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Photoluminescence in Conjugated Polymers: Experimental Investigations of Excited State Events
Linköping University, Department of Physics, Measurement Technology, Biology and Chemistry. Linköping University, The Institute of Technology.
2000 (English)Doctoral thesis, comprehensive summary (Other academic)
Abstract [en]

After an extensive scientific effort spent on the understanding of conjugated polymers and molecules, these material are on the border of commercialisation. Even though highly efficient devices can be made with conjugated polymers the underlying physics is far from being fully understood. In this thesis, photoluminescence is used for studying excited state events inconjugated polymers. The work is relevant for a number of applications, such as photodiodes, lasers and light emitting devices.

A close co-operation with chemists which have synthesised a number of phenyl substituted polythiophenes has made it possible to find correlation's between the chemical structure and the resulting photoluminescence of these polythiophenes. The yield of photoluminescence is set by intrachain properties influencing the geometry of the single chain and interchain properties. By comparing the photoluminescence of the polymers in solution and thin film one can assign the intrachain properties, which are dominant in solution and the interchain properties which act in the thin film. We have found that polymers with planar backbones give the most luminescent polymers in solution. Using interchain interaction to increase the planarity has been shown to increase the PL yield even further. In thin films the interchain interaction between different chains can give both intrachain emitting species, and an increase of exciton transport, which increase the possibility of finding PL quenching sites in the polymer film, thus reducing the PL yield in the thin film.

With a strong electron acceptor, the exciton on the polymer chain can split into its constituents, forming an electron and a hole. A quenching of the photoluminescence occurs. This has been used to determine the exciton quenching range in a polythiophene, close to a strong donor-acceptor interface. A short distance was found (5 nm) which is strongly limiting the efficiency of photovoltaic devices.

Place, publisher, year, edition, pages
Linköping: Linköping University , 2000. , p. 54
Series
Linköping Studies in Science and Technology. Dissertations, ISSN 0345-7524 ; 649
National Category
Polymer Chemistry Condensed Matter Physics
Identifiers
URN: urn:nbn:se:liu:diva-185682Libris ID: 7624624ISBN: 9172198265 (print)OAI: oai:DiVA.org:liu-185682DiVA, id: diva2:1666191
Public defence
2000-09-25, Planck, Fysikhuset, Linköpings universitet, Linköping, 10:15
Note

All or some of the partial works included in the dissertation are not registered in DIVA and therefore not linked in this post.

Available from: 2022-06-08 Created: 2022-06-08 Last updated: 2022-06-08Bibliographically approved
List of papers
1. High luminescence from a substituted polythiophene in a solvent with low solubility
Open this publication in new window or tab >>High luminescence from a substituted polythiophene in a solvent with low solubility
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2001 (English)In: Chemical Physics Letters, ISSN 0009-2614, E-ISSN 1873-4448, Vol. 337, no 4-6, p. 277-283Article in journal (Refereed) Published
Abstract [en]

Steady-state and time-resolved photoluminescence (PL) is used to probe different states of order in highly regular poly(3-(2'-methoxy-5'-octylphenyl)thiophene) (POMeOPT). In a good solvent (chloroform) the polymer has a PL yield of 0.33 and in a solvent with low solubility (mixture of chloroform and toluene) a new phase appears with higher PL yield (0.50). The new phase is attributed to micro-crystals formed by the regular part of the polymer which have low solubility in toluene. The crystallites have highly structured and redshifted electronic transitions compared with chains which are dissolved.

National Category
Engineering and Technology
Identifiers
urn:nbn:se:liu:diva-47418 (URN)10.1016/S0009-2614(01)00208-1 (DOI)
Available from: 2009-10-11 Created: 2009-10-11 Last updated: 2022-06-08
2. Photoluminescence quenching at a polythiophene/C-60 heterojunction
Open this publication in new window or tab >>Photoluminescence quenching at a polythiophene/C-60 heterojunction
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2000 (English)In: Physical Review B. Condensed Matter and Materials Physics, ISSN 1098-0121, E-ISSN 1550-235X, Vol. 61, no 19, p. 12957-12963Article in journal (Refereed) Published
Abstract [en]

Quenching of photoluminescence in a substituted polythiophene in the presence of a deposited C-60 layer is studied by steady-state and time-resolved photoluminescence (PL). The steady-state PL is evaluated by con -sidering the interference of the absorbed and emitted electro-optical field in the thin film coupled to exciton diffusion in the conjugated polymer. PL quenching occurs for excitons generated within 5 nm from the heterojunction. A blueshift of the polymer emission spectrum is observed when C-60 is deposited on top of a polymer thin film. The blueshift is shown to be caused by PL quenching before the excitation is transferred to the lowest-energy sites.

National Category
Engineering and Technology
Identifiers
urn:nbn:se:liu:diva-49741 (URN)10.1103/PhysRevB.61.12957 (DOI)
Available from: 2009-10-11 Created: 2009-10-11 Last updated: 2022-06-08
3. A polythiophene microcavity laser
Open this publication in new window or tab >>A polythiophene microcavity laser
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1998 (English)In: Chemical Physics Letters, ISSN 0009-2614, E-ISSN 1873-4448, Vol. 288, no 5-6, p. 879-884Article in journal (Refereed) Published
Abstract [en]

We report photopumped lasing in a microcavity device with a polythiophene layer as the emitter. These microcavity devices are built by joining two polymer coated dielectric mirrors at elevated temperature. When photopumping the film, a lasing threshold is observed at 120 nJ/cm(2). Comparative studies with fast pump-probe spectroscopy of thin polythiophene films and the same polymer in photopumped lasing studies, indicate that the gain coefficient is 80 +/- 20 cm(-1), and that the exciton concentration is 2 X 10(17) cm(-3) at the lasing transition, well below the exciton-exciton recombination level. (C) 1998 Elsevier Science B.V. All rights reserved.

Place, publisher, year, edition, pages
Elsevier, 1998
National Category
Engineering and Technology
Identifiers
urn:nbn:se:liu:diva-74870 (URN)10.1016/S0009-2614(98)00320-0 (DOI)000074285700043 ()
Available from: 2012-02-10 Created: 2012-02-10 Last updated: 2022-06-15
4. Lasing in a microcavity with an oriented liquid-crystalline polyfluorene copolymer as active layer
Open this publication in new window or tab >>Lasing in a microcavity with an oriented liquid-crystalline polyfluorene copolymer as active layer
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2001 (English)In: Advanced Materials, ISSN 0935-9648, E-ISSN 1521-4095, Vol. 13, no 5, p. 323-327Article in journal (Refereed) Published
National Category
Engineering and Technology
Identifiers
urn:nbn:se:liu:diva-49330 (URN)
Available from: 2009-10-11 Created: 2009-10-11 Last updated: 2022-06-15

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