Thermal wet oxidation of GaP and Al0.4Ga0.6P J. H. Epple, K. L. Chang, G. W. Pickrell, K. Y. Cheng, and K. C. Hsieh Citation: Appl. Phys. Lett. 77, 1161 (2000); doi: 10.1063/1.1286871 View online: http://dx.doi.org/10.1063/1.1286871 View Table of Contents: http://apl.aip.org/resource/1/APPLAB/v77/i8 Published by the American Institute of Physics. Related Articles Ge redistribution in SiO2/SiGe structures under thermal oxidation: Dynamics and predictions J. Appl. Phys. 111, 024308 (2012) Effect of the capping on the local Mn oxidation state in buried (001) and (110) SrTiO3/La2/3Ca1/3MnO3 interfaces J. Appl. Phys. 110, 103903 (2011) Stress release phenomena in chromia scales formed on NiCr-30 alloys: Influence of metallurgical parameters J. Appl. Phys. 110, 093516 (2011) Electrical properties of thermally oxidized AlInN/AlN/GaN-based metal oxide semiconductor hetero field effect transistors J. Appl. Phys. 110, 084501 (2011) Stress evolution during the oxidation of silicon nanowires in the sub-10 nm diameter regime Appl. Phys. Lett. 99, 143115 (2011) Additional information on Appl. Phys. Lett. Journal Homepage: http://apl.aip.org/ Journal Information: http://apl.aip.org/about/about_the_journal Top downloads: http://apl.aip.org/features/most_downloaded Information for Authors: http://apl.aip.org/authors Downloaded 05 Feb 2012 to 140.114.195.186. Redistribution subject to AIP license or copyright; see http://apl.aip.org/about/rights_and_permissions APPLIED PHYSICS LETTERS VOLUME 77, NUMBER 8 21 AUGUST 2000 Thermal wet oxidation of GaP and Al0.4Ga0.6P J. H. Epple, K. L. Chang, G. W. Pickrell, K. Y. Cheng, and K. C. Hsieha) Department of Electrical and Computer Engineering and Microelectronics Laboratory, University of Illinois at Urbana-Champaign, Urbana, Illinois 61820 共Received 24 March 2000; accepted for publication 19 May 2000兲 Thermal wet oxidations of GaP and Al0.4Ga0.6P at 650 °C for various times have been performed. Comparisons are made on oxidation rates and post oxidation morphology. Transmission electron microscopy shows that when oxidizing GaP, polycrystalline monoclinic GaPO4•2H2O forms without noticeable loss of phosphorus. Oxidation for 6 h or more leads to poor morphology resulting in cracks and detachment. A thickness expansion of about 2.5–3 times is noticed as a result of oxidation. In contrast, oxidized Al0.4Ga0.6P exhibits much better morphology without cracks or detachment from the substrate. The oxide has an almost amorphous-like microstructure. The oxidation process shows typical diffusion-limited reaction at long anneals. Preliminary work on the oxidation of AlP indicates that the reaction leads to formation of Al2O3 and possible volatile P2O5 diffusing out of the specimen. Thus, from the structural viewpoint, AlGaP forms a better oxide suitable for device needs. © 2000 American Institute of Physics. 关S0003-6951共00兲02228-2兴 metalorganic chemical vapor deposition system. The material was grown on a 共100兲 GaP substrate miscut 10° towards the 关111兴 direction. Oxidation was performed in a Lindberg open tube furnace. Water vapor was supplied to the samples using nitrogen bubbled through a water reservoir kept at 85 °C. Samples were oxidized for times ranging from 1 to 36 h at 650 °C. After oxidation, the samples were analyzed using cross-sectional transmission electron microscopy 共TEM兲 to determine oxidation rates, volume changes, and microstructure. Compositions were estimated using energy dispersive x-ray spectroscopy 共EDAX兲. GaP was wet oxidized at 650 °C for varying times up to 24 h. After an oxidation of 6 h the surface of the oxidized GaP began to get very rough, cracked, and detached as was reported for thermal wet oxidations of GaP by Kato et al.8 This can be seen in a Nomarski photograph of the GaP oxidized at 650 °C for 24 h shown in Fig. 1共a兲. This oxide has a thickness of ⬃1.3 m and is obviously very rough and cracked as shown in the cross-sectional TEM micrograph, Fig. 1共b兲. Also seen is the detachment between the oxide and substrate. The oxidized material was identified using TEM diffraction 关insert in Fig. 1共b兲兴 and EDAX. The x-ray spectroscopy confirmed the presence of oxygen and equal atomic concentrations of Ga and P. Among various possible GaPOx compounds listed by the International Center for Diffraction Data, the hydrous monoclinic GaPO4•2H2O is the only structure that matches the TEM diffraction data.11 TEM also showed that the oxide was polycrystalline without any preferred crystal orientation correlation between the oxide and substrate. GaP oxidized for less than 6 h did not have as severe structural damage or detachment. However, there were noticeable spots on the surface. It was also noticed that the oxide was 2.5–3 times the thickness of the original material. This can be attributed to the absorption of O and H2O. It is indicated by the breakdown after longer oxidation times that there is likely a critical volume for the highly strained oxide at which it will crack and detach from the substrate. For a comparison, published results on the oxidation of For decades the oxidation of many compound semiconductors has been investigated to yield native oxides for different applications. Most beneficial has been the study of oxidizing Alx Ga1⫺x As. 1 This technology has been used for numerous applications such as distributed Bragg reflectors in vertical cavity surface emitting lasers,2,3 insulating layers in field effect transistors, and current guiding in heterojunction bipolar transistors.4–6 Less extensive work has been done to study the materials grown on GaP. Rubenstein and Kato et al. have studied the thermal dry oxidation of GaP.7,8 They reported that the product of the oxidation was mostly GaPO4 with very little Ga2O3. This is in contrast to both GaAs and GaSb, which when oxidized form primarily Ga2O3 with the As and Sb forming volatile oxides that diffuse out of the sample. Dry oxidations for 30 min at temperature of 850 °C resulted in the GaPO4 being very rough with caverns forming at the oxide/substrate interface. In contrast, when GaP was thermally wet oxidized the material was smoother without the cavern formation but was cracked and separated from the substrate.8 It was determined that thermally oxidized GaP could not be used for device applications. Following this there was much work done on the anodic oxidation of GaP. Schwartz experimented with annealing anodically oxidized GaP with various P2O5 overpressures to formulate a Ga–P–O ternary phase diagram.9 The anodic oxide consisted of P2O5 and Ga2O3. His results indicated that GaPO4 formed after annealing. Kato et al. also did work annealing anodically oxidized GaP in a nitrogen ambient instead of P2O5 overpressure.10 It was found that when the anodic oxide was annealed at temperatures above 600 °C, the surface became very rough with hollow bumps and blisters believed to be caused by vaporization of P2O5 in the material. In this letter results are presented on the thermal wet oxidation of both Al0.4Ga0.6P and GaP. A 1.5 m Al0.4Ga0.6P layer was grown in an Emcore GS 3000 DFM low-pressure a兲 Electronic mail: [email protected] 0003-6951/2000/77(8)/1161/3/$17.00 1161 © 2000 American Institute of Physics Downloaded 05 Feb 2012 to 140.114.195.186. Redistribution subject to AIP license or copyright; see http://apl.aip.org/about/rights_and_permissions 1162 Epple et al. Appl. Phys. Lett., Vol. 77, No. 8, 21 August 2000 FIG. 2. Oxidation distance vs time for Al0.4Ga0.6P oxidized at 650 °C. FIG. 1. Nomarski photograph 共a兲 and TEM and diffraction pattern 共b兲 of GaP oxidized at 650 °C for 24 h. The GaP is cracked and damaged. Note the detachment at the oxide/substrate interface. The TEM also shows the material is polycrystalline. A typical diffraction of a small grain is shown in the insert, and diffraction analysis indicates that the material is monoclinic GaPO4 •2H2O. GaAs were analyzed. Rubenstein published data on the oxidation of GaAs with his GaP work.7 It is proposed that upon wet oxidation, GaAs forms Ga2O3 and some volatile material such as As2O3 that diffuses out of the sample. Also, Oh et al.12 have noticed that thermal wet oxidation of GaAs leads to a volume shrinkage of about 5%–10%. Thus, GaP and GaAs oxidize very differently. GaP will retain its column-V element and will form GaPO4 whereas GaAs will not hold on to its column-V element and will form Ga2O3 leaving the As to form volatile compounds. This suggests that the formation of GaPO4 is more favorable than that of Ga2O3. With the recent success in various applications of wet oxidized Al-bearing arsenides, it is of interest to study the oxidation of Alx Ga1⫺x P. Two different aluminum contents have been chosen for the study, i.e., 40% and 100%. To study the oxidation of AlP, a sample was grown with 1500 Å of GaP covering a 1000 Å AlP layer. The AlP was then oxidized from the top down through the GaP cap layer at 650 °C for a sufficiently long time and analyzed by TEM. The resulting material showed again the presence of oxygen but with a significant drop in the P content as compared to aluminum. The P likely forms P2O5 and diffuses out of the sample. In addition, the loss of P results in a volume shrink- age of about 10%. Apparently, the oxidation mechanism of AlP is very different from that of GaP. Sugg et al. studied the thermal wet oxidation of Al0.8Ga0.2As. 13 It was found that after oxidation the material was mostly polycrystalline ␥ -Al2O3 with As being below the detection level for Auger electron spectroscopy. At the oxidation temperatures used 共⬃425 °C兲 it was found that Ga did not oxidize. Thus, the resulting products are Al2O3 and elemental Ga. Choquette et al. presented information on the thermal wet oxidation of AlAs.14 It is stated that when AlAs reacts with water the products are ␥ -Al2O3, As2O3, and H2. Thermodynamically, As2O3 can react with H2 to form elemental As, and both As2O3 and As are volatile.15 They can easily diffuse and escape from the sample. As a result of the material loss, a volume shrinkage of 12%–13% after oxidation is experimentally observed. Hence, the results of oxidizing AlP in this work are similar to those of oxidizing AlAs. The Al easily forms Al2O3 leaving the column-V element to form volatile compounds. Oxidations of Al0.4Ga0.6P were done for various times up to 36 h at 650 °C. The oxidation thickness versus time is shown in Fig. 2. It should be noted that the graph indicates growth of the oxide and not consumption of the material being oxidized. As can be seen in Fig. 2, the oxidation rate starts out at about 700 Å/h but begins to slow as oxidation times approach 20 h. This roll off is caused by the oxidation becoming diffusion limited rather than reaction limited. On the oxidation layer, EDAX showed that the relative amount of P dropped slightly compared to the as-grown sample. This indicates there was some loss of P due to the oxidation. It is believed that some volatile P2O5 has formed and diffused out of the sample. This phenomenon was not noticed in GaP. After the oxidation it was found the material swelled to roughly twice its original volume. Compared to oxidized GaP, the volume expansion 共increase in thickness兲 of oxidized Al0.4Ga0.6P is smaller, which further supports the notion that AlP shrinks upon wet oxidation probably due to the loss of volatile P2O5. The postoxidation morphology of the Al0.4Ga0.6P and GaP can be used as evidence that the damage to oxidized material is caused by excessive expansion of a polycrystalline material. A Nomarski photograph of Al0.4Ga0.6P oxidized at 650 °C for 24 h is shown in Fig. 3共a兲. The oxidized Al0.4Ga0.6P has a thickness of ⬃1.5 m and is very smooth. Downloaded 05 Feb 2012 to 140.114.195.186. Redistribution subject to AIP license or copyright; see http://apl.aip.org/about/rights_and_permissions Epple et al. Appl. Phys. Lett., Vol. 77, No. 8, 21 August 2000 1163 from ellipsometer measurements that the index of refraction is ⬃1.7–1.8, which is significantly smaller than those of crystalline AlGaP. In conclusion, GaP and Al0.4Ga0.6P are oxidized at 650 °C for various times up to 36 h. The result of the GaP oxidation is the formation of polycrystalline monoclinic GaPO4 •2H2O. This material tends to have poor structural quality and detaches from the substrate, probably due to a large volume expansion. Oxidizing a buried layer of AlP shows similarities to AlAs in that the column-V element diffuses out of the sample leaving Al2O3 and showing a volume shrinkage. Al0.4Ga0.6P oxidizes at a faster rate than does GaP and the resulting oxide has a smooth morphology with no cracking or detachment even after 36 h of oxidation despite an expanded volume. The smooth morphology and large change in the index of refraction makes the oxide attractive for different applications in passivation and waveguiding. The authors greatly appreciate the use of the facility at the Center for Microanalysis of Materials, University of Illinois, which is supported by the U.S. Department of Energy under Grant No. DEFG02-91-ER45439. This work is further supported by DARPA DAAG 55-98-1-0303 and F49602-981-10496. 1 FIG. 3. Nomarski photograph 共a兲 and TEM and diffraction pattern 共b兲 of Al0.4Ga0.6P oxidized at 650 °C for 24 h. The Nomarski photograph shows the oxidized material is very smooth in contrast to the oxidized GaP. The TEM diffraction analysis indicates that the material is practically amorphous. Shown in Fig. 3共b兲 is the TEM micrograph of the Al0.4Ga0.6P after oxidation. In contrast to GaP, the oxidized Al0.4Ga0.6P has no noticeable structural problems as seen in the oxidized GaP. The diffraction pattern in Fig. 3共b兲 shows practically only amorphous rings, which indicates that the oxidized Al0.4Ga0.6P either consists of extremely fine polycrystalline grains or is basically amorphous in structure. This is in contrast to the obvious polycrystalline material after the oxidation of GaP. It is possible that when the Al0.4Ga0.6P is oxidized it forms a glassy phase material that conforms to the substrate. This material is not subject to the same problems caused by large expansion the way polycrystalline material is. Thus, instead of being cracked and detached the material is smooth and adheres well. This is an important advantage to the oxidation of Alx Ga1⫺x P. In addition, it was found J. M. Dallesasse, N. Holonyak, Jr., A. R. Sugg, T. A. Richard, and N. El-Zein, Appl. Phys. Lett. 57, 2844 共1990兲. 2 K. D. Choquette, K. L. Lear, R. P. Schneider, Jr., and K. M. Geib, Appl. Phys. Lett. 66, 3413 共1995兲. 3 J. J. Wierer, P. W. Evans, N. Holonyak, Jr., and D. A. Kellogg, Appl. Phys. Lett. 71, 2286 共1997兲. 4 E. I. Chen, N. Holonyak, Jr., and S. A. Maranowski, Appl. Phys. Lett. 66, 2688 共1995兲. 5 A. Massengale, M. C. Larson, C. Dai, and J. S. Harris, Jr., Electron. Lett. 32, 399 共1996兲. 6 P. A. Parikh, P. M. Chavarkar, and U. K. Mishra, IEEE Electron Device Lett. 18, 111 共1997兲. 7 M. Rubenstein, J. Electrochem. Soc. 113, 540 共1966兲. 8 Y. Kato, K. M. Geib, R. G. Gann, P. R. Brusenback, and C. W. Wilmsen, J. Vac. Sci. Technol. A 2, 588 共1984兲. 9 G. P. Schwartz, G. J. Gualtieri, J. E. Griffiths, C. D. Thurmond, and B. Schwartz, J. Electrochem. Soc. 127, 2488 共1980兲. 10 Y. Kato, K. M. Geib, R. G. Gann, P. R. Brusenback, and C. W. Wilmsen, J. Vac. Sci. Technol. B 9, 1530 共1991兲. 11 JCPDS Powder Diffraction File, International Centre for Diffraction Data 共1994兲. 12 T. H. Oh, D. L. Huffaker, L. A. Graham, H. Deng, and D. G. Deppe, Electron. Lett. 32, 2024 共1996兲. 13 A. R. Sugg, E. I. Chen, N. Holonyak, Jr., K. C. Hsieh, J. E. Baker, and N. Finnegan, J. Appl. Phys. 74, 3880 共1993兲. 14 K. D. Choquette, K. M. Geib, C. I. H. Ashby, R. D. Twesten, O. Blum, H. Q. Hou, D. M. Follstaedt, B. E. Hammons, D. Mathes, and R. Hull, IEEE J. Sel. Top. Quantum Electron. 3, 916 共1997兲. 15 C. I. H. Ashby, J. P. Sullivan, P. P. Newcomer, N. A. Missert, H. Q. Huo, B. E. Hammons, M. J. Hafich, and A. G. Baca, Appl. Phys. Lett. 70, 2443 共1997兲. Downloaded 05 Feb 2012 to 140.114.195.186. Redistribution subject to AIP license or copyright; see http://apl.aip.org/about/rights_and_permissions
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