Solvent Dependent Assembly of a Polyfluorene−Polythiophene “Rod−Rod” Block Copolyelectrolyte: Influence on Photophysical Properties
We report the solvent-driven assembly of a polyelectrolytic polyfluorene−polythiophene diblock copolymer−poly[9,9-bis(2-ethylhexyl)fluorene]-b-poly[3-(6-trimethylammoniumhexyl)thiophene] (PF2/6-b-P3TMAHT)−in tetrahydrofuran (THF), water, their 1:1 mixture and in subsequently prepared thin films, as...
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Veröffentlicht in: | Langmuir 2010-04, Vol.26 (7), p.5056-5066 |
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description | We report the solvent-driven assembly of a polyelectrolytic polyfluorene−polythiophene diblock copolymer−poly[9,9-bis(2-ethylhexyl)fluorene]-b-poly[3-(6-trimethylammoniumhexyl)thiophene] (PF2/6-b-P3TMAHT)−in tetrahydrofuran (THF), water, their 1:1 mixture and in subsequently prepared thin films, as investigated using a combination of scattering, microscopic and photoluminescence techniques. In solution PF2/6-b-P3TMAHT forms large (>100 nm) aggregates which undergo a transition from objects with surface fractal interface (THF) to ones with a significant planar component due to the presence of the 2-dimensionally merged ribbon-like aggregates or fused walls of the observed vesicular aggregates [THF−water (1:1)]. In THF−water and water the blocks are loosely segregated into P3TMAHT and PF2/6 rich domains, with PF2/6 dominating the aggregate interior. Depending on solvent, the spun films contain either aggregates with a crystalline interior (THF) or large 200 nm−2 μm vesicular aggregates embedded in a featureless matrix (THF−water and water). Structural variations are concomitant with distinctive solvatochromic changes in the photophysical properties including a color change from deep red (THF) to pale orange (THF−water and water) in solution, a decrease in fluorescence quantum yield with increasing water content, and a shift from photoluminescence of individual PF2/6 blocks (THF) to efficient PF2/6 → P3TMAHT energy transfer (THF−water and water). |
doi_str_mv | 10.1021/la903520w |
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In THF−water and water the blocks are loosely segregated into P3TMAHT and PF2/6 rich domains, with PF2/6 dominating the aggregate interior. Depending on solvent, the spun films contain either aggregates with a crystalline interior (THF) or large 200 nm−2 μm vesicular aggregates embedded in a featureless matrix (THF−water and water). Structural variations are concomitant with distinctive solvatochromic changes in the photophysical properties including a color change from deep red (THF) to pale orange (THF−water and water) in solution, a decrease in fluorescence quantum yield with increasing water content, and a shift from photoluminescence of individual PF2/6 blocks (THF) to efficient PF2/6 → P3TMAHT energy transfer (THF−water and water).</description><identifier>ISSN: 0743-7463</identifier><identifier>EISSN: 1520-5827</identifier><identifier>DOI: 10.1021/la903520w</identifier><identifier>PMID: 20085283</identifier><identifier>CODEN: LANGD5</identifier><language>eng</language><publisher>Washington, DC: American Chemical Society</publisher><subject>Chemistry ; Colloidal state and disperse state ; Exact sciences and technology ; General and physical chemistry ; Materials: Nano-and Mesostructured Materials, Polymers, Gels, Liquid Crystals, Composites ; Surface physical chemistry</subject><ispartof>Langmuir, 2010-04, Vol.26 (7), p.5056-5066</ispartof><rights>Copyright © 2010 American Chemical Society</rights><rights>2015 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-a344t-bad18f83fb56bc4bb72dc3663deeb075ca9f96e9747e504fedcd351ab9f709793</citedby><cites>FETCH-LOGICAL-a344t-bad18f83fb56bc4bb72dc3663deeb075ca9f96e9747e504fedcd351ab9f709793</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://pubs.acs.org/doi/pdf/10.1021/la903520w$$EPDF$$P50$$Gacs$$H</linktopdf><linktohtml>$$Uhttps://pubs.acs.org/doi/10.1021/la903520w$$EHTML$$P50$$Gacs$$H</linktohtml><link.rule.ids>314,776,780,2752,27053,27901,27902,56713,56763</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=22581923$$DView record in Pascal Francis$$Hfree_for_read</backlink><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/20085283$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Knaapila, M</creatorcontrib><creatorcontrib>Evans, R. 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In solution PF2/6-b-P3TMAHT forms large (>100 nm) aggregates which undergo a transition from objects with surface fractal interface (THF) to ones with a significant planar component due to the presence of the 2-dimensionally merged ribbon-like aggregates or fused walls of the observed vesicular aggregates [THF−water (1:1)]. In THF−water and water the blocks are loosely segregated into P3TMAHT and PF2/6 rich domains, with PF2/6 dominating the aggregate interior. Depending on solvent, the spun films contain either aggregates with a crystalline interior (THF) or large 200 nm−2 μm vesicular aggregates embedded in a featureless matrix (THF−water and water). Structural variations are concomitant with distinctive solvatochromic changes in the photophysical properties including a color change from deep red (THF) to pale orange (THF−water and water) in solution, a decrease in fluorescence quantum yield with increasing water content, and a shift from photoluminescence of individual PF2/6 blocks (THF) to efficient PF2/6 → P3TMAHT energy transfer (THF−water and water).</description><subject>Chemistry</subject><subject>Colloidal state and disperse state</subject><subject>Exact sciences and technology</subject><subject>General and physical chemistry</subject><subject>Materials: Nano-and Mesostructured Materials, Polymers, Gels, Liquid Crystals, Composites</subject><subject>Surface physical chemistry</subject><issn>0743-7463</issn><issn>1520-5827</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2010</creationdate><recordtype>article</recordtype><recordid>eNpt0EFvFCEYBmBiNHatPfgHDBdjPIwyMAyDt7pWbdLEjdrzBJiP7FQWRpjR7K3HJr31rH-uv0QmXdsevAAfefISXoSeleR1SWj5xilJGKfk1wO0KPNe8IaKh2hBRMUKUdVsDz1J6YwQIlklH6M9SkjDacMW6PJrcD_Bj_g9DOC7-XSYEmy02-JgscKr4LbWTSGCh-uLq3kc130Y1nnG1-e_v4QuX8_r-R_8zgXzHS_DkBU4MGOcObzFxz5ngDeAg8erdRhzwDb1Rjm8imGAOPaQnqJHVrkEB7t9H51-OPq2_FScfP54vDw8KRSrqrHQqisb2zCrea1NpbWgnWF1zToATQQ3SlpZgxSVAE4qC53pGC-VllYQKSTbRy9vcocYfkyQxnbTJwPOKQ9hSq1gjErZNDzLVzfSxJBSBNsOsd-ouG1L0s7Vt7fVZ_t8lzrpDXS38l_XGbzYAZXyx21U3vTpzlHelJLec8qk9ixM0ecy_vPgX3g9n0Y</recordid><startdate>20100406</startdate><enddate>20100406</enddate><creator>Knaapila, M</creator><creator>Evans, R. 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In solution PF2/6-b-P3TMAHT forms large (>100 nm) aggregates which undergo a transition from objects with surface fractal interface (THF) to ones with a significant planar component due to the presence of the 2-dimensionally merged ribbon-like aggregates or fused walls of the observed vesicular aggregates [THF−water (1:1)]. In THF−water and water the blocks are loosely segregated into P3TMAHT and PF2/6 rich domains, with PF2/6 dominating the aggregate interior. Depending on solvent, the spun films contain either aggregates with a crystalline interior (THF) or large 200 nm−2 μm vesicular aggregates embedded in a featureless matrix (THF−water and water). Structural variations are concomitant with distinctive solvatochromic changes in the photophysical properties including a color change from deep red (THF) to pale orange (THF−water and water) in solution, a decrease in fluorescence quantum yield with increasing water content, and a shift from photoluminescence of individual PF2/6 blocks (THF) to efficient PF2/6 → P3TMAHT energy transfer (THF−water and water).</abstract><cop>Washington, DC</cop><pub>American Chemical Society</pub><pmid>20085283</pmid><doi>10.1021/la903520w</doi><tpages>11</tpages></addata></record> |
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title | Solvent Dependent Assembly of a Polyfluorene−Polythiophene “Rod−Rod” Block Copolyelectrolyte: Influence on Photophysical Properties |
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