2021
DOI: 10.3390/photonics8020041
|View full text |Cite
|
Sign up to set email alerts
|

Optical Characterization of Ultra-Thin Films of Azo-Dye-Doped Polymers Using Ellipsometry and Surface Plasmon Resonance Spectroscopy

Abstract: The determination of optical constants (i.e., real and imaginary parts of the complex refractive index (nc) and thickness (d)) of ultrathin films is often required in photonics. It may be done by using, for example, surface plasmon resonance (SPR) spectroscopy combined with either profilometry or atomic force microscopy (AFM). SPR yields the optical thickness (i.e., the product of nc and d) of the film, while profilometry and AFM yield its thickness, thereby allowing for the separate determination of nc and d.… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
4
1

Citation Types

1
10
0

Year Published

2021
2021
2025
2025

Publication Types

Select...
5
1
1

Relationship

1
6

Authors

Journals

citations
Cited by 14 publications
(11 citation statements)
references
References 63 publications
1
10
0
Order By: Relevance
“…Note that the slope p = 178 of the slow rate k 2 = 0.35 k vs X ′ yields ϕ tc 633.8 nm = 0.11 ± 0.01, confirming that the double exponential with the rates k 1,2 is appropriate for describing PIB dynamics and measuring reaction parameters, such as ϕ , ε trans 632.8 nm = 4.46 × 10 3 L mol –1 cm –1 (σ trans 632.8 nm = 1.7 × 10 –17 cm 2 molecule –1 ) …”
Section: Introductionmentioning
confidence: 64%
“…Note that the slope p = 178 of the slow rate k 2 = 0.35 k vs X ′ yields ϕ tc 633.8 nm = 0.11 ± 0.01, confirming that the double exponential with the rates k 1,2 is appropriate for describing PIB dynamics and measuring reaction parameters, such as ϕ , ε trans 632.8 nm = 4.46 × 10 3 L mol –1 cm –1 (σ trans 632.8 nm = 1.7 × 10 –17 cm 2 molecule –1 ) …”
Section: Introductionmentioning
confidence: 64%
“…The pump beam was in diameter and it was centered on the probe beam and irradiated the plasmonic structure from the back perpendicularly to the plane of the structure. The pump wavelength is close to the absorption maximum of the SL and efficiently induces photoisomerization of DR1 10 , 27 , 28 .…”
Section: Methodsmentioning
confidence: 99%
“…Indeed, SPs are highly sensitive to any change of the metal/dielectric interface, i.e. boundary, such as the adsorption of molecules to the conducting surface 8 , 9 , thereby allowing for thin film sensing and characterization 10 , and SPs waves penetrate to different extents, i.e. penetration depths, into metals and dielectrics, allowing for sensing of changes in the refractive index of media thicker than the SPs penetration depths 11 15 .…”
Section: Introductionmentioning
confidence: 99%
“…The Lorentz oscillator model satisfies the Kramer-Kronig (KK) causality relations. Some authors [8,9] have used Lorentz oscillator models for dispersion relations for azo-dyes. The Lorentz oscillator model can produce realistic absorption frequencies and amplitudes.…”
Section: Introductionmentioning
confidence: 99%
“…The Lorentz oscillator model can produce realistic absorption frequencies and amplitudes. However, as the Lorentz oscillator model tends to predict tails with slower decays, the fitting to the absorption data is poor away from the absorbance peaks [9,10].…”
Section: Introductionmentioning
confidence: 99%