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Ohmic contacts to p-type GaP
dc.creator | Jorge Estevez, Humberto Angel | |
dc.date.accessioned | 2012-06-07T22:45:10Z | |
dc.date.available | 2012-06-07T22:45:10Z | |
dc.date.created | 1996 | |
dc.date.issued | 1996 | |
dc.identifier.uri | https://hdl.handle.net/1969.1/ETD-TAMU-1996-THESIS-J675 | |
dc.description | Due to the character of the original source materials and the nature of batch digitization, quality control issues may be present in this document. Please report any quality issues you encounter to digital@library.tamu.edu, referencing the URI of the item. | en |
dc.description | Includes bibliographical references. | en |
dc.description | Issued also on microfiche from Lange Micrographics. | en |
dc.description.abstract | The objective of thisresearch was to develop ohmic contact schemes of low resistance, i.e. in the mid10-1 QCM2, to p-type Gallium Phosphide by the mechanism of solid-phase regrowth. The contact resistivityof the samples fabricated in this work was measured by the Cox-Strack method. Ohmic contacts based on the Zn/Pd system were developed. The Zn(350A)/Pd(IOOA)/p-GaP and Zn(350A)/Pd(IOOA)/p-GaP gave rather high values of the contact resistivity, 3-8xl 0-4 f2CM2. An improvement in the contact resistivity was achieved by developing the Si(750A)/Pd(400A)/Zn(xA)/Pd(IOOA)/p-GaP scheme. Values of the contact resistivity in the range of 3xlO-5 to 7xlO-' nCM2 were obtained. It was found that the optimum Zn layer thickness is 30 A for the Pd and Si thickness used in this scheme. The samples were annealed for I @n at temperatures ranging from 3 5 0 to 4 5 0 'C. Lower values of the contact resistivity than those of the Si/Pd/Zn/Pd/p-GaP scheme were achieved by depositing an Aluminum layer on the top of the Si/Pd/Zn/Pd/p-GaP system. Values of the contact resistivity in the range of 2xl 0-5 f2CM2 to 5xlO-5 flcM2 were achieved for the contacts AI(IOOOA)/Si(750A)/Pd(400A)/Zn(30A)/Pd(IOOA)/p-GaPand AI(200A)/Si(750A)/Pd(400A)/Zn(30A)/Pd(IOOA)/p-GaP, respectively. The low values of the contact resistivity were attributed to the formation of a heavilydoped surface layer beneath the contact area. The doping concentration of this surface layer was estimated by using theoretical plots of the contact resisvity versus doping concentration. | en |
dc.format.medium | electronic | en |
dc.format.mimetype | application/pdf | |
dc.language.iso | en_US | |
dc.publisher | Texas A&M University | |
dc.rights | This thesis was part of a retrospective digitization project authorized by the Texas A&M University Libraries in 2008. Copyright remains vested with the author(s). It is the user's responsibility to secure permission from the copyright holder(s) for re-use of the work beyond the provision of Fair Use. | en |
dc.subject | electrical engineering. | en |
dc.subject | Major electrical engineering. | en |
dc.title | Ohmic contacts to p-type GaP | en |
dc.type | Thesis | en |
thesis.degree.discipline | electrical engineering | en |
thesis.degree.name | M.S. | en |
thesis.degree.level | Masters | en |
dc.type.genre | thesis | en |
dc.type.material | text | en |
dc.format.digitalOrigin | reformatted digital | en |
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