High Tc Tri-Layers for Josephson Junctions

1992 ◽  
Vol 275 ◽  
Author(s):  
J. N. Eckstein ◽  
I. Bozovic ◽  
M. E. Klausmeier-Brown ◽  
G. F. Virshup

ABSTRACTAtomic Layer-by-Layer Molecular Beam Epitaxy (ALL-MBE) of high Tc superconducting films can be used to grow defect-free and flat multi-layer structures in which superconducting molecular layers are stacked with molecular layers having other electronic properties. In particular, tri-layers consisting of c-axis Bi2Sr2CaCu2O8 base and counter electrode layers, each several hundred angstroms thick, have been grown separated by single molecular layers of metastable compounds such as Bi2Sr2Can-1CunO2+4 where n ranged from 5 to 11. Furthermore, the electronic properties of such barrier layers have been modified by doping with trivalent cations. Using such structures, tri-layer Josephson junctions have been fabricated which exhibit hysteretic I - V characteristics. Other doping schemes have given insulating layers which dominate c-axis transport, demonstrating the ability of this technique to grow thin, 25 Å, single molecular layers that are free of pinholes.

2020 ◽  
Vol 117 (7) ◽  
pp. 072601 ◽  
Author(s):  
D. Putzky ◽  
P. Radhakrishnan ◽  
Y. Wang ◽  
P. Wochner ◽  
G. Christiani ◽  
...  

1989 ◽  
Vol 169 ◽  
Author(s):  
K. Wasa ◽  
H. Adachi ◽  
K. Hirochi ◽  
Y. Ichikawa ◽  
K. Setsune

AbstractBasic thin film deposition processes for the high-Tc superconductors of Bi-systems are described. There appear several superconducting phases including the low-Tc phase Bi2Sr2Ca1 Cu2Ox and the high-Tc phase Bi2Sr2Ca2Cu3Ox. Thin films with these superconducting phases are synthesized by a selection of the substrate temperature Ts during the deposition : the high-Tc phase with Tc=100K is synthesized at Ts>800 °C; the low-Tc phase with Tc=80K, at Ts<600°C. However, these films often comprise show structure comprizing the different superconducting phases.The close control of the superconducting phase has been achieved by the layer-by-layer deposition in the atomic layer epitaxy process.


2013 ◽  
pp. 509-528 ◽  
Author(s):  
James N. Eckstein ◽  
Mao Zheng ◽  
Xiaofang Zhai ◽  
Bruce Davidson ◽  
Maitri Warusawithana ◽  
...  

2014 ◽  
Vol 5 ◽  
pp. 596-602 ◽  
Author(s):  
Federico Baiutti ◽  
Georg Christiani ◽  
Gennady Logvenov

In this paper we present the atomic-layer-by-layer oxide molecular beam epitaxy (ALL-oxide MBE) which has been recently installed in the Max-Planck Institute for Solid State Research and we report on its present status, providing some examples that demonstrate its successful application in the synthesis of different layered oxides, with particular reference to superconducting La2CuO4 and insulator-to-metal La2− x Sr x NiO4. We briefly review the ALL-oxide MBE technique and its unique capabilities in the deposition of atomically smooth single-crystal thin films of various complex oxides, artificial compounds and heterostructures, introducing our goal of pursuing a deep investigation of such systems with particular emphasis on structural defects, with the aim of tailoring their functional properties by precise defects control.


2017 ◽  
Vol 2 (1) ◽  
Author(s):  
Qingyu Lei ◽  
Maryam Golalikhani ◽  
Bruce A. Davidson ◽  
Guozhen Liu ◽  
Darrell G. Schlom ◽  
...  

1996 ◽  
Vol 11 (7) ◽  
pp. 1609-1615 ◽  
Author(s):  
A. Chaiken ◽  
M. A. Wall ◽  
R. H. Howell ◽  
I. Bozovic ◽  
J. N. Eckstein ◽  
...  

Films of Bi2Sr2CaCu2O8 and Bi2Sr2CuO6 have been grown using Atomic-Layer-by-Layer Molecular Beam Epitaxy (ALL-MBE) on lattice-matched substrates. These materials have been combined with layers of closely related metastable compounds like Bi2Sr2Ca7Cu8O20 (2278) and rare-earth-doped compounds like Bi2Sr2DyxCa1–xCu2O8 (Dy: 2212) to form heterostructures with unique superconducting properties, including superconductor/insulator multilayers and tunnel junctions. Transmission electron microscopy (TEM) has been used to study the morphology and microstructure of these heterostructures. These TEM studies shed light on the physical properties of the films, and give insight into the growth mode of highly anisotropic solids like Bi2Sr2CaCu2O8.


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