scholarly journals Novel Electronic State and Superconductivity in the Electron-Doped High-Tc T’-Superconductors

2017 ◽  
Vol 2 (3) ◽  
pp. 23 ◽  
Author(s):  
Tadashi Adachi ◽  
Takayuki Kawamata ◽  
Yoji Koike
Keyword(s):  
2000 ◽  
Vol 14 (29n31) ◽  
pp. 3536-3541 ◽  
Author(s):  
S. Kuwata

We examine the possibility of high-Tc superconductivity mediated by the elementary excitation of an electron stripe which is realized by neutralizing local polarization mainly caused by the c-displacement of ions on the CuO 2 plane. Under the translation invariance of the electronic state of the neutralization charges, it is found that both itinerant and localized electrons and/or holes can coexist in the stripe phase. If the frequency of the localized charge oscillation tends to soften along the stripe direction, superconductivity with Tc around 100 K can be realized, due to the enhancement of the coupling constant.


Materia Japan ◽  
1995 ◽  
Vol 34 (12) ◽  
pp. 1354-1357
Author(s):  
Sadamichi Maekawa

2016 ◽  
Vol 523 ◽  
pp. 28-54 ◽  
Author(s):  
Michio Naito ◽  
Yoshiharu Krockenberger ◽  
Ai Ikeda ◽  
Hideki Yamamoto

2003 ◽  
Vol 388-389 ◽  
pp. 293-294
Author(s):  
Atsushi Suzuki ◽  
Kenta Kainuma ◽  
Morio Suzuki
Keyword(s):  

2000 ◽  
Vol 331 (2) ◽  
pp. 97-112 ◽  
Author(s):  
A.S. Alexandrov ◽  
P.P. Edwards

Author(s):  
H.-J. Ou ◽  
J. M. Cowley

Using the dedicate VG-HB5 STEM microscope, the crystal structure of high Tc superconductor of YBa2Cu3O7-x has been studied via high resolution STEM (HRSTEM) imaging and nanobeam (∽3A) diffraction patterns. Figure 1(a) and 2(a) illustrate the HRSTEM image taken at 10' times magnification along [001] direction and [100] direction, respectively. In figure 1(a), a grain boundary with strong field contrast is seen between two crystal regions A and B. The grain boundary appears to be parallel to a (110) plane, although it is not possible to determine [100] and [001] axes as it is in other regions which contain twin planes [3]. Following the horizontal lattice lines, from left to right across the grain boundary, a lattice bending of ∽4° is noticed. Three extra lattice planes, indicated by arrows, were found to terminate at the grain boundary and form dislocations. It is believed that due to different chemical composition, such structure defects occur during crystal growth. No bending is observed along the vertical lattice lines.


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