Comparison of surface photovoltage behavior for n-type versus p-type GaN

被引:17
作者
Foussekis, M. [1 ]
Baski, A. A. [1 ]
Reshchikov, M. A. [1 ]
机构
[1] Virginia Commonwealth Univ, Dept Phys, Richmond, VA 23284 USA
来源
JOURNAL OF VACUUM SCIENCE & TECHNOLOGY B | 2011年 / 29卷 / 04期
基金
美国国家科学基金会;
关键词
adsorption; desorption; gallium compounds; III-V semiconductors; semiconductor epitaxial layers; semiconductor growth; surface photovoltage; ultraviolet radiation effects; vapour phase epitaxial growth; wide band gap semiconductors; NEGATIVE ELECTRON-AFFINITY; GALLIUM NITRIDE; GROWN GAN; FIELD; EPITAXY; FILMS;
D O I
10.1116/1.3605299
中图分类号
TM [电工技术]; TN [电子技术、通信技术];
学科分类号
0808 ; 0809 ;
摘要
Using a Kelvin probe, the authors have studied changes in surface contact potential during illumination, i.e., surface photovoltage (SPV), for n- and p-type GaN films grown by hydride vapor phase epitaxy. Short ultraviolet (UV) exposures (3 s) generate a positive SPV of about 0.5 eV for n-type and a negative SPV of about -0.6 eV for p-type GaN, which is consistent with the expected surface band bending for these two surface types. The fast component of the SPV is attributed to the accumulation of photogenerated holes (n-type) or electrons (p-type) at the surface, which results in a decrease in band bending. During long UV exposures (1 h), however, slower photoinduced processes can cause the SPV signal to change as a function of the ambient conditions. For both n- and p-type GaN, UV illumination causes the adsorption of negatively charged oxygen species on the surface in air and their subsequent desorption in vacuum. It appears that this adsorbate effect is most prevalent for n-type GaN in vacuum and p-type GaN in air, with significant changes in the SPV of up to 0.3 eV (n-type) and 0.6 eV (p-type). One important difference between the GaN films is the sensitivity of p-type GaN to the illumination geometry. When the sample contacts are exposed to near-bandgap light, unexpected offsets of the SPV signal can result. If such offsets are appropriately taken into account, however, then the SPV behaviors for both n- and p-type GaN can be reasonably modeled by thermionic expressions. (C) 2011 American Vacuum Society. [DOI: 10.1116/1.3605299]
引用
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页数:6
相关论文
共 22 条
[1]  
BEIRERLEIN TA, 2007, SYNTHETIC MET, V111, P295
[2]   Study of oxygen chemisorption on the GaN(0001)-(1x1) surface [J].
Bermudez, VM .
JOURNAL OF APPLIED PHYSICS, 1996, 80 (02) :1190-1200
[3]   Electric field effects on excitons in gallium nitride [J].
Binet, F ;
Duboz, JY ;
Rosencher, E ;
Scholz, F ;
Harle, V .
PHYSICAL REVIEW B, 1996, 54 (11) :8116-8121
[4]   Negative electron affinity of cesiated p-GaN(0001) surfaces [J].
Eyckeler, M ;
Monch, W ;
Kampen, TU ;
Dimitrov, R ;
Ambacher, O ;
Stutzmann, M .
JOURNAL OF VACUUM SCIENCE & TECHNOLOGY B, 1998, 16 (04) :2224-2228
[5]  
FERGUSON JD, 2009, MAT RES SOC S P, V1202
[6]   Photoadsorption and photodesorption for GaN [J].
Foussekis, M. ;
Baski, A. A. ;
Reshchikov, M. A. .
APPLIED PHYSICS LETTERS, 2009, 94 (16)
[7]  
FRANZ W, 1958, Z NATURFORSCH PT A, V13, P484
[8]   Mechanisms of current collapse and gate leakage currents in AlGaN/GaN heterostructure field effect transistors [J].
Hasegawa, H ;
Inagaki, T ;
Ootomo, S ;
Hashizume, T .
JOURNAL OF VACUUM SCIENCE & TECHNOLOGY B, 2003, 21 (04) :1844-1855
[9]   Characterization of band bendings on Ga-face and N-face GaN films grown by metalorganic chemical-vapor deposition [J].
Jang, HW ;
Lee, JH ;
Lee, JL .
APPLIED PHYSICS LETTERS, 2002, 80 (21) :3955-3957
[10]  
KELDYSH LV, 1958, SOV PHYS JETP-USSR, V7, P788