Simulation of growth dynamics in atomic layer deposition. Part I. Amorphous films

2007 ◽  
Vol 515 (11) ◽  
pp. 4527-4537 ◽  
Author(s):  
Ola Nilsen ◽  
Ole Bjørn Karlsen ◽  
Arne Kjekshus ◽  
Helmer Fjellvåg
2017 ◽  
Vol 26 (2) ◽  
pp. 027701 ◽  
Author(s):  
Xue-Li Ma ◽  
Hong Yang ◽  
Jin-Juan Xiang ◽  
Xiao-Lei Wang ◽  
Wen-Wu Wang ◽  
...  

2007 ◽  
Vol 515 (11) ◽  
pp. 4538-4549 ◽  
Author(s):  
Ola Nilsen ◽  
Ole Bjørn Karlsen ◽  
Arne Kjekshus ◽  
Helmer Fjellvåg

2020 ◽  
Author(s):  
Petro Deminskyi ◽  
Chih-Wei Hsu ◽  
Babak Bakhit ◽  
Polla Rouf ◽  
Henrik Pedersen

Gallium nitride (GaN) is one of the most important semiconductor materials in modern electronics. While GaN films are routinely deposited by chemical vapor deposition at around 1000 °C, low-temperature routes for GaN deposition need to be better understood. Herein, we present an atomic layer deposition (ALD) process for GaN-based on triethyl gallium (TEG) and ammonia plasma and show that the process can be improved by adding a reactive pulse between the TEG and ammonia plasma, making it an ABC-type pulsed process. We show that the material quality of the deposited GaN is not affected by the B-pulse, but that the film growth per ALD cycle increase when a B-pulse is added. We suggest that this can be explained by removal of ethyl ligands from the surface by the B-pulse, enabling a more efficient nitridation by the ammonia plasma. We show that the B-pulsing can be used to enable GaN deposition with a thermal ammonia pulse, albeit of X-ray amorphous films.


2007 ◽  
Vol 515 (11) ◽  
pp. 4550-4558 ◽  
Author(s):  
Ola Nilsen ◽  
Ole Bjørn Karlsen ◽  
Arne Kjekshus ◽  
Helmer Fjellvåg

2020 ◽  
Author(s):  
Petro Deminskyi ◽  
Chih-Wei Hsu ◽  
Babak Bakhit ◽  
Polla Rouf ◽  
Henrik Pedersen

Gallium nitride (GaN) is one of the most important semiconductor materials in modern electronics. While GaN films are routinely deposited by chemical vapor deposition at around 1000 °C, low-temperature routes for GaN deposition need to be better understood. Herein, we present an atomic layer deposition (ALD) process for GaN-based on triethyl gallium (TEG) and ammonia plasma and show that the process can be improved by adding a reactive pulse between the TEG and ammonia plasma, making it an ABC-type pulsed process. We show that the material quality of the deposited GaN is not affected by the B-pulse, but that the film growth per ALD cycle increase when a B-pulse is added. We suggest that this can be explained by removal of ethyl ligands from the surface by the B-pulse, enabling a more efficient nitridation by the ammonia plasma. We show that the B-pulsing can be used to enable GaN deposition with a thermal ammonia pulse, albeit of X-ray amorphous films.


2021 ◽  
Vol 3 (1) ◽  
pp. 59-71
Author(s):  
Degao Wang ◽  
Qing Huang ◽  
Weiqun Shi ◽  
Wei You ◽  
Thomas J. Meyer

2018 ◽  
Author(s):  
Peter George Gordon ◽  
Goran Bacic ◽  
Gregory P. Lopinski ◽  
Sean Thomas Barry

Al-doped ZnO (AZO) is a promising earth-abundant alternative to Sn-doped In<sub>2</sub>O<sub>3</sub> (ITO) as an n-type transparent conductor for electronic and photovoltaic devices; AZO is also more straightforward to deposit by atomic layer deposition (ALD). The workfunction of this material is particularly important for the design of optoelectronic devices. We have deposited AZO films with resistivities as low as 1.1 x 10<sup>-3</sup> Ωcm by ALD using the industry-standard precursors trimethylaluminum (TMA), diethylzinc (DEZ), and water at 200<sup>◦</sup>C. These films were transparent and their elemental compositions showed reasonable agreement with the pulse program ratios. The workfunction of these films was measured using a scanning Kelvin Probe (sKP) to investigate the role of aluminum concentration. In addition, the workfunction of AZO films prepared by two different ALD recipes were compared: a “surface” recipe wherein the TMA was pulsed at the top of each repeating AZO stack, and a interlamellar recipe where the TMA pulse was introduced halfway through the stack. As aluminum doping increases, the surface recipe produces films with a consistently higher workfunction as compared to the interlamellar recipe. The resistivity of the surface recipe films show a minimum at a 1:16 Al:Zn atomic ratio and using an interlamellar recipe, minimum resistivity was seen at 1:19. The film thicknesses were characterized by ellipsometry, chemical composition by EDX, and resistivity by four-point probe.<br>


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