Interference-enhanced Raman scattering of F sub(16)CuPc thin films
Interference-enhanced Raman scattering (IERS) was observed for thin films of copper(II) hexadecafluorophthalocyanine (F sub(16)CuPc) deposited on SiO sub(2) layers on a Si substrate. The enhancement of the Raman scattering originates from the interference of the light in the transparent SiO sub(2) l...
Gespeichert in:
Veröffentlicht in: | Journal of physics. D, Applied physics Applied physics, 2016-03, Vol.49 (11), p.115502-115508 |
---|---|
Hauptverfasser: | , , , , , |
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
Online-Zugang: | Volltext |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
Zusammenfassung: | Interference-enhanced Raman scattering (IERS) was observed for thin films of copper(II) hexadecafluorophthalocyanine (F sub(16)CuPc) deposited on SiO sub(2) layers on a Si substrate. The enhancement of the Raman scattering originates from the interference of the light in the transparent SiO sub(2) layer. Stripes of SiO sub(2)/Si with gradually varying oxide layer thickness were used as IERS substrates for a systematic study of the enhancement parameters. Raman measurements were carried out using three laser lines (325, 514.7, and 632.8 nm) in order to probe the F sub(16)CuPc thin films at non-resonant and resonant Raman conditions. Spectroscopic ellipsometry was used to determine both the SiO sub(2) layer and thin film thicknesses. The intensity enhancement of the F sub(16)CuPc Raman peaks occurs periodically, corresponding to the alternating interference conditions for the Raman scattered light with increasing SiO sub(2) layer thickness. The enhancement factors were calculated using the optical constants of the layers involved and the geometric parameters. This allows a straightforward application of IERS for optical studies of thin films and interfaces by calculating the dielectric thickness where maximum Raman enhancement is expected. |
---|---|
ISSN: | 0022-3727 1361-6463 |
DOI: | 10.1088/0022-3727/49/11/115502 |