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Student Project Abstracts 2005 - Pluto - University of Washington

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facethef therfaceding, theITOthird layer, DBR, was scanned with ITOand glass layers below it. Additional measurements with a surfacepr<strong>of</strong>iler were done to analysis theroughness Figure 7. Dynamic <strong>of</strong> the Modulation individual Measurement layers Schematic <strong>of</strong> theFabry-Perot Etalon device. Each surfaceAdditional was scanned measurements in sequence with a surface with preceding pr<strong>of</strong>iler were donematerial layers in place. For example, theto analysisthirdthelayer,roughnessDBR,<strong>of</strong>wasthe individualscannedlayerswith<strong>of</strong>ITOthe Fabry-Perot Etalon and glass device. layers Each below surface it. was scanned in sequence withAdditional measurements with a surfacepreceding material layers in place. For example, the third layer,pr<strong>of</strong>ilerDBR, were done to analysis thewas scanned with ITO and glass layers below it.roughness By varying<strong>of</strong> the the voltage individual over alayers range<strong>of</strong> <strong>of</strong>the60Fabry-Perot V, the shiftsEtalon in device. were Each observed. surfacewas Afterscanned normalizing RESULTSin sequence/ the DISCUSSION shift with wavelengths, precedingBythevaryingaveragetheshiftvoltagewasovercalculated.material layers in place. a range For example, <strong>of</strong> 60 V, the the shifts inFigure third 8 were layer, observed. DBR, After was normalizing scanned the with shift wavelengths, ITOthe average shift was calculated.and glass layers below it.By varying the voltage over a range <strong>of</strong> 60V, the shifts in were observed.After normalizing the shift wavelengths,the average shift was calculated.ExtinctionFigure measurements 9. Shift Measurement Results also showpromising results with an extinction ratioExtinction measured measurements at 5 Volts. also The show extinction promising ratio results withan extinction is theratio logmeasured ratio <strong>of</strong>at the 5 Volts. intensity The extinction at 0 volts ratio is thelog ratio compared <strong>of</strong> the intensity to the at 0 volts intensity compared at to anthe applied intensity at anapplied voltage.4 CMDITR Review <strong>of</strong> Undergraduate Research Vol. 1 No. 1 Summer 20044 CMDITR Review <strong>of</strong> Undergraduate Research Vol. 1 No. 1 Summer 2004Figure10: Extinction Results TCBD Sol-gelExtinction measurements also showEBY promising results with an extinction ratiomeasured at 5 Volts. The extinction ratiois the Surface log ratio analysis <strong>of</strong> the <strong>of</strong> the intensity sample was at shown 0 volts to be a major factorin the performance <strong>of</strong> the device. Scans <strong>of</strong> the different deviceExtinction compared tomeasurements the intensity atalso an applied showpromising voltage.levels are results with an extinction ratioshown along with the average standard deviation values.See Figures 11,measured at 5 Volts. The extinction ratio12.By varying the voltage over a range <strong>of</strong> 60V, the shifts in were observed.After normalizing the shift wavelengths,the average shift was calculated. is the log Surface ratioanalysis <strong>of</strong> the intensity <strong>of</strong> the sample at 0 volts was showncompared to beto a the major intensity factor inat the an performance applied <strong>of</strong>voltage.DBRSurface analysis <strong>of</strong> the sample ITOwas shownto be a major factor in the performance <strong>of</strong>the device. Scans <strong>of</strong> the different Glass devicelevels are shown along with the averagestandard deviation values. See Surfacethe analysis device. <strong>of</strong> Scans the Figure sample 8: <strong>of</strong>Surface the was Scans different shown deviceto be alevels major are factor shown in thealong performance with the<strong>of</strong>averagethe device. standard Scans deviation <strong>of</strong> the different values. device See levels are shown along with the averageTCBD Sol-Gelstandard deviation values. See DBR 4 CMDITR Review <strong>of</strong> Undergraduate Research Vol. 1 No. 1 Summer 2004 ITOGlassSurface analysis <strong>of</strong> the sample was shownto be a major factor in the performance <strong>of</strong>TCBD Sol-Gel DBRFigure 12. Probability Density Distribution for TCBD Sol-Gel standard ITOThe average standard deviation shown deviation below is shown the value obtainedfrom averaging Glassbelow is thethe distributionvalue obtained<strong>of</strong> each surfacefromscan. Sixor more scans for each surface were recorded. The DBR mirroraveraging the distribution <strong>of</strong> each surfaceis the roughest surface in the device. This has implications in thescan. Six or more scans for each surfacedevice performance as the roughness can be directly tied to thewereperformancerecorded. The DBR mirror is the<strong>of</strong> the device.roughest surface in the device. This hasimplications in the device performance asthe roughness can be directly tied to theperformance <strong>of</strong> the device.SurfaceTCBD Sol-GelDBR MirrorITOGlassTCBD Sol-GelAverage Standard Deviation3.02 nm5.36 nm1.36 nm2.31 nm Table 1. Indication <strong>of</strong> Roughness from Surface Scanning <strong>of</strong> MaterialsCMDITR Review <strong>of</strong> Undergraduate Research Vol. 2 No. 1 Summer <strong>2005</strong> 37avperPeITImmapuper1.Un2.Jou3.AnLig4.M.Jen15NaUnCo

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