in the bulk by means of the muon-spin rotation/relaxation technique demonstrates that the suppression of the s-wave component of the order parameter near the surface is associated with a reduction of the superfluid density by more than a factor of two.


1991 ◽  
Vol 185-189 ◽  
pp. 1087-1088 ◽  
Author(s):  
Hideaki Kitazawa ◽  
Eiko Torikai ◽  
Kusuo Nishiyama ◽  
Kanetada Nagamine ◽  
Fumitoshi Iga ◽  
...  

1993 ◽  
Vol 71 (23) ◽  
pp. 3862-3865 ◽  
Author(s):  
S. L. Lee ◽  
P. Zimmermann ◽  
H. Keller ◽  
M. Warden ◽  
I. M. Savić ◽  
...  

1995 ◽  
Vol 140-144 ◽  
pp. 1381-1382 ◽  
Author(s):  
K. Prokeš ◽  
P. Svoboda ◽  
V. Sechovsky ◽  
E. Brück ◽  
A. Amato ◽  
...  

2007 ◽  
Vol 21 (18n19) ◽  
pp. 3086-3095 ◽  
Author(s):  
JOHN D. DOW ◽  
DALE R. HARSHMAN

Muon spin rotation (μ+SR) measurements conducted on crystalline YBa 2 Cu 3 O 7 are consistent with s-wave pairing, not d-wave, suggesting that the superconducting hole condensate resides in the BaO layers, not in the cuprate-planes. The specific heat and thermal conductivity data are explained by the superconducting BaO layers alone, unlike the failed interpretation based on CuO 2-plane superconductivity. The layer charges of the CuO 2 planes are almost -2 | e |, indicating that those planes are primarily carriers of electrons, not holes. The cuprate-planes are not the dominant hole-carriers of high- T C superconductivity, as demonstrated by doped YBa 2 RuO 6, which has no such CuO 2 lanes, yet superconducts at ~ 93 K. Moreover the trio of related compounds, YSr 2 RuO 6 (doped with Cu on Ru sites), undoped GdSr 2 Cu 2 RuO 8, and undoped Gd 2-z Ce z Sr 2 Cu 2 RuO 10 all start superconducting near 49 K in their SrO layers, not in the cuprate planes of the two compounds that have such planes, because those planes are either antiferromagnetic or weakly ferromagnetic and so do not superconduct. In PrBa 2 Cu 3 O 7, a Pr -on- Ba -site ( Pr Ba) defect kills the superconductivity, but Pr -on- Pr -site ( Pr Pr) does not. Both defects are approximately equidistant from the intervening cuprate plane, suggesting that the cuprate plane does not carry significant superconductivity. In GdBa 2 Cu 3 O 7, Gd -on-a- Gd -site ( Gd Gd) does not break Cooper pairs, but Gd -on-a- Ba -site ( Gd Ba) does, indicating that the superconductivity is in the BaO layers, and not in the cuprate-planes. In HgBa 2 Ca n-1 Cu n O 2n+2, the BaO layers, not the cuprate-planes, gain positive charge as T C, pressure, and the number of layers n increase. The reason that theories based on holes in the cuprate-planes have done so poorly is that those planes were incorrectly identified as the source of high-temperature superconductivity on the basis of a single datum by Cava et al., that was first contradicted by Jorgensen et al., and then endorsed by Jorgensen alone on the basis of the Cava datum, not his own. This error is the main reason why cuprate-plane superconductivity, which probably does not exist, has been so widely accepted.


1997 ◽  
Vol 85 (1-3) ◽  
pp. 1495-1496 ◽  
Author(s):  
S.L. Lee ◽  
S.J. Blundell ◽  
F.L. Pratt ◽  
P.A. Pattenden ◽  
E.M. Forgan ◽  
...  

2000 ◽  
Vol 14 (25n27) ◽  
pp. 2828-2833 ◽  
Author(s):  
R. Rogai ◽  
R. Marcon ◽  
E. Silva ◽  
R. Fastampa ◽  
M. Giura ◽  
...  

We present measurements of the magnetic field dependent complex resistivity at 48 GHz in a nearly-optimally doped thin YBa 2 Cu 3 O 7-δ film. Below Tc the application of the magnetic field leads to a detectable magnetoresistivity. The real part is clearly measurable from our lowest temperature up to Tc, while the imaginary part can be distinguished from zero only for T>87 K . The magnetoresistivity arises from the combined effects of fluxon motion and field-induced superfluid depletion. We discuss whether our data can be described or not by models for the magnetic response in an s-wave or d-wave superconductor.


1999 ◽  
Vol 59 (5) ◽  
pp. 3775-3782 ◽  
Author(s):  
Th. Jestädt ◽  
K. H. Chow ◽  
S. J. Blundell ◽  
W. Hayes ◽  
F. L. Pratt ◽  
...  

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