Cargando…
Dielectric Function of Undoped and Doped Poly[2-methoxy-5-(3′,7′-dimethyloctyloxy)-1,4-phenylene-vinylene] by Ellipsometry in a Wide Spectral Range
[Image: see text] Ellipsometric measurements in a wide spectral range (from 0.05 to 6.5 eV) have been carried out on the organic semiconducting polymer, poly[2-methoxy-5-(3′,7′-dimethyloctyloxy)-1,4-phenylene-vinylene] (MDMO-PPV), in both undoped and doped states. The real and imaginary parts of the...
Autores principales: | , , , , , , , |
---|---|
Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Chemical
Society
2013
|
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3809355/ https://www.ncbi.nlm.nih.gov/pubmed/24175008 http://dx.doi.org/10.1021/jp4061957 |
_version_ | 1782288689961893888 |
---|---|
author | Gasiorowski, Jacek Hingerl, Kurt Menon, Reghu Plach, Thomas Neugebauer, Helmut Wiesauer, Karin Yumusak, Cigdem Sariciftci, Niyazi S. |
author_facet | Gasiorowski, Jacek Hingerl, Kurt Menon, Reghu Plach, Thomas Neugebauer, Helmut Wiesauer, Karin Yumusak, Cigdem Sariciftci, Niyazi S. |
author_sort | Gasiorowski, Jacek |
collection | PubMed |
description | [Image: see text] Ellipsometric measurements in a wide spectral range (from 0.05 to 6.5 eV) have been carried out on the organic semiconducting polymer, poly[2-methoxy-5-(3′,7′-dimethyloctyloxy)-1,4-phenylene-vinylene] (MDMO-PPV), in both undoped and doped states. The real and imaginary parts of the dielectric function and the refractive index are determined accurately, provided that the layer thickness is measured independently. After doping, the optical properties show the presence of new peaks, which could be well-resolved by spectroscopic ellipsometry. Also for the doped material, the complex refractive index, with respect to the dielectric function, has been determined. The broadening of the optical transitions is due to the delocalization of polarons at higher doping level. The detailed information about the dielectric function as well as refractive index function obtained by spectroscopic ellipsometry allows not only qualitative but also quantitative description of the optical properties of the undoped/doped polymer. For the direct characterization of the optical properties of MDMO-PPV, ellipsometry turns out to be advantageous compared to conventional reflection and transmission measurements. |
format | Online Article Text |
id | pubmed-3809355 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2013 |
publisher | American Chemical
Society |
record_format | MEDLINE/PubMed |
spelling | pubmed-38093552013-10-28 Dielectric Function of Undoped and Doped Poly[2-methoxy-5-(3′,7′-dimethyloctyloxy)-1,4-phenylene-vinylene] by Ellipsometry in a Wide Spectral Range Gasiorowski, Jacek Hingerl, Kurt Menon, Reghu Plach, Thomas Neugebauer, Helmut Wiesauer, Karin Yumusak, Cigdem Sariciftci, Niyazi S. J Phys Chem C Nanomater Interfaces [Image: see text] Ellipsometric measurements in a wide spectral range (from 0.05 to 6.5 eV) have been carried out on the organic semiconducting polymer, poly[2-methoxy-5-(3′,7′-dimethyloctyloxy)-1,4-phenylene-vinylene] (MDMO-PPV), in both undoped and doped states. The real and imaginary parts of the dielectric function and the refractive index are determined accurately, provided that the layer thickness is measured independently. After doping, the optical properties show the presence of new peaks, which could be well-resolved by spectroscopic ellipsometry. Also for the doped material, the complex refractive index, with respect to the dielectric function, has been determined. The broadening of the optical transitions is due to the delocalization of polarons at higher doping level. The detailed information about the dielectric function as well as refractive index function obtained by spectroscopic ellipsometry allows not only qualitative but also quantitative description of the optical properties of the undoped/doped polymer. For the direct characterization of the optical properties of MDMO-PPV, ellipsometry turns out to be advantageous compared to conventional reflection and transmission measurements. American Chemical Society 2013-09-18 2013-10-24 /pmc/articles/PMC3809355/ /pubmed/24175008 http://dx.doi.org/10.1021/jp4061957 Text en Copyright © 2013 American Chemical Society Terms of Use (http://pubs.acs.org/page/policy/authorchoice_termsofuse.html) |
spellingShingle | Gasiorowski, Jacek Hingerl, Kurt Menon, Reghu Plach, Thomas Neugebauer, Helmut Wiesauer, Karin Yumusak, Cigdem Sariciftci, Niyazi S. Dielectric Function of Undoped and Doped Poly[2-methoxy-5-(3′,7′-dimethyloctyloxy)-1,4-phenylene-vinylene] by Ellipsometry in a Wide Spectral Range |
title | Dielectric
Function of Undoped and Doped Poly[2-methoxy-5-(3′,7′-dimethyloctyloxy)-1,4-phenylene-vinylene]
by Ellipsometry in a Wide Spectral Range |
title_full | Dielectric
Function of Undoped and Doped Poly[2-methoxy-5-(3′,7′-dimethyloctyloxy)-1,4-phenylene-vinylene]
by Ellipsometry in a Wide Spectral Range |
title_fullStr | Dielectric
Function of Undoped and Doped Poly[2-methoxy-5-(3′,7′-dimethyloctyloxy)-1,4-phenylene-vinylene]
by Ellipsometry in a Wide Spectral Range |
title_full_unstemmed | Dielectric
Function of Undoped and Doped Poly[2-methoxy-5-(3′,7′-dimethyloctyloxy)-1,4-phenylene-vinylene]
by Ellipsometry in a Wide Spectral Range |
title_short | Dielectric
Function of Undoped and Doped Poly[2-methoxy-5-(3′,7′-dimethyloctyloxy)-1,4-phenylene-vinylene]
by Ellipsometry in a Wide Spectral Range |
title_sort | dielectric
function of undoped and doped poly[2-methoxy-5-(3′,7′-dimethyloctyloxy)-1,4-phenylene-vinylene]
by ellipsometry in a wide spectral range |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3809355/ https://www.ncbi.nlm.nih.gov/pubmed/24175008 http://dx.doi.org/10.1021/jp4061957 |
work_keys_str_mv | AT gasiorowskijacek dielectricfunctionofundopedanddopedpoly2methoxy537dimethyloctyloxy14phenylenevinylenebyellipsometryinawidespectralrange AT hingerlkurt dielectricfunctionofundopedanddopedpoly2methoxy537dimethyloctyloxy14phenylenevinylenebyellipsometryinawidespectralrange AT menonreghu dielectricfunctionofundopedanddopedpoly2methoxy537dimethyloctyloxy14phenylenevinylenebyellipsometryinawidespectralrange AT plachthomas dielectricfunctionofundopedanddopedpoly2methoxy537dimethyloctyloxy14phenylenevinylenebyellipsometryinawidespectralrange AT neugebauerhelmut dielectricfunctionofundopedanddopedpoly2methoxy537dimethyloctyloxy14phenylenevinylenebyellipsometryinawidespectralrange AT wiesauerkarin dielectricfunctionofundopedanddopedpoly2methoxy537dimethyloctyloxy14phenylenevinylenebyellipsometryinawidespectralrange AT yumusakcigdem dielectricfunctionofundopedanddopedpoly2methoxy537dimethyloctyloxy14phenylenevinylenebyellipsometryinawidespectralrange AT sariciftciniyazis dielectricfunctionofundopedanddopedpoly2methoxy537dimethyloctyloxy14phenylenevinylenebyellipsometryinawidespectralrange |