scholarly journals d-wave model for microwave response of high-Tcsuperconductors

1994 ◽  
Vol 50 (14) ◽  
pp. 10250-10264 ◽  
Author(s):  
P. J. Hirschfeld ◽  
W. O. Putikka ◽  
D. J. Scalapino
Keyword(s):  
2015 ◽  
Vol 39 (6) ◽  
pp. 898-906
Author(s):  
SaeedReza Tofighi ◽  
Masoud Shafiee ◽  
Sayyid Mehdi Alavinia

In this paper, the problem of three-dimensional (3-D) system stability is studied. In order to investigate the stability of 3-D systems, a new representation scheme is introduced based on the local state model proposed by Givone–Roesser for 3-D systems. This representation is obtained from the extended expression of the 1-D wave model proposed by Porter–Aravena. Then, according to the obtained model a new criteria for the stability of 3-D systems is stated. This criteria provides a simpler way to investigate asymptotic stability. Furthermore, an algorithm is performed to illustrate the procedure of analysing stability. Finally, some examples are performed and verified using numerical simulations in order to illustrate the given criteria for the stability.


2000 ◽  
Vol 14 (25n27) ◽  
pp. 2932-2937 ◽  
Author(s):  
G. LAMURA ◽  
J. LE COCHEC ◽  
J. BOK ◽  
A. GAUZZI ◽  
F. LICCI ◽  
...  

In order to unveil the origin of the gapless properties of cuprate superconductors, we study the low temperature dependence of the magnetic penetration depth λ in: a) conventional NbN superconducting films with granular and epitaxial microstructure; b) single crystals of La 2-x Sr x CuO 4, Bi 2 Sr 2 CaCu 2 O 8 (BSCCO) and YBa 2 Cu 3 O 6+x at various doping levels ranging from the under- to the overdoped regimes. The measurements are performed by using a novel single-coil technique achieving 10 pm resolution. Our experimental results are as follows. a) The granular NbN films exhibit a linear low-temperature dependence of λ similar to the dependence reported earlier in cuprates. In the epitaxial NbN films, we find the characteristic exponential behaviour of conventional s-wave superconductors. b) In all single crystals of cuprates, the data confirm the linear dependence of λ ab reported earlier. In BSCCO, we find that the slope d λ ab / dT is rapidly increasing as doping decreases. As to a), our results give evidence for a gapless behaviour in conventional s-wave superconductors induced by a granular microstructure. As to b), our analysis indicates that a simple d-wave model accounts for the experimental slope values only in the optimally and over-doped samples. In the underdoped samples, the d-wave model underestimates the large slope values observed experimentally. Such large values are rather consistent with a simple model of thermodynamic phase fluctuations suited for metals with reduced dimensionality and low carrier density, as in cuprates. We argue that this fluctuation model also accounts for the linear dependence of λ found in our granular NbN films. We discuss possible mechanisms associated with the existence of weak links across the grains, which would favour thermally activated phase fluctuations of the gap in this conventional superconductor. Finally, we put forward the hypothesis that a similar phenomenon may occur in cuprates because of the intrinsic granularity associated with phase-separated metallic and insulating regions in the superconducting ab-plane.


2005 ◽  
Vol 19 (01n03) ◽  
pp. 147-151 ◽  
Author(s):  
DALE R. HARSHMAN ◽  
JOHN D. DOW

Previous interpretations of the thermal conductivity data of YBa 2 Cu 3 O 7 in terms of d-wave superconductivity have created the impression that this experiment can only be successfully explained in terms of a d-wave model. Here we show that thermal conductivity data can be (better) explained in terms of s-wave hole-pairing, which also handles some outstanding problems with the d-wave interpretation, namely, muon spectra that are s-wave and specific heat data that exhibit a zero-field linear-T term. The basic notion is that a high-temperature superconductor such as YBa 2 Cu 2 O 7 contains both superconducting and non-superconducting bands. The main superconducting bands are associated with BaO , and the CuO 2 bands are non-superconducting.


1995 ◽  
Vol 8 (5) ◽  
pp. 673-674
Author(s):  
C. O'Donovan ◽  
J. P. Carbotte
Keyword(s):  

2005 ◽  
Vol 86 (11) ◽  
pp. 112509 ◽  
Author(s):  
M. I. Salkola ◽  
D. J. Scalapino

1995 ◽  
Vol 56 (12) ◽  
pp. 1945-1949 ◽  
Author(s):  
T. Jacobs ◽  
S. Sridhar ◽  
C.T. Rieck ◽  
K. Scharnberg ◽  
T. Wolf ◽  
...  

1992 ◽  
Vol 2 (3) ◽  
pp. 355-372 ◽  
Author(s):  
M. R. Trunin ◽  
G. I. Leviev
Keyword(s):  

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