A non-destructive n-doping method for graphene with precise control of electronic properties via atomic layer deposition

Nanoscale ◽  
2016 ◽  
Vol 8 (9) ◽  
pp. 5000-5005 ◽  
Author(s):  
Kyu Seok Han ◽  
Pranav Y. Kalode ◽  
Yong-Eun Koo Lee ◽  
Hongbum Kim ◽  
Lynn Lee ◽  
...  
2020 ◽  
Vol 8 (36) ◽  
pp. 12662-12668
Author(s):  
Henrik H. Sønsteby ◽  
Erik Skaar ◽  
Jon E. Bratvold ◽  
John W. Freeland ◽  
Angel Yanguas-Gil ◽  
...  

Cu-Substitution in LaNiO3 by atomic layer deposition provides films spanning six orders of magnitude in resistivity, with metal insulator transition temperatures from 0 K to room temperature.


2019 ◽  
Vol 2 (12) ◽  
pp. 8747-8756 ◽  
Author(s):  
Pascal Büttner ◽  
Florian Scheler ◽  
Craig Pointer ◽  
Dirk Döhler ◽  
Maïssa K. S. Barr ◽  
...  

2013 ◽  
Vol 24 (45) ◽  
pp. 455701
Author(s):  
Joonsung Kim ◽  
Jangyeol Yoon ◽  
Junhong Na ◽  
Seongmin Yee ◽  
Gyu Tae Kim ◽  
...  

2011 ◽  
Vol 119 (5) ◽  
pp. 696-698 ◽  
Author(s):  
A. Taube ◽  
S. Gierałtowska ◽  
T. Gutt ◽  
T. Małachowski ◽  
I. Pasternak ◽  
...  

2017 ◽  
Vol 132 (2) ◽  
pp. 329-331
Author(s):  
K. Król ◽  
N. Kwietniewski ◽  
S. Gierałtowska ◽  
Ł. Wachnicki ◽  
M. Sochacki

Nanoscale ◽  
2015 ◽  
Vol 7 (7) ◽  
pp. 3028-3034 ◽  
Author(s):  
N. Kemnade ◽  
C. J. Shearer ◽  
D. J. Dieterle ◽  
A. S. Cherevan ◽  
P. Gebhardt ◽  
...  

The hybridisation of metal oxides and nanocarbons has created a promising new class of functional materials for environmental and sustainable energy applications.


2015 ◽  
Vol 1096 ◽  
pp. 93-97
Author(s):  
Bao Jun Yan ◽  
Shu Lin Liu ◽  
Lu Ping Yang

Oxide thin films such as aluminum oxide doped with zinc (AZO), and aluminum oxide (Al2O3) were prepared in the pores of microchannel plate (MCP) by atomic layer deposition (ALD), which is a precise control thin film thickness on substrate with high aspect ratio structure. In this paper, homogenous oxide thin films deposited on varied substrates were prepared by ALD technology under different conditions, and the morphology, element distribution and structure of deposited samples are systematically investigated by scanning electron microscopy (SEM), energy dispersive x-ray (EDX), and x-ray diffraction (XRD) respectively, The results show that ALD technique is a good method to grow homogenous thin films on MCP.


1999 ◽  
Vol 564 ◽  
Author(s):  
Jae-Sik Min ◽  
Hyung-Sang Park ◽  
Wonyong Koh ◽  
Sang-Won Kang

AbstractTitanium-silicon-nitride films were grown by atomic layer deposition using an alternating supply of tetrakis(dimethylamido)titanium (TDMAT), silane. and ammonia, at substrate temperature of 180°C. The supply of a reactant was followed by a purge with inert gas before introducing another reactant onto the substrate in order to prevent gas-phase reactions. In one set of experiments the reactants were supplied separately in the sequence of TDMAT. silane. and ammonia. The Si content of the films remained constant at 18 at.%. and the film growth rate varied little from 0.24 nm per reactant-supply-cycle, even though silane partial pressure varied from 0.002 to 0.1 torr. In the other set of experiments silane and ammonia were simultaneously supplied in the sequence of TDMAT and silane/ammonia. The Si content varied from 3 to 23 at.% as the silane-to-ammonia ratio varied from 0.01 to 10. Atomic layer deposition of Ti-Si-N films allows the precise control of Si content as well as film thickness.


Nanomaterials ◽  
2019 ◽  
Vol 9 (8) ◽  
pp. 1083 ◽  
Author(s):  
Weiguang Hu ◽  
Truong Thi Hien ◽  
Dojin Kim ◽  
Hyo Sik Chang

Two-dimensional (2D) nanomaterials have distinct optical and electrical properties owing to their unique structures. In this study, smooth 2D amorphous tin disulfide (SnS2) films were fabricated by atomic layer deposition (ALD), and applied for the first time to photoelectrochemical water splitting. The optimal stable photocurrent density of the 50-nm-thick amorphous SnS2 film fabricated at 140 °C was 51.5 µA/cm2 at an oxygen evolution reaction (0.8 V vs. saturated calomel electrode (SCE)). This value is better than those of most polycrystalline SnS2 films reported in recent years. These results are attributed mainly to adjustable optical band gap in the range of 2.80 to 2.52 eV, precise control of the film thickness at the nanoscale, and the close contact between the prepared SnS2 film and substrate. Subsequently, the photoelectron separation mechanisms of the amorphous, monocrystalline, and polycrystalline SnS2 films are discussed. Considering above advantages, the ALD amorphous SnS2 film can be designed and fabricated according to the application requirements.


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