Universality of Low-Energy Mass Renormalization in the Superconducting State of Hole-Doped High-Tc Superconductors

2007 ◽  
Vol 76 (10) ◽  
pp. 103707 ◽  
Author(s):  
Takafumi Sato ◽  
Kensei Terashima ◽  
Kosuke Nakayama ◽  
Hiroaki Matsui ◽  
Takashi Takahashi ◽  
...  
2007 ◽  
Vol 463-465 ◽  
pp. 123-125
Author(s):  
T. Hata ◽  
S. Onari ◽  
S. Honda ◽  
H. Itoh ◽  
Y. Tanaka ◽  
...  

2000 ◽  
Vol 14 (29n31) ◽  
pp. 3334-3341 ◽  
Author(s):  
C. D. BATISTA ◽  
G. ORTIZ ◽  
A. V. BALATSKY

We present a unified theory for the resonance peak and low-energy incommensurate response observed in high-Tc cuprate superconductors. The origin of both features is purely magnetic and they represent universal features signaling the existence of an incommensurate spin state both below and above the superconducting transition temperature. We argue that the resonance peak is the reflection of commensurate antiferromagnetism. Our theoretical scenario gives an account of the main universal features observed in various families of superconductors and predicts those that have not been observed yet experimentally.


1989 ◽  
Vol 03 (17) ◽  
pp. 1275-1283 ◽  
Author(s):  
I. J. R. AITCHISON ◽  
N. E. MAVROMATOS

In the presence of monopole configurations of the spin (or "statistical") gauge field arising in effective theories of systems may be relevant to high T c superconductivity, the coefficient of the Chern-Simons term, which determines the statistics of the anyons, is quantized in such a way that, in the superconducting state, the electromagnetic flux quantum is restricted to the values 2π/2qe, q = integer . This result is achieved by requiring U(1) gauge invariance on manifolds of the form R2 × S1 where S1 is the compactified Matsubara time of quantum statistics. A brief discussion on the role of holes in the cancellation of the bare Chern-Simons term, and the consequences thereof, is also presented.


1994 ◽  
Vol 235-240 ◽  
pp. 67-70 ◽  
Author(s):  
C. Berthier ◽  
M. Horvatić ◽  
P. Carretta ◽  
Y. Berthier ◽  
P. Ségransan ◽  
...  

1989 ◽  
Vol 03 (02) ◽  
pp. 141-143
Author(s):  
W. GORZKOWSKI

The following effect should be observed in certain high-T c superconductors: for T<T c , the superconducting state, after being destroyed by an applied magnetic field greater than H c2 (at T), cannot spontaneously reappear or does so after a long delay, at the temperature T.


1996 ◽  
Vol 46 (S2) ◽  
pp. 935-936
Author(s):  
A. Bussmann-Holder ◽  
L. Genzel ◽  
A. R. Bishop ◽  
A. Simon

Author(s):  
John Silcox

Determination of the microstructure and microchemistry of small features often provides the insight needed for the understanding of processes in real materials. In many cases, it is not adequate to use microscopy alone. Microdiffraction and microspectroscopic information such as EELS, X-ray microprobe analysis and Auger spectroscopy can all contribute vital parts of the picture. For a number of reasons, dedicated STEM offers considerable promise as a quantitative instrument. In this paper, we review progress towards effective quantitative use of STEM with illustrations drawn from studies of high Tc superconductors, compound semiconductors and metallization of H-terminated silicon.Intrinsically, STEM is a quantitative instrument. Images are acquired directly by detectors in serial mode which is particularly convenient for digital image acquisition, control and display. The VG HB501A at Cornell has been installed in a particularly stable electromagnetic, vibration and acoustic environment. Care has been paid to achieving UHV conditions (i.e., 10-10 Torr). Finally, it has been interfaced with a VAX 3200 work station by Kirkland. This permits, for example, the acquisition of bright field (or energy loss) images and dark field images simultaneously as quantitative arrays in perfect registration.


Author(s):  
Maryvonne Hervieu

Four years after the discovery of superconductivity at high temperature in the Ba-La-Cu-O system, more than thirty new compounds have been synthesized, which can be classified in six series of copper oxides: La2CuO4 - type oxides, bismuth cuprates, YBa2Cu3O7 family, thallium cuprates, lead cuprates and Nd2CuO4 - type oxides. Despite their quite different specific natures, close relationships allow their structures to be simply described through a single mechanism. The fifth first families can indeed be described as intergrowths of multiple oxygen deficient perovskite slabs with multiple rock salt-type slabs, according to the representation [ACuO3-x]m [AO]n.The n and m values are integer in the parent structures, n varying from 0 to 3 and m from 1 to 4; every member of this large family can thus be symbolized by [m,n]. The oxygen deficient character of the perovskite slabs involves the existence or the co-existence of several types of copper environment: octahedral, pyramidal and square planar.Both mechanisms, oxygen deficiency and intergrowth, are well known to give rise easily to nonstoichiometry phenomena. Numerous and various phenomena have actually been characterized in these cuprates, strongly depending on the thermal history of the samples.


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