{"title":"GaAs双极结构中的相互扩散","authors":"W. Li, R. M. Cohen, D. Simons, P. Chi","doi":"10.1109/COMMAD.1996.610097","DOIUrl":null,"url":null,"abstract":"Emitter, base, and collector layers of GaAs with a nominal thickness of 0.5 /spl mu/m each were grown by organometallic vapor phase epitaxy (OMVPE). Each layer contained concentration spikes of the interdiffusion marker, indium. Annealing was performed in an open tube system for 1 h at T=900/spl deg/C using a controlled arsenic pressure. The dopants used, tellurium and carbon, reside on the group V sublattice and they are not expected to induce the so-called kick-out diffusion mechanism. The measured interdiffusion results are consistent with native defect concentrations' which approach their equilibrium values during the annealing process. A small emitter push effect can be measured for npn structures. We find that a Ga vacancy, with a charge of -1, provides a consistent explanation for interdiffusion in both n-type and p-type GaAs over the range of carrier density n=1/spl times/10/sup 19/ cm/sup -3/ to p=1/spl times/10/sup 19/ cm/sup -3/.","PeriodicalId":171952,"journal":{"name":"1996 Conference on Optoelectronic and Microelectronic Materials and Devices. Proceedings","volume":"1 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1996-12-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Interdiffusion in GaAs bipolar structures\",\"authors\":\"W. Li, R. M. Cohen, D. Simons, P. Chi\",\"doi\":\"10.1109/COMMAD.1996.610097\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Emitter, base, and collector layers of GaAs with a nominal thickness of 0.5 /spl mu/m each were grown by organometallic vapor phase epitaxy (OMVPE). Each layer contained concentration spikes of the interdiffusion marker, indium. Annealing was performed in an open tube system for 1 h at T=900/spl deg/C using a controlled arsenic pressure. The dopants used, tellurium and carbon, reside on the group V sublattice and they are not expected to induce the so-called kick-out diffusion mechanism. The measured interdiffusion results are consistent with native defect concentrations' which approach their equilibrium values during the annealing process. A small emitter push effect can be measured for npn structures. We find that a Ga vacancy, with a charge of -1, provides a consistent explanation for interdiffusion in both n-type and p-type GaAs over the range of carrier density n=1/spl times/10/sup 19/ cm/sup -3/ to p=1/spl times/10/sup 19/ cm/sup -3/.\",\"PeriodicalId\":171952,\"journal\":{\"name\":\"1996 Conference on Optoelectronic and Microelectronic Materials and Devices. Proceedings\",\"volume\":\"1 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1996-12-08\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"1996 Conference on Optoelectronic and Microelectronic Materials and Devices. Proceedings\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/COMMAD.1996.610097\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"1996 Conference on Optoelectronic and Microelectronic Materials and Devices. Proceedings","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/COMMAD.1996.610097","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Emitter, base, and collector layers of GaAs with a nominal thickness of 0.5 /spl mu/m each were grown by organometallic vapor phase epitaxy (OMVPE). Each layer contained concentration spikes of the interdiffusion marker, indium. Annealing was performed in an open tube system for 1 h at T=900/spl deg/C using a controlled arsenic pressure. The dopants used, tellurium and carbon, reside on the group V sublattice and they are not expected to induce the so-called kick-out diffusion mechanism. The measured interdiffusion results are consistent with native defect concentrations' which approach their equilibrium values during the annealing process. A small emitter push effect can be measured for npn structures. We find that a Ga vacancy, with a charge of -1, provides a consistent explanation for interdiffusion in both n-type and p-type GaAs over the range of carrier density n=1/spl times/10/sup 19/ cm/sup -3/ to p=1/spl times/10/sup 19/ cm/sup -3/.