A New Type of Electrolyte with a Light‐Trapping Scheme for High‐Efficiency Quasi‐Solid‐State Dye‐Sensitized Solar Cells

Dye-sensitized solar cells (DSSCs) are attracting both academic and industrial interest owing to their high-effi ciency and potential low-cost. [ 1 ] The electrolyte, containing the I − /I 3 − redox couple, is the one of the most-important components of a DSSC, and directly infl uences their performance and stability. [ 2,3 ] Generally, the role of the electrolyte in a DSSC is to fi nish the charge cycle, including the transport of the I − /I 3 − redox couple, [ 4 ] the regeneration of oxidized dye at the dyed TiO 2 /electrolyte interface and the reduction of I 3 − at the counter electrode. [ 5 ] However, I 3 − in the electrolyte will absorb visible light, [ 6 ] which results in energy loss. Furthermore, due to the inhomogeneous dye distribution, [ 7 ] a certain part of the incident light transmits through the photoanode, which decreases the light-harvesting effi ciency. As we know, although relatively large particles have already been used in DSSCs to help increase the light-harvesting effi ciency, still part of the incident light will transmit through the photoanode. Moreover. an excess of large particles will not only lower the light-harvesting effi ciency over the whole range of visible wavelengths owing to enhanced light refl ection at the conducting glass/TiO 2 interface, but also decrease the electron-transfer yield. [ 8 ] As reported previously, [ 9 ] light trapping has become a standard technique to increase the light absorption of incident light in the active layers of hydrogenated amorphous-siliconbased solar cells, based on the use of textured substrates and highly refl ective back contacts. This triggered our interest in exploring a new type of electrolyte with a light-trapping scheme to enhance the light-harvesting effi ciency of DSSCs. Liquid crystals (LCs), as the fourth state of matter, combining properties of liquids and solids, [ 10 ] are usually used as the medium for organic catalytic synthesis, [ 11 ] functional nanostructured materials, [ 12 ] and especially in the fi eld of polymer-dispersed liquidcrystal (PDLC) displays, due to the light-scattering properties of the LC. [ 13 ] Thus, we tried to introduce an LC to the liquid electrolyte of a DSSC. Furthermore, when the LC was added to the liquid electrolyte, a quasi-solid-state electrolyte was formed, which could help to resolve the sealing diffi culty in the DSSCs.

[1]  Y. Kang,et al.  Liquid Crystals Embedded in Polymeric Electrolytes for Quasi-Solid State Dye-Sensitized Solar Cell Applications , 2009 .

[2]  Alex B. F. Martinson,et al.  Advancing beyond current generation dye-sensitized solar cells , 2008 .

[3]  E. Stathatos,et al.  Increase of the Efficiency of Quasi‐Solid State Dye‐Sensitized Solar Cells by a Synergy between Titania Nanocrystallites of Two Distinct Nanoparticle Sizes , 2007 .

[4]  A. Hinsch,et al.  Quasi-solid state polymer electrolytes for dye-sensitized solar cells: Effect of the electrolyte components variation on the triiodide ion diffusion properties and charge-transfer resistance at platinum electrode , 2006 .

[5]  Liyuan Han,et al.  Improvement of efficiency of dye-sensitized solar cells based on analysis of equivalent circuit , 2006 .

[6]  K. Binnemans Ionic liquid crystals. , 2005, Chemical reviews.

[7]  Michael Grätzel,et al.  Influence of 4-guanidinobutyric acid as coadsorbent in reducing recombination in dye-sensitized solar cells. , 2005, The journal of physical chemistry. B.

[8]  M. Watanabe,et al.  Anomaly of charge transport of an iodide/tri-iodide redox couple in an ionic liquid and its importance in dye-sensitized solar cells. , 2005, Chemical communications.

[9]  O. Yaroshchuk,et al.  Ordering of droplets and light scattering in polymer dispersed liquid crystal films , 2004, cond-mat/0406005.

[10]  Hironori Arakawa,et al.  Efficiencies of Electron Injection from Excited N3 Dye into Nanocrystalline Semiconductor (ZrO2, TiO2, ZnO, Nb2O5, SnO2, In2O3) Films , 2004 .

[11]  Markus Antonietti,et al.  Ionic Self‐Assembly: Facile Synthesis of Supramolecular Materials , 2003 .

[12]  Hironori Arakawa,et al.  Quantitative Analysis of Light-Harvesting Efficiency and Electron-Transfer Yield in Ruthenium-Dye-Sensitized Nanocrystalline TiO2 Solar Cells , 2002 .

[13]  Andreas Georg,et al.  Diffusion in the electrolyte and charge-transfer reaction at the platinum electrode in dye-sensitized solar cells , 2001 .

[14]  M. Zeman,et al.  Optical modeling of a-Si:H solar cells with rough interfaces: Effect of back contact and interface roughness , 2000 .

[15]  E. A. Ponomarev,et al.  Detection of inhomogeneous dye distribution in dye sensitised nanocrystalline solar cells by intensity modulated photocurrent spectroscopy (IMPS) , 1999 .

[16]  L. Peter,et al.  Frequency-Resolved Optical Detection of Photoinjected Electrons in Dye-Sensitized Nanocrystalline Photovoltaic Cells , 1999 .

[17]  R. Schropp,et al.  Charge Dynamics following Dye Photoinjection into a TiO2 Nanocrystalline Network , 1998 .

[18]  Mohammad Khaja Nazeeruddin,et al.  Conversion of light to electricity by cis-X2bis(2,2'-bipyridyl-4,4'-dicarboxylate)ruthenium(II) charge-transfer sensitizers (X = Cl-, Br-, I-, CN-, and SCN-) on nanocrystalline titanium dioxide electrodes , 1993 .

[19]  M. Grätzel,et al.  A low-cost, high-efficiency solar cell based on dye-sensitized colloidal TiO2 films , 1991, Nature.

[20]  P. Kubelka,et al.  New Contributions to the Optics of Intensely Light-Scattering Materials. Part I , 1948 .

[21]  Juan Bisquert,et al.  Theory of the Impedance of Electron Diffusion and Recombination in a Thin Layer , 2002 .

[22]  R. Weiss Thermotropic liquid crystals as reaction media for mechanistic investigations1 , 1988 .