Interface Engineering for Solid‐State Dye‐Sensitized Nanocrystalline Solar Cells: The Use of Ion‐Solvating Hole‐Transporting Polymers
Source abstract
Abstract
Abstract The control of interfacial charge transfer is central to the design of photovoltaic devices. This charge transfer is strongly dependent upon the local chemical environment at each interface. In this paper we report a methodology for the fabrication of a novel nanostructured multicomponent film, employing a dual‐function supramolecular organic semiconductor to allow molecular‐level control of the local chemical composition at a nanostructured inorganic/organic semiconductor heterojunction. The multicomponent film comprises a lithium ion doped dual‐functional hole‐transporting material (Li+–DFHTM), sandwiched between a dye‐sensitized nanocrystalline TiO2 film and a mono‐functional organic hole‐transporting material (MFHTM). The DFHTM consists of a conjugated organic semiconductor with ion supporting side chains, designed to allow both electronic and ionic charge transport properties. The Li+–DFHTM layers provide a new and versatile way to control the interface electrostatics, and consequently the charge transfer, at a nanostructured dye‐sensitized inorganic/organic semiconductor heterojunction.
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Research context
OpenAlex topics: Conducting polymers and applications · Analytical Chemistry and Sensors · TiO2 Photocatalysis and Solar Cells
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References (32)
Show source-provided references
1. M. D. Archer R. Hill Clean Electricity from Photovoltaics Imperial College Press London2001.10.1142/p139 ↗
2. 10.1038/2693610.1038/26936 ↗
3. 10.1126/science.106915610.1126/science.1069156 ↗
4. 10.1038/nature0121710.1038/nature01217 ↗
5. 10.1038/1639310.1038/16393 ↗
6. 10.1063/1.138380010.1063/1.1383800 ↗
7. 10.1021/ja027945w10.1021/ja027945w ↗
8. 10.1002/(SICI)1521-4095(200003)12:6<447::AID-ADMA447>3.0.CO;2-810.1002/(SICI)1521-4095(200003)12:6<447::AID-ADMA447>3.0.CO;2-8 ↗
9. 10.1126/science.269.5227.108610.1126/science.269.5227.1086 ↗
10. 10.1103/PhysRevB.57.1295110.1103/PhysRevB.57.12951 ↗
11. 10.1063/1.140614810.1063/1.1406148 ↗
12. 10.1021/ma001997t10.1021/ma001997t ↗
13. 10.1016/S0379-6779(98)80041-610.1016/S0379-6779(98)80041-6 ↗
14. 10.1039/b306604e10.1039/b306604e ↗
15. 10.1016/0040-6090(94)90575-410.1016/0040-6090(94)90575-4 ↗
16. 10.1016/0040-6090(94)90617-310.1016/0040-6090(94)90617-3 ↗
17. 10.1126/science.277.5330.123210.1126/science.277.5330.1232 ↗
18. 10.1002/(SICI)1521-4095(199807)10:10<769::AID-ADMA769>3.0.CO;2-310.1002/(SICI)1521-4095(199807)10:10<769::AID-ADMA769>3.0.CO;2-3 ↗
19. 10.1038/3500661010.1038/35006610 ↗
20. 10.1063/1.149039410.1063/1.1490394 ↗
21. 10.1002/cphc.20039001410.1002/cphc.200390014 ↗
22. Films cast from DFHTM doped with lithium triflamide salt displayed no crystallisation of salt consistent with formation of Li+–DFHTM complex. We also note that assembly of this layer resulted in no detectable dye desorption/degradation as confirmed by steady‐state absorption spectroscopy.
23. Steady‐state absorption spectroscopy was employed to determine the extinction coefficient (ε) of the DFHTM at 407 nm. This extinction coefficient was calculated using the Beer–Lambert law.
24. 10.1002/1521-4095(200106)13:11<826::AID-ADMA826>3.0.CO;2-L10.1002/1521-4095(200106)13:11<826::AID-ADMA826>3.0.CO;2-L ↗
25. 10.1016/S0379-6779(00)01495-810.1016/S0379-6779(00)01495-8 ↗
26. Comparison of the transient feature at 520 nm with the absorption feature of the chemically oxidized DFHTM led us to assign the positive band at 520 nm to the cation of the DFHTM. The chemical oxidation of the DFHTM achieved by using N(PhBr)3SbCl6(as in reference [2]).
27. 10.1021/ja991540310.1021/ja9915403 ↗
28. 10.1103/PhysRevB.63.20532110.1103/PhysRevB.63.205321 ↗
29. 10.1021/jp991085x10.1021/jp991085x ↗
30. 10.1016/0013-4686(95)90400-W10.1016/0013-4686(95)90400-W ↗
31. 10.1021/j100109a02910.1021/j100109a029 ↗
32. 10.1021/j100193a06210.1021/j100193a062 ↗