scholarly journals Realization of Epitaxial Thin Films of the Topological Crystalline Insulator Sr 3 SnO

2020 ◽  
Vol 32 (34) ◽  
pp. 2000809 ◽  
Author(s):  
Yanjun Ma ◽  
Anthony Edgeton ◽  
Hanjong Paik ◽  
Brendan D. Faeth ◽  
Christopher T. Parzyck ◽  
...  
2021 ◽  
Vol 207 ◽  
pp. 116683
Author(s):  
Jun Young Lee ◽  
Gopinathan Anoop ◽  
Sanjith Unithrattil ◽  
WooJun Seol ◽  
Youngki Yeo ◽  
...  

2020 ◽  
Vol 102 (21) ◽  
Author(s):  
Stephan Geprägs ◽  
Björn Erik Skovdal ◽  
Monika Scheufele ◽  
Matthias Opel ◽  
Didier Wermeille ◽  
...  

2021 ◽  
Vol 5 (1) ◽  
Author(s):  
Dongyi Qin ◽  
Kazumasa Iida ◽  
Takafumi Hatano ◽  
Hikaru Saito ◽  
Yiming Ma ◽  
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2021 ◽  
Vol 129 (9) ◽  
pp. 093903
Author(s):  
Manik Kuila ◽  
Uday Deshpande ◽  
R. J. Choudhary ◽  
Parasmani Rajput ◽  
D. M. Phase ◽  
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2017 ◽  
Vol 1 (7) ◽  
Author(s):  
Irene Lucas ◽  
Pilar Jiménez-Cavero ◽  
J. M. Vila-Fungueiriño ◽  
Cesar Magén ◽  
Soraya Sangiao ◽  
...  

AIP Advances ◽  
2021 ◽  
Vol 11 (4) ◽  
pp. 045124
Author(s):  
Cacie Hart ◽  
Zoey Warecki ◽  
Grace Yong ◽  
David Houston ◽  
Rajeswari Kolagani

2010 ◽  
Vol 82 (18) ◽  
Author(s):  
E. Karhu ◽  
S. Kahwaji ◽  
T. L. Monchesky ◽  
C. Parsons ◽  
M. D. Robertson ◽  
...  

2013 ◽  
Vol 1507 ◽  
Author(s):  
Ryosuke Yamauchi ◽  
Geng Tan ◽  
Daishi Shiojiri ◽  
Nobuo Tsuchimine ◽  
Koji Koyama ◽  
...  

ABSTRACTWe examined the influence of momentary annealing on the nanoscale surface morphology of NiO(111) epitaxial thin films deposited on atomically stepped sapphire (0001) substrates at room temperature in O2 at 1.3 × 10−3 and 1.3 × 10−6 Pa using a pulsed laser deposition (PLD) technique. The NiO films have atomically flat surfaces (RMS roughness: approximately 0.1–0.2 nm) reflecting the step-and-terrace structures of the substrates, regardless of the O2 deposition pressure. After rapid thermal annealing (RTA) of the NiO(111) epitaxial film deposited at 1.3 × 10−3 Pa O2, a periodic straight nanogroove array related to the atomic steps of the substrate was formed on the film surface for 60 s. In contrast, the fabrication of a transient state in the nanogroove array formation was achieved with RTA of less than 1 s. However, when the O2 atmosphere during PLD was 1.3 × 10−6 Pa, random crystal growth was observed and resulted in a disordered rough surface nanostructure after RTA.


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