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dc.contributor.advisorTonio Buonassisi.en_US
dc.contributor.authorLenahan, Frances Daggetten_US
dc.contributor.otherMassachusetts Institute of Technology. Department of Materials Science and Engineering.en_US
dc.date.accessioned2016-09-13T18:09:57Z
dc.date.available2016-09-13T18:09:57Z
dc.date.copyright2016en_US
dc.date.issued2016en_US
dc.identifier.urihttp://hdl.handle.net/1721.1/104147
dc.descriptionThesis: S.B., Massachusetts Institute of Technology, Department of Materials Science and Engineering, 2016.en_US
dc.descriptionThis electronic version was submitted by the student author. The certified thesis is available in the Institute Archives and Special Collections.en_US
dc.descriptionCataloged from student-submitted PDF version of thesis.en_US
dc.descriptionIncludes bibliographical references (pages 54-55).en_US
dc.description.abstractThe growth and maintenance of the modern technological world requires immediate solutions in the field of clean, renewable energy. One prominent solution is the rapid advancement of solar cell technologies due to the wide availability of solar energy and the growing versatility of harnessing it. As efficiencies for these devices creep upwards, it becomes increasingly more important to find the greatest inhibiting factor. Through a solar cell simulator program (SCAPS), improvements in the minority-carrier lifetime of cell materials show not only significant improvements in cell efficiencies, but also an un-masking of improvements by other properties, which are inhibited when the lifetime is too short. This work aims to calculate the mobilitylifetime products ([mu][tau]) of gallium arsenide (GaAs) and annealed and un-annealed tin sulfide (SnS) with respective p-doping carrier concentrations of 1018 cm-3, 1016 cm-3, and 1015 cm-3 through photoconductivity measurements. Films are 1 [mu]m thick and have a four-bar and two-bar contact configuration to model carrier conductivity as a sheet. For calculations, two methods of modeling charge carrier generation are considered; a uniform generation throughout the film and a depth and wavelength-dependent generation. This work found values on the order of 10-1 cm2 V-1, 10-4 cm2 V-1, and 10-5 cm2 V-1, for GaAs, annealed SnS, and un-annealed SnS, respectively, for both methods of calculation. The simplified approach considering a uniform generation yielded lower results than the depth and wavelength dependent calculations by about a factor of two. All values were three to four orders of magnitude higher than those found in the literature. For this reason, it is believed that the majority-carrier is dominating measurements due to an inhibited minority-carrier lifetime.en_US
dc.description.statementofresponsibilityby Frances Daggett Lenahan.en_US
dc.format.extent59 pagesen_US
dc.language.isoengen_US
dc.publisherMassachusetts Institute of Technologyen_US
dc.rightsM.I.T. theses are protected by copyright. They may be viewed from this source for any purpose, but reproduction or distribution in any format is prohibited without written permission. See provided URL for inquiries about permission.en_US
dc.rights.urihttp://dspace.mit.edu/handle/1721.1/7582en_US
dc.subjectMaterials Science and Engineering.en_US
dc.titlePhotoconductivity and minority carrier lifetime in tin sulfide and gallium arsenide semiconductors for photovoltaicsen_US
dc.typeThesisen_US
dc.description.degreeS.B.en_US
dc.contributor.departmentMassachusetts Institute of Technology. Department of Materials Science and Engineering
dc.identifier.oclc958278833en_US


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