Holes photogeneration in phthalocyanine-doped polysilane
Abstract Polysilane polymers are attractive photoconductive materials, due to the high mobility of the charge carriers (holes). The photoconductivity in the visible region is greatly enhanced by the addition of a phthalocyanine, because the dopant increases the absorption of light and the quantum yi...
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| Autor*in: |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
1991 |
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| Umfang: |
10 |
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| Reproduktion: |
Springer Online Journal Archives 1860-2002 |
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| Übergeordnetes Werk: |
in: Molecular engineering - 1991, 1(1991) vom: März, Seite 221-230 |
| Übergeordnetes Werk: |
volume:1 ; year:1991 ; month:03 ; pages:221-230 ; extent:10 |
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NLEJ195190866 |
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| 520 | |a Abstract Polysilane polymers are attractive photoconductive materials, due to the high mobility of the charge carriers (holes). The photoconductivity in the visible region is greatly enhanced by the addition of a phthalocyanine, because the dopant increases the absorption of light and the quantum yield of the holes photogeneration. The quantum yield has been measured by the technique of xerographic discharge at several values of the polarisation field. From these data the intrinsic quantum yield Φ0 and the thermalisation distance r 0 were calculated. r 0 is similar to the value measured in the trinitrofluorenone doped polyvinylcarbazole system (27.5 Å) while Φ0 is much lower (2.8·10−2 compared to 0.11). In fact, r 0 is assumed to be mainly dependent on the polymeric environment, while Φ0 depends on the nature of the coupling between the dopant and the polymer. | ||
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| 700 | 1 | |a Moisan, J. Y. |4 oth | |
| 700 | 1 | |a Dubois, J. C. |4 oth | |
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(DE-627)NLEJ195190866 DE-627 ger DE-627 rakwb eng Holes photogeneration in phthalocyanine-doped polysilane 1991 10 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Abstract Polysilane polymers are attractive photoconductive materials, due to the high mobility of the charge carriers (holes). The photoconductivity in the visible region is greatly enhanced by the addition of a phthalocyanine, because the dopant increases the absorption of light and the quantum yield of the holes photogeneration. The quantum yield has been measured by the technique of xerographic discharge at several values of the polarisation field. From these data the intrinsic quantum yield Φ0 and the thermalisation distance r 0 were calculated. r 0 is similar to the value measured in the trinitrofluorenone doped polyvinylcarbazole system (27.5 Å) while Φ0 is much lower (2.8·10−2 compared to 0.11). In fact, r 0 is assumed to be mainly dependent on the polymeric environment, while Φ0 depends on the nature of the coupling between the dopant and the polymer. Springer Online Journal Archives 1860-2002 Lagarde, M. oth Moisan, J. Y. oth Dubois, J. C. oth in Molecular engineering 1991 1(1991) vom: März, Seite 221-230 (DE-627)NLEJ188990151 (DE-600)2003655-3 1572-8951 nnns volume:1 year:1991 month:03 pages:221-230 extent:10 http://dx.doi.org/10.1007/BF00161665 GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 1 1991 3 221-230 10 |
| spelling |
(DE-627)NLEJ195190866 DE-627 ger DE-627 rakwb eng Holes photogeneration in phthalocyanine-doped polysilane 1991 10 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Abstract Polysilane polymers are attractive photoconductive materials, due to the high mobility of the charge carriers (holes). The photoconductivity in the visible region is greatly enhanced by the addition of a phthalocyanine, because the dopant increases the absorption of light and the quantum yield of the holes photogeneration. The quantum yield has been measured by the technique of xerographic discharge at several values of the polarisation field. From these data the intrinsic quantum yield Φ0 and the thermalisation distance r 0 were calculated. r 0 is similar to the value measured in the trinitrofluorenone doped polyvinylcarbazole system (27.5 Å) while Φ0 is much lower (2.8·10−2 compared to 0.11). In fact, r 0 is assumed to be mainly dependent on the polymeric environment, while Φ0 depends on the nature of the coupling between the dopant and the polymer. Springer Online Journal Archives 1860-2002 Lagarde, M. oth Moisan, J. Y. oth Dubois, J. C. oth in Molecular engineering 1991 1(1991) vom: März, Seite 221-230 (DE-627)NLEJ188990151 (DE-600)2003655-3 1572-8951 nnns volume:1 year:1991 month:03 pages:221-230 extent:10 http://dx.doi.org/10.1007/BF00161665 GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 1 1991 3 221-230 10 |
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(DE-627)NLEJ195190866 DE-627 ger DE-627 rakwb eng Holes photogeneration in phthalocyanine-doped polysilane 1991 10 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Abstract Polysilane polymers are attractive photoconductive materials, due to the high mobility of the charge carriers (holes). The photoconductivity in the visible region is greatly enhanced by the addition of a phthalocyanine, because the dopant increases the absorption of light and the quantum yield of the holes photogeneration. The quantum yield has been measured by the technique of xerographic discharge at several values of the polarisation field. From these data the intrinsic quantum yield Φ0 and the thermalisation distance r 0 were calculated. r 0 is similar to the value measured in the trinitrofluorenone doped polyvinylcarbazole system (27.5 Å) while Φ0 is much lower (2.8·10−2 compared to 0.11). In fact, r 0 is assumed to be mainly dependent on the polymeric environment, while Φ0 depends on the nature of the coupling between the dopant and the polymer. Springer Online Journal Archives 1860-2002 Lagarde, M. oth Moisan, J. Y. oth Dubois, J. C. oth in Molecular engineering 1991 1(1991) vom: März, Seite 221-230 (DE-627)NLEJ188990151 (DE-600)2003655-3 1572-8951 nnns volume:1 year:1991 month:03 pages:221-230 extent:10 http://dx.doi.org/10.1007/BF00161665 GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 1 1991 3 221-230 10 |
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(DE-627)NLEJ195190866 DE-627 ger DE-627 rakwb eng Holes photogeneration in phthalocyanine-doped polysilane 1991 10 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Abstract Polysilane polymers are attractive photoconductive materials, due to the high mobility of the charge carriers (holes). The photoconductivity in the visible region is greatly enhanced by the addition of a phthalocyanine, because the dopant increases the absorption of light and the quantum yield of the holes photogeneration. The quantum yield has been measured by the technique of xerographic discharge at several values of the polarisation field. From these data the intrinsic quantum yield Φ0 and the thermalisation distance r 0 were calculated. r 0 is similar to the value measured in the trinitrofluorenone doped polyvinylcarbazole system (27.5 Å) while Φ0 is much lower (2.8·10−2 compared to 0.11). In fact, r 0 is assumed to be mainly dependent on the polymeric environment, while Φ0 depends on the nature of the coupling between the dopant and the polymer. Springer Online Journal Archives 1860-2002 Lagarde, M. oth Moisan, J. Y. oth Dubois, J. C. oth in Molecular engineering 1991 1(1991) vom: März, Seite 221-230 (DE-627)NLEJ188990151 (DE-600)2003655-3 1572-8951 nnns volume:1 year:1991 month:03 pages:221-230 extent:10 http://dx.doi.org/10.1007/BF00161665 GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 1 1991 3 221-230 10 |
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(DE-627)NLEJ195190866 DE-627 ger DE-627 rakwb eng Holes photogeneration in phthalocyanine-doped polysilane 1991 10 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Abstract Polysilane polymers are attractive photoconductive materials, due to the high mobility of the charge carriers (holes). The photoconductivity in the visible region is greatly enhanced by the addition of a phthalocyanine, because the dopant increases the absorption of light and the quantum yield of the holes photogeneration. The quantum yield has been measured by the technique of xerographic discharge at several values of the polarisation field. From these data the intrinsic quantum yield Φ0 and the thermalisation distance r 0 were calculated. r 0 is similar to the value measured in the trinitrofluorenone doped polyvinylcarbazole system (27.5 Å) while Φ0 is much lower (2.8·10−2 compared to 0.11). In fact, r 0 is assumed to be mainly dependent on the polymeric environment, while Φ0 depends on the nature of the coupling between the dopant and the polymer. Springer Online Journal Archives 1860-2002 Lagarde, M. oth Moisan, J. Y. oth Dubois, J. C. oth in Molecular engineering 1991 1(1991) vom: März, Seite 221-230 (DE-627)NLEJ188990151 (DE-600)2003655-3 1572-8951 nnns volume:1 year:1991 month:03 pages:221-230 extent:10 http://dx.doi.org/10.1007/BF00161665 GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 1 1991 3 221-230 10 |
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Holes photogeneration in phthalocyanine-doped polysilane |
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Abstract Polysilane polymers are attractive photoconductive materials, due to the high mobility of the charge carriers (holes). The photoconductivity in the visible region is greatly enhanced by the addition of a phthalocyanine, because the dopant increases the absorption of light and the quantum yield of the holes photogeneration. The quantum yield has been measured by the technique of xerographic discharge at several values of the polarisation field. From these data the intrinsic quantum yield Φ0 and the thermalisation distance r 0 were calculated. r 0 is similar to the value measured in the trinitrofluorenone doped polyvinylcarbazole system (27.5 Å) while Φ0 is much lower (2.8·10−2 compared to 0.11). In fact, r 0 is assumed to be mainly dependent on the polymeric environment, while Φ0 depends on the nature of the coupling between the dopant and the polymer. |
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Abstract Polysilane polymers are attractive photoconductive materials, due to the high mobility of the charge carriers (holes). The photoconductivity in the visible region is greatly enhanced by the addition of a phthalocyanine, because the dopant increases the absorption of light and the quantum yield of the holes photogeneration. The quantum yield has been measured by the technique of xerographic discharge at several values of the polarisation field. From these data the intrinsic quantum yield Φ0 and the thermalisation distance r 0 were calculated. r 0 is similar to the value measured in the trinitrofluorenone doped polyvinylcarbazole system (27.5 Å) while Φ0 is much lower (2.8·10−2 compared to 0.11). In fact, r 0 is assumed to be mainly dependent on the polymeric environment, while Φ0 depends on the nature of the coupling between the dopant and the polymer. |
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Abstract Polysilane polymers are attractive photoconductive materials, due to the high mobility of the charge carriers (holes). The photoconductivity in the visible region is greatly enhanced by the addition of a phthalocyanine, because the dopant increases the absorption of light and the quantum yield of the holes photogeneration. The quantum yield has been measured by the technique of xerographic discharge at several values of the polarisation field. From these data the intrinsic quantum yield Φ0 and the thermalisation distance r 0 were calculated. r 0 is similar to the value measured in the trinitrofluorenone doped polyvinylcarbazole system (27.5 Å) while Φ0 is much lower (2.8·10−2 compared to 0.11). In fact, r 0 is assumed to be mainly dependent on the polymeric environment, while Φ0 depends on the nature of the coupling between the dopant and the polymer. |
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