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dc.contributor.authorChiang, Ching-Yuen_US
dc.contributor.authorHsiao, Sheng-Weien_US
dc.contributor.authorWu, Pin-Jiunen_US
dc.contributor.authorYang, Chu-Shouen_US
dc.contributor.authorChen, Chia-Haoen_US
dc.contributor.authorChou, Wu-Chingen_US
dc.date.accessioned2017-04-21T06:55:11Z-
dc.date.available2017-04-21T06:55:11Z-
dc.date.issued2016-09-14en_US
dc.identifier.issn1944-8244en_US
dc.identifier.urihttp://dx.doi.org/10.1021/acsami.6b03869en_US
dc.identifier.urihttp://hdl.handle.net/11536/134232-
dc.description.abstractUtilizing a scanning photoelectron microscope (SPEM) and grazing-incidence X-ray powder diffraction (GIXRD), we studied the electronic band structure and the crystalline properties of the pentanary Cu(In,Ga)(S,Se)(2) (CIGSSe) thin-film solar cell as a function of sample depth on measuring the thickness-gradient sample. A novel approach is proposed for studying the depth-dependent information on thin films, which can provide a gradient thickness and a wide cross-section of the sample by polishing process. The results exhibit that the CIGSSe absorber layer possesses four distinct stoichiometries. The growth mechanism of this distinctive compositional: distribution formed by a two stage process is described according to the thermodynamic reaction and the manufacturing, process. On the basis of the depth-profiling results, the gradient profiles of the conduction and valence bands were constructed to elucidate the performance of the electrical properties (in this case, V-oc = 620 mV, J(sc) = 34.6 mA/cm(2), and eta = 14.04%); the valence-band maxima (VBM) measured with a SPEM in the spectroscopic mode coincide with this band-structure model, except for a lowering of the VBM observed in the surface region of the absorber layer due to the ordered defect compound (ODC). In addition, the depth-dependent texturing X-ray diffraction pattern presents the crystalline quality and the residual stress for each depth of a thin-film device. We find that the randomly oriented grains in the bottom region of the absorber layer and the different residual stress between the underlying Mo and the absorber interface, which can deteriorate the electrical performance due to peeling-off effect. An anion interstitial defect can be observed on comparing the anion concentration, of the elemental distribution with crystalline composition; a few excess sulfur atoms insert in interstitial sites at the front side of the absorber layer, whereas the interstitial selenium atoms insert at the back side.en_US
dc.language.isoen_USen_US
dc.subjectCIGSSeen_US
dc.subjectsolar cellen_US
dc.subjectscanning photoelectron microscope (SPEM)en_US
dc.subjectgrazing-incidence X-ray powder diffraction (GIXRD)en_US
dc.subjectpolishingen_US
dc.subjectband diagramen_US
dc.subjectresidual stressen_US
dc.subjectordered defect compound (ODC)en_US
dc.titleDepth-Profiling Electronic and Structural Properties of Cu(In,Ga)(S,Se)(2) Thin-Film Solar Cellen_US
dc.identifier.doi10.1021/acsami.6b03869en_US
dc.identifier.journalACS APPLIED MATERIALS & INTERFACESen_US
dc.citation.volume8en_US
dc.citation.issue36en_US
dc.citation.spage24152en_US
dc.citation.epage24160en_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.identifier.wosnumberWOS:000383412000079en_US
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