Bonded interface properties of Nb direct bonding with Si intermediate layer for 3D interconnection of superconducting devices

Author(s):  
Yuta Takahashi ◽  
Masahisa Fujino ◽  
Hiroshi Nakagawa ◽  
Katsuya Kikuchi ◽  
Tohru Taino
2014 ◽  
Vol 778-780 ◽  
pp. 714-717 ◽  
Author(s):  
Yukihiro Sasada ◽  
Takamasa Kurumi ◽  
Hideo Shimizu ◽  
Hiroyuki Kinoshita ◽  
Masahiro Yoshimoto

Si wafers were directly bonded to 6H-SiC wafers without the formation of an intermediate layer. Heterojunctions of n-Si/n-SiC and p-Si/n-SiC exhibited ohmic and rectifying characteristics, respectively, as expected based on their band lineups. Band bending of Si at the bonded interface was observed for Si/semi-insulating 6H-SiC heterointerfaces. This band bending can be explained by either heterojunction formation based on Anderson’s model or the existence of negative charge with a density of ~2 × 1010 cm−2 at the Si/SiC interface.


Author(s):  
O. Eibl ◽  
G. Gieres ◽  
H. Behner

The microstructure of high-Tc YBa2Cu3O7-X thin films deposited by DC-sputtering on SrTiO3 substrates was analysed by TEM. Films were either (i) deposited in the amorphous state at substrate temperatures < 450°C and crystallised by a heat treatment at 900°C (process 1) or (ii) deposited at around 740°C in the crystalline state (process 2). Cross sections were prepared for TEM analyses and are especially useful for studying film substrate interdiffusion (fig.1). Films deposited in process 1 were polycristalline and the grain size was approximately 200 nm. Films were porous and the size of voids was approximately 100 nm. Between the SrTiO3 substrate and the YBa2Cu3Ox film a densly grown crystalline intermediate layer approximately 150 nm thick covered the SrTiO3 substrate. EDX microanalyses showed that the layer consisted of Sr, Ba and Ti, however, did not contain Y and Cu. Crystallites of the layer were carefully tilted in the microscope and diffraction patterns were obtained in five different poles for every crystallite. These patterns were consistent with the phase (Ba1-XSrx)2TiO4. The intermediate layer was most likely formed during the annealing at 900°C. Its formation can be understood as a diffusion of Ba from the amorphously deposited film into the substrate and diffusion of Sr from the substrate into the film. Between the intermediate layer and the surface of the film the film consisted of YBa2Cu3O7-x grains. Films prepared in process 1 had Tc(R=0) close to 90 K, however, critical currents were as low as jc = 104A/cm2 at 77 K.


2001 ◽  
Vol 25 (4−2) ◽  
pp. 767-770 ◽  
Author(s):  
T. Daibou ◽  
M. Oogane ◽  
Y. Ando ◽  
C. Kim ◽  
O. Song ◽  
...  

Author(s):  
Lucas Copeland ◽  
Mukul Saran

Abstract This paper presents a mechanical cross-sectioning approach that produces an image clarity not yet demonstrated in published literature. It demonstrates how a critical sequence of polishing, basic slurry optimization and staining, in conjunction with correct imaging parameters can be used to highlight the growth morphology of the intermetallic compound (IMCs). Utilizing this approach, the paper describes the results of a SEM imaging study of the intermetallic formation and growth at the Cu-Al bond interface during thermal ageing for up to 4000hrs at 150 deg C. The paper uses direct SEM imaging to catalog observations which are used to create an initial model for IMC and void growth at the wire bonded interface. It examines the effect of aluminum splash and concludes that growth of intermetallics at the Cu-Al interface is rapid into the bond-pad aluminum than into the Cu-ball, but the growth thickness uniformity is much higher into the Cu-ball.


2009 ◽  
Vol 13 (9) ◽  
pp. 1073-1082
Author(s):  
Sylvain Chataigner ◽  
Jean-François Caron ◽  
Karim Benzarti ◽  
Marc Quiertant ◽  
Christophe Aubagnac

2002 ◽  
Author(s):  
T. P. Orlando ◽  
J. E. Mooij ◽  
Seth Lloyd

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