Exploring hafnium oxide's potential for passivating contacts for silicon solar cells

被引:9
作者
Wratten, A. [1 ]
Pain, S. L. [1 ]
Yadav, A. [1 ]
Khorani, E. [1 ]
Niewelt, T. [1 ,2 ,3 ]
Black, L. [4 ]
Bartholazzi, G. [4 ]
Walker, D. [5 ]
Grant, N. E. [1 ]
Murphy, J. D. [1 ]
机构
[1] Univ Warwick, Sch Engn, Coventry CV4 7AL, England
[2] Fraunhofer Inst Solar Energy Syst ISE, Heidenhofstr 2, D-79110 Freiburg, Germany
[3] Univ Freiburg, Lab Photovolta Energy Convers, Emmy Noether Str 2, D-79110 Freiburg, Germany
[4] Australian Natl Univ, Sch Engn, Canberra 2600, Australia
[5] Univ Warwick, Dept Phys, Coventry CV4 7AL, England
基金
英国科学技术设施理事会; 英国工程与自然科学研究理事会;
关键词
Silicon; Passivation; Contact; HfO2; Atomic layer deposition; SURFACE PASSIVATION; CRYSTALLINE SILICON; FORCE MICROSCOPY; HFO2; TRANSITION; EXTRACTION; MECHANISM; LAYERS; FILMS;
D O I
10.1016/j.solmat.2023.112457
中图分类号
TE [石油、天然气工业]; TK [能源与动力工程];
学科分类号
0807 ; 0820 ;
摘要
We investigate the potential of ultra-thin HfO2 films grown by atomic layer deposition for passivating contacts to silicon focusing on variations in film thickness and post-deposition annealing temperature. A peak in passivation quality - as assessed by carrier lifetime measurements - is reported for 2.2 nm thick films annealed at 475 degrees C, for which a surface recombination velocity <1 cm/s is determined. For films <2.2 nm thick, there is a marked decrease in passivation quality. X-ray diffraction highlights a change from crystallised monoclinic to amorphous HfO2 as film thickness decreases from 12 nm to 2.2 nm. Kelvin probe results indicate that as-deposited 2.2-12 nm films have similar effective work functions, although the work function of 1 nm films is considerably lower. Upon post-deposition annealing in vacuum, all films exhibit a reduction in effective work function at temperatures coincident with the onset of passivation in air-annealed samples. An initial investigation into the contact resistivity in a passivating contact structure utilizing HfO2 reveals a strong post-deposition annealing temperature dependence, with the lowest resistance achieved below 375 degrees C, followed by a decrease in performance as temperature increases towards the optimal temperature for passivation (475 degrees C). Limitations of the contact structure used are discussed.
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页数:11
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