Supporting Information A facile route to fabricate anodic TiO2

advertisement

Electronic Supplementary Material (ESI) for Nanoscale

This journal is © The Royal Society of Chemistry 2012

Supporting Information

A facile route to fabricate anodic TiO

2

nanotube/nanoparticle hybrid structure for high efficiency dye-sensitized solar cells

By Jia Lin, a,b

Xiaolin Liu, a

Min Guo, b

Wei Lu, a

Guoge Zhang, b,c

Limin Zhou, d

Xianfeng Chen

*a and Haitao Huang

*b a

Department of Physics, The State Key Laboratory on Fiber Optic Local Area Communication Networks and Advanced Optical Communication Systems, Shanghai Jiao Tong University, Shanghai 200240, China.

E-mail: xfchen@sjtu.edu.cn b

Department of Applied Physics and Materials Research Center, The Hong Kong Polytechnic University,

Hung Hom, Kowloon, Hong Kong. E-mail: aphhuang@polyu.edu.hk c

School of Materials Science and Engineering, South China University of Technology, Guangzhou, China. d

Department of Mechanical Engineering, The Hong Kong Polytechnic University, Hung Hom, Kowloon,

Hong Kong.

Electronic Supplementary Material (ESI) for Nanoscale

This journal is © The Royal Society of Chemistry 2012

Fig. S1.

SEM images of TNAs with a prolonged immersion in water (5 days): (a) top view; (b) cross-sectional view.

Electronic Supplementary Material (ESI) for Nanoscale

This journal is © The Royal Society of Chemistry 2012

Fig. S2.

XRD patterns of water-treated TNAs with a hybrid structure after annealing at

400 °C for 2 h.

Electronic Supplementary Material (ESI) for Nanoscale

This journal is © The Royal Society of Chemistry 2012

Fig. S3.

The equivalent circuit model used to fit the Nyquist curves.

R s

: series resistance. R

CO

/ C

CO

, R

TCO

/ C

TCO

, and R

CE

/ C

CE

are the resistance/capacitance at the FTO/TiO

2

, FTO/electrolyte and Pt electrode/electrolyte interfaces, respectively. W is the impedance of I

/I

3

diffusion in the electrolyte. R ct

: charge transfer resistance. C  : chemical capacitance. R t

: transport resistance.

The charge transport time was calculated by the relation

 c

= d

2

/2.35

D n

= R t

C  /2.35, where d and D n

are the film thickness and the effective diffusion constant, respectively

[1, 2]

, and

the charge collection efficiency by

 cc

=1−

 c

/

 r

[3]

.

1. J. van de Lagemaat and A. Frank, J. Phys. Chem. B , 2001, 105 , 11194-11205.

2. F. Fabregat-Santiago, J. Bisquert, G. Garcia-Belmonte, G. Boschloo and A. Hagfeldt, Sol.

Energy Mater. Sol. Cells , 2005, 87 , 117–131.

3. G. Schlichthörl, N. Park and A. Frank, J. Phys. Chem. B , 1999, 103 , 782–791.

Download