Crossref
journal-article
Wiley
Advanced Materials (311)
References
40
Referenced
18
10.1038/16393
10.1038/376498a0
10.1038/nmat959
10.1063/1.1456550
10.1063/1.1537049
10.1088/0953-8984/17/8/010
10.1016/j.orgel.2005.02.002
10.1088/0953-8984/14/47/301
- S. Walheim M. Bôltau U. Steiner inPolymer Surfaces and Interfaces 3rd ed. (Eds: R. W. Richards S. K. Peace) Wiley New York1999.
10.1016/S0378-4371(96)00471-2
10.1016/S0379-6779(01)00423-4
10.1002/(SICI)1521-4095(200004)12:7<498::AID-ADMA498>3.0.CO;2-H
10.1002/1521-4095(200008)12:15<1110::AID-ADMA1110>3.0.CO;2-T
10.1063/1.1537049
10.1021/ma049625y
10.1063/1.1383799
10.1063/1.1467981
10.1016/S0379-6779(00)00566-X
10.1021/ma050787j
10.1021/la981467e
10.1023/A:1022182930454
10.1016/S0032-3861(00)00057-4
10.1016/S0032-3861(03)00490-7
10.1103/PhysRevB.67.195333
10.1063/1.122205
{'key': 'e_1_2_1_27_2', 'first-page': '141', 'volume': '5214', 'author': 'Kreouzis T.', 'year': '2004', 'journal-title': 'Proc. SPIE—Int. Soc. Opt. Eng.'}
/ Proc. SPIE—Int. Soc. Opt. Eng. by Kreouzis T. (2004)10.1063/1.1383799
10.1063/1.1467981
10.1046/j.1365-2818.2003.01110.x
10.1046/j.1365-2818.2001.00871.x
10.1021/nl051525y
10.1063/1.366901
10.1021/nl048590c
10.1016/j.polymer.2005.05.056
10.1038/nmat1476
10.1021/ma951739
10.1063/1.1532531
- The fluorescence quantum efficiency (Φ) is defined as Φ = τobs/τrad where τobsis the observed fluorescence decay lifetime and τradis the natural radiative decay lifetime. If we neglect possible electronic interactions between polymer molecules and thus assume that the intrinsic radiative lifetime of the molecule is unchanged by dilution (i.e. changes only occur to the nonradiative decay rate) then changes in the observed decay lifetime are directly proportional to changes in the fluorescence quantum efficiency. We find that the fluorescence decay lifetime of a pure film of F8BT is 1.1 ns which increases by ca. 60 % to 1.8 ns when it is diluted into a PMMA thin film (at a concentration of 2 % by mass). The decay lifetime of F8 is ca. 320 ps in a pure thin film which increases by around 6 % to 340 ps when diluted (also at 2 % by mass) into PMMA. This suggests that the fluorescence quantum efficiency of F8BT increases strongly when diluted into PMMA however the F8 quantum efficiency is much less sensitive to PMMA dilution.
10.1063/1.1407863
10.1021/ma035750i
Dates
Type | When |
---|---|
Created | 18 years, 11 months ago (Sept. 20, 2006, 6:32 a.m.) |
Deposited | 1 year, 9 months ago (Nov. 20, 2023, 5:02 p.m.) |
Indexed | 1 year, 9 months ago (Nov. 20, 2023, 5:42 p.m.) |
Issued | 18 years, 11 months ago (Sept. 20, 2006) |
Published | 18 years, 11 months ago (Sept. 20, 2006) |
Published Online | 18 years, 11 months ago (Sept. 20, 2006) |
Published Print | 18 years, 10 months ago (Oct. 17, 2006) |
@article{Cadby_2006, title={Suppression of Energy‐Transfer Between Conjugated Polymers in a Ternary Blend Identified Using Scanning Near‐Field Optical Microscopy}, volume={18}, ISSN={1521-4095}, url={http://dx.doi.org/10.1002/adma.200600114}, DOI={10.1002/adma.200600114}, number={20}, journal={Advanced Materials}, publisher={Wiley}, author={Cadby, A. and Dean, R. and Jones, R. A. L. and Lidzey, D. G.}, year={2006}, month=sep, pages={2713–2719} }