Identification of superconducting phases in the Ba-Ca-Cu-O system: an unstable phase with Tc≈126 K and its derivative with Tc≈90 K

1999 ◽  
Vol 9 (5) ◽  
pp. 1141-1148 ◽  
Author(s):  
T. Hosomi ◽  
H. Suematsu ◽  
H. Fjellvåg ◽  
M. Karppinen ◽  
H. Yamauchi

Author(s):  
A.Q. He ◽  
G.W. Qiao ◽  
J. Zhu ◽  
H.Q. Ye

Since the first discovery of high Tc Bi-Sr-Ca-Cu-O superconductor by Maeda et al, many EM works have been done on it. The results show that the superconducting phases have a type of ordered layer structures similar to that in Y-Ba-Cu-O system formulated in Bi2Sr2Can−1CunO2n+4 (n=1,2,3) (simply called 22(n-1) phase) with lattice constants of a=0.358, b=0.382nm but the length of c being different according to the different value of n in the formulate. Unlike the twin structure observed in the Y-Ba-Cu-O system, there is an incommensurate modulated structure in the superconducting phases of Bi system superconductors. Modulated wavelengths of both 1.3 and 2.7 nm have been observed in the 2212 phase. This communication mainly presents the intergrowth of these two kinds of one-dimensional modulated structures in 2212 phase.



Author(s):  
J.G. Wen ◽  
K.K. Fung

Bi-based superconducting phases have been found to be members of a structural series represented by Bi2Sr2Can−1Cun−1On+4, n=1,2,3, and are referred to as 2201, 2212, 2223 phases. All these phases are incommensurate modulated structures. The super space groups are P2/b, NBbmb 2201, 2212 phases respectively. Pb-doped ceramic samples and single crystals and Y-doped single crystals have been studied by transmission electron microscopy.Modulated structures of all Bi-based superconducting phases are in b-c plane, therefore, it is the best way to determine modulated structure and c parameter in diffraction pattern. FIG. 1,2,3 show diffraction patterns of three kinds of modulations in Pb-doped ceramic samples. Energy dispersive X-ray analysis (EDAX) confirms the presence of Pb in the three modulated structures. Parameters c are 3 0.06, 38.29, 30.24Å, ie 2212, 2223, 2212 phases for FIG. 1,2,3 respectively. Their average space groups are all Bbmb.



2021 ◽  
Vol 126 (11) ◽  
Author(s):  
Yu-Hui Chen ◽  
Sebastian P. Horvath ◽  
Jevon J. Longdell ◽  
Xiangdong Zhang


1996 ◽  
Vol 9 (3) ◽  
pp. 273-276 ◽  
Author(s):  
G. Aldica ◽  
I. I. Geru ◽  
B. M. Puscasu ◽  
F. Constantinescu ◽  
P. Badica


2003 ◽  
Vol 10 (3) ◽  
pp. 636-642 ◽  
Author(s):  
Andrea Willfort-Ehringer ◽  
Ramazanali Ahmadi ◽  
Michael E. Gschwandtner ◽  
Angelika Haumer ◽  
Gottfried Heinz ◽  
...  

Purpose: To study the dynamics of carotid stent healing over a 2-year period using duplex ultrasound imaging. Methods: One hundred twelve patients with 121 successfully stented carotid arteries were examined with color-coded duplex ultrasound the day after the stent procedure and at 1, 3, 6, 12, and 24 months in follow-up. The maximal thickness and echogenicity of the layer between the stent and the perfused lumen (SPL) were evaluated. Echogenicity was classified as echogenic if the SPL layer was clearly detected in B mode and echolucent if the SPL layer was barely visible in B mode, its border defined by assistance of color-coded flow. Results: At day 1, an echolucent SPL layer with a median thickness of 0.7 mm was interpreted as a thrombotic layer, which decreased at 1 month to practically zero (i.e., not detectable). In follow-up, increases in thickness (mainly up to 6 months) and echogenicity (up to 12 months) of the SPL layer were interpreted as neointimal ingrowth. At 3, 6, and 12 months, the median maximal thickness of the SPL layer was 0.5 mm, 0.9 mm, and 1.0 mm, respectively, whereas the percentage of patients with an echogenic SPL layer was 27% (32/119), 56% (66/117), and 95% (105/110), respectively, at the same time intervals. No further change was observed at the 24-month examination. Conclusions: Three phases of carotid stent incorporation are defined: (1) an early unstable period soon after stent placement with an echolucent (thrombotic) SPL layer, (2) a moderately unstable phase with ingrowing neointima (1–12 months), and (3) a stable phase from the second year on. These data may indicate the need for different intensities of therapy and surveillance intervals.



1991 ◽  
Vol 185-189 ◽  
pp. 583-584 ◽  
Author(s):  
A. Tressaud ◽  
B. Chevalier ◽  
C. Robin ◽  
E. Hickey ◽  
J. Etourneau


1989 ◽  
Vol 40 (7) ◽  
pp. 5266-5269 ◽  
Author(s):  
S. X. Dou ◽  
H. K. Liu ◽  
A. J. Bourdillon ◽  
M. Kviz ◽  
N. X. Tan ◽  
...  


2017 ◽  
Vol 129 (34) ◽  
pp. 10326-10329 ◽  
Author(s):  
Tiange Bi ◽  
Daniel P. Miller ◽  
Andrew Shamp ◽  
Eva Zurek


1990 ◽  
Vol 165-166 ◽  
pp. 369-370 ◽  
Author(s):  
G.J.C.L. Bruls ◽  
D. Weber ◽  
B. Wolf ◽  
B. Luthi ◽  
A.A. Menovsky ◽  
...  


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