Diffusion Length Mapping for Dye-Sensitized Solar Cells

The diffusion length (L) of photogenerated carriers in the nanoporous electrode is a key parameter that summarizes the collection efficiency behavior in dye-sensitized solar cells (DSCs). At present, there are few techniques able to spatially resolve L over the active area of the device. Most of the...

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Main Authors: Lucio Cinà, Babak Taheri, Andrea Reale, Aldo Di Carlo
Format: Article
Language:English
Published: MDPI AG 2016-08-01
Series:Energies
Subjects:
Online Access:http://www.mdpi.com/1996-1073/9/9/686
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author Lucio Cinà
Babak Taheri
Andrea Reale
Aldo Di Carlo
author_facet Lucio Cinà
Babak Taheri
Andrea Reale
Aldo Di Carlo
author_sort Lucio Cinà
collection DOAJ
description The diffusion length (L) of photogenerated carriers in the nanoporous electrode is a key parameter that summarizes the collection efficiency behavior in dye-sensitized solar cells (DSCs). At present, there are few techniques able to spatially resolve L over the active area of the device. Most of them require contact patterning and, hence, are intrinsically destructive. Here, we present the first electron diffusion length mapping system for DSCs based on steady state incident photon to collected electron (IPCE) conversion efficiency ( η I P C E ) analysis. The measurement is conducted by acquiring complete transmittance ( T DSC ) and η I P C E spectra from the photo electrode (PE) and counter electrode (CE) for each spatial point in a raster scan manner. L ( x , y ) is obtained by a least square fitting of the IPCE ratio spectrum ( I P C E R = η I P C E -CE η I P C E -PE ). An advanced feature is the ability to acquire η I P C E spectra using low-intensity probe illumination under weakly-absorbed background light (625 nm) with the device biased close to open circuit voltage. These homogeneous conditions permit the linearization of the free electron continuity equation and, hence, to obtain the collection efficiency expressions ( η COL-PE and η COL-CE ). The influence of the parameter’s uncertainty has been quantified by a sensitivity study of L. The result has been validated by quantitatively comparing the average value of L map with the value estimated from electrochemical impedance spectroscopy (EIS).
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spelling doaj.art-71afd424b6f7444c86517b8488182a162022-12-22T02:20:58ZengMDPI AGEnergies1996-10732016-08-019968610.3390/en9090686en9090686Diffusion Length Mapping for Dye-Sensitized Solar CellsLucio Cinà0Babak Taheri1Andrea Reale2Aldo Di Carlo3Centre for Hybrid and Organic Solar Energy (C.H.O.S.E.), Department of Electronic Engineering, University of Rome “Tor Vergata”, via del Politecnico 1, 00133 Rome, ItalyCentre for Hybrid and Organic Solar Energy (C.H.O.S.E.), Department of Electronic Engineering, University of Rome “Tor Vergata”, via del Politecnico 1, 00133 Rome, ItalyCentre for Hybrid and Organic Solar Energy (C.H.O.S.E.), Department of Electronic Engineering, University of Rome “Tor Vergata”, via del Politecnico 1, 00133 Rome, ItalyCentre for Hybrid and Organic Solar Energy (C.H.O.S.E.), Department of Electronic Engineering, University of Rome “Tor Vergata”, via del Politecnico 1, 00133 Rome, ItalyThe diffusion length (L) of photogenerated carriers in the nanoporous electrode is a key parameter that summarizes the collection efficiency behavior in dye-sensitized solar cells (DSCs). At present, there are few techniques able to spatially resolve L over the active area of the device. Most of them require contact patterning and, hence, are intrinsically destructive. Here, we present the first electron diffusion length mapping system for DSCs based on steady state incident photon to collected electron (IPCE) conversion efficiency ( η I P C E ) analysis. The measurement is conducted by acquiring complete transmittance ( T DSC ) and η I P C E spectra from the photo electrode (PE) and counter electrode (CE) for each spatial point in a raster scan manner. L ( x , y ) is obtained by a least square fitting of the IPCE ratio spectrum ( I P C E R = η I P C E -CE η I P C E -PE ). An advanced feature is the ability to acquire η I P C E spectra using low-intensity probe illumination under weakly-absorbed background light (625 nm) with the device biased close to open circuit voltage. These homogeneous conditions permit the linearization of the free electron continuity equation and, hence, to obtain the collection efficiency expressions ( η COL-PE and η COL-CE ). The influence of the parameter’s uncertainty has been quantified by a sensitivity study of L. The result has been validated by quantitatively comparing the average value of L map with the value estimated from electrochemical impedance spectroscopy (EIS).http://www.mdpi.com/1996-1073/9/9/686mappinglight-beam-induced current (LBIC)diffusion lengthdye-sensitized solar cells (DSCs)spectrally-resolved analysis by transmittance and efficiency mapping (SATEM)
spellingShingle Lucio Cinà
Babak Taheri
Andrea Reale
Aldo Di Carlo
Diffusion Length Mapping for Dye-Sensitized Solar Cells
Energies
mapping
light-beam-induced current (LBIC)
diffusion length
dye-sensitized solar cells (DSCs)
spectrally-resolved analysis by transmittance and efficiency mapping (SATEM)
title Diffusion Length Mapping for Dye-Sensitized Solar Cells
title_full Diffusion Length Mapping for Dye-Sensitized Solar Cells
title_fullStr Diffusion Length Mapping for Dye-Sensitized Solar Cells
title_full_unstemmed Diffusion Length Mapping for Dye-Sensitized Solar Cells
title_short Diffusion Length Mapping for Dye-Sensitized Solar Cells
title_sort diffusion length mapping for dye sensitized solar cells
topic mapping
light-beam-induced current (LBIC)
diffusion length
dye-sensitized solar cells (DSCs)
spectrally-resolved analysis by transmittance and efficiency mapping (SATEM)
url http://www.mdpi.com/1996-1073/9/9/686
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AT babaktaheri diffusionlengthmappingfordyesensitizedsolarcells
AT andreareale diffusionlengthmappingfordyesensitizedsolarcells
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