Spiral - Modeling of Waves in Photonic Crystals
J. Barolak, P. Biagioni, G. Pellegrini
1DPC for Superchiral Sensing/Spectroscopy
Dipartimento di Fisica - Università di Pavia
Spiral Meeting, 21 February 2025, Online
Bloch Surface Waves (BSW)
TE ± i*TM
TE ± i*TM
-
Large optical chirality enhancement
-
Uniformity over large areas
-
Optical chirality switching
-
Broadband operation
-
Flat spectral response
Planar Geometries as an Ideal Candidate
Calculation Methods
Dipartimento di Fisica - Università di Pavia
Spiral Meeting, 21 February 2025, Online
Transfer Matrix Method:
\begin{aligned}
\begin{pmatrix}
a_n \\ b_n
\end{pmatrix}
=
\begin{pmatrix}
A & B \\ C & D
\end{pmatrix}^{-n}
\begin{pmatrix}
a_0 \\ b_0
\end{pmatrix}
\end{aligned}
Calculation Methods
Dipartimento di Fisica - Università di Pavia
Spiral Meeting, 21 February 2025, Online
Rigorous Coupled Wave Analysis
(RCWA):
\begin{aligned}
\mathbf{H}(\mathbf{r}, z)= & \sum_{\mathbf{G}}\left(\phi_x(\mathbf{G})\left[\hat{\mathbf{x}}-\frac{1}{q}\left(k_x+G_x\right) \hat{\mathbf{z}}\right]\right. \\
& \left.+\phi_y(\mathbf{G})\left[\hat{\mathbf{y}}-\frac{1}{q}\left(k_y+G_y\right) \hat{\mathbf{z}}\right]\right) e^{i(\mathbf{k}+\mathbf{G}) \cdot \mathbf{r}+i q z}
\end{aligned}
RCWA Solvers
Dipartimento di Fisica - Università di Pavia
Spiral Meeting, 21 February 2025, Online
- Released in 2012
- Written in Lua with a Python interface
- Written in python
- Compatible with many backends
- Contains many different FMM formulations
- Written in Python with Jax
- Advanced features like:
- Brillouin zone integration
- Vector FMM formulations
Automated Design of Photonic Crystals
Dipartimento di Fisica - Università di Pavia
Spiral Meeting, 21 February 2025, Online
Genetic Optimization for improved photonic crystal designs!
}
Input parameters:
- 1DPC Properties
- Illumination properties
θ
n1
n2
t1
t2
t3
t5
t7
t4
t6
Evalutation Functions for Broadband Sensing
Dipartimento di Fisica - Università di Pavia
Spiral Meeting, 21 February 2025, Online
Freedom to choose parameters, constraints and evaluation metrics!
Evaluation 1: Optical Chirality C for 400nm to 450nm
Evaluation 2: Optical Chirality C for 450nm to 500nm
C = -\frac{\epsilon_0 \omega}{2}*Im(E^* \cdot B)
Investigating Parameters from the Optimization
Dipartimento di Fisica - Università di Pavia
Spiral Meeting, 21 February 2025, Online
Parameters:
- 1-7: Thicknesses
- 8: Angle of Incidence
- 9-10: Refractive Indicies
θ
n1
n2
t1
t2
t3
t5
t7
t4
t6
High chirality over a range of wavelengths
Low dielectric contrast
Jones Matrix Analysis: Light as Jones Vectors
Dipartimento di Fisica - Università di Pavia
Spiral Meeting, 21 February 2025, Online
\left[\begin{array}{l}
0 \\
1
\end{array}\right]
\left[\begin{array}{l}
1 \\
0
\end{array}\right]
S-polarized Light - TE:
P-polarized Light - TM:
\frac{1}{\sqrt{2}}
\left[\begin{array}{l}
1 \\
-i
\end{array}\right]
\frac{1}{\sqrt{2}}
\left[\begin{array}{l}
1 \\
i
\end{array}\right]
Right Circular Pol. - R:
Left Circular Pol. - R:
\frac{1}{\sqrt{2}}
\left[\begin{array}{l}
1 \\
1
\end{array}\right]
Diagonal Polarization:
Jones Matrix Analysis: Optical Elements as Jones Matrices
Dipartimento di Fisica - Università di Pavia
Spiral Meeting, 21 February 2025, Online
\left[\begin{array}{cc}
1 & 0 \\
0 & e^{i \varphi}
\end{array}\right]
PEM:
\left[\begin{array}{cc}
r_{p p} & r_{p s} \\
-r_{p s} & r_{s s}
\end{array}\right]
Fresnel R:
S polarizer:
P Polarizer:
45 Polarizer:
\left[\begin{array}{ll}
0 & 0 \\
0 & 1
\end{array}\right]
\left[\begin{array}{ll}
1 & 0 \\
0 & 0
\end{array}\right]
\left[\begin{array}{ll}
\frac{1}{2} & \frac{1}{2} \\[5pt]
\frac{1}{2} & \frac{1}{2}
\end{array}\right]
Jones Matrix Analysis: Combining Optical Elements and Light
Dipartimento di Fisica - Università di Pavia
Spiral Meeting, 21 February 2025, Online
S polarizer:
\left[\begin{array}{ll}
0 & 0 \\
0 & 1
\end{array}\right]
\left[\begin{array}{l}
1 \\
0
\end{array}\right]
P-polarized Light - TM:
\left[\begin{array}{ll}
0 & 0 \\
0 & 1
\end{array}\right]
\cdot
\left[\begin{array}{l}
1 \\
0
\end{array}\right]
=
\left[\begin{array}{l}
0 \\
0
\end{array}\right]
P polarizer:
\left[\begin{array}{ll}
1 & 0 \\
0 & 0
\end{array}\right]
\left[\begin{array}{ll}
1 & 0 \\
0 & 0
\end{array}\right]
\cdot
\frac{1}{\sqrt{2}}
\left[\begin{array}{l}
1 \\
-i
\end{array}\right]
=
\frac{1}{\sqrt{2}}
\left[\begin{array}{l}
1 \\
0
\end{array}\right]
\frac{1}{\sqrt{2}}
\left[\begin{array}{l}
1 \\
-i
\end{array}\right]
Right Circular Pol. - R:
Jones Matrix Analysis: Combining Optical Elements and Light
Dipartimento di Fisica - Università di Pavia
Spiral Meeting, 21 February 2025, Online
PEM:
\left[\begin{array}{cc}
1 & 0 \\
0 & e^{i \varphi}
\end{array}\right]
\left[\begin{array}{l}
0 \\
1
\end{array}\right]
S-polarized Light - TE:
\left[\begin{array}{cc}
1 & 0 \\
0 & e^{i \varphi}
\end{array}\right]
\cdot
\left[\begin{array}{l}
0 \\
1
\end{array}\right]
=
\left[\begin{array}{l}
0 \\
e^{i \varphi}
\end{array}\right]
R:
\left[\begin{array}{cc}
r_{p p} & r_{p s} \\
-r_{p s} & r_{s s}
\end{array}\right]
\left[\begin{array}{l}
0 \\
1
\end{array}\right]
S-polarized Light - TE:
\left[\begin{array}{cc}
r_{p p} & r_{p s} \\
-r_{p s} & r_{s s}
\end{array}\right]
\cdot
\left[\begin{array}{l}
0 \\
1
\end{array}\right]
=
\left[\begin{array}{l}
r_{ps} \\
r_{ss}
\end{array}\right]
A Useful Identity: Jacobi-Anger Identity
Dipartimento di Fisica - Università di Pavia
Spiral Meeting, 21 February 2025, Online
e^{i z \cos \theta} \equiv J_0(z)+2 \sum_{n=1}^{\infty} i^n J_n(z) \cos (n \theta)
\begin{cases}
e^{i \varphi}=e^{i \frac{2 \pi A l}{\lambda} \cos \omega t} \\
\varphi = z \cos \theta \\
z = \frac{2 \pi A l}{\lambda} = \varphi_m=2 \\
\theta = \omega t \\
\Delta n=A \cos \omega t \\
\end{cases}
J_0\left(\varphi_m\right) - [2 i J_1\left(\varphi_m\right)] \cos (\omega t) -[2 J_2\left(\varphi_m\right)] \cos (2 \omega t )
Polimi Original Optical Setup
Dipartimento di Fisica - Università di Pavia
Spiral Meeting, 21 February 2025, Online
M = R \cdot PEM \cdot P45
=
\left[\begin{array}{cc}
\frac{r_{p p}}{2}+\frac{r_{p s} e^{i \varphi}}{2} & \frac{r_{p p}}{2}+\frac{r_{p s} e^{i \varphi}}{2} \\
-\frac{r_{p s}}{2}+\frac{r_{s s} e^{i \varphi}}{2} & -\frac{r_{p s}}{2}+\frac{r_{s s} e^{i \varphi}}{2}
\end{array}\right]
M
\cdot
\left[\begin{array}{cc}
1 \\
0
\end{array}\right]
=
J
=
\left[\begin{array}{c}
\frac{r_{p p}}{2}+\frac{r_{p s} e^{i \varphi}}{2} \\
-\frac{r_{p s}}{2}+\frac{r_{s s} e^{i \varphi}}{2}
\end{array}\right]
I =J \cdot J^{*} = \left[-\frac{r_{p p} e^{i \varphi} \overline{r_{p s}}}{4}+\frac{r_{p p} \overline{r_{p p}}}{2}+\frac{r_{p p} e^{-i \varphi} \overline{r_{p s}}}{4}+\frac{r_{p s} e^{i \varphi} \overline{r_{p p}}}{4}+\frac{r_{p s} \overline{r_{p s}}}{2}-\frac{r_{p s} e^{-i \varphi} \overline{r_{p p}}}{4}\right]
Polimi Original Optical Setup
Dipartimento di Fisica - Università di Pavia
Spiral Meeting, 21 February 2025, Online
After a few trival algebraic steps
\omega \Rightarrow \Im \Biggl \{ \frac{r_{pp}r_{ps}^{*}-r_{ps}r_{ss}^*}{|r_{ss}|^2 + |r_{pp}|^2} \Biggl \}
2 \omega \Rightarrow \Re \Biggl \{ \frac{r_{pp}r_{ps}^{*}-r_{ps}r_{ss}^*}{|r_{ss}|^2 + |r_{pp}|^2} \Biggl \}
R D \simeq \frac{4}{\log (10)} \frac{\operatorname{Re}\left\{e^{-i \phi}\left(r_{pp} r_{p s}^*-r_{p s} r_{s s}^*\right)\right\}}{\left|r_{p p}\right|^2+\left|r_{s s}\right|^2}
But our reflection dichroism is:
J_0\left(\varphi_m\right) - [2 i J_1\left(\varphi_m\right)] \cos (\omega t) -[2 J_2\left(\varphi_m\right)] \cos (2 \omega t )
Alternative Setups
Dipartimento di Fisica - Università di Pavia
Spiral Meeting, 21 February 2025, Online
\omega \Rightarrow \Im \Biggl \{ \frac{r_{ps}}{r_{ss}} \Biggl \}
2 \omega \Rightarrow \Re \Biggl \{ \frac{r_{ps}}{r_{ss}} \Biggl \}
\left[\begin{array}{cc}
r_{p p} & r_{p s} \\
-r_{p s} & r_{s s}
\end{array}\right]
DNA Sensing with 1DPC - Overview
Dipartimento di Fisica - Università di Pavia
Spiral Meeting, 21 February 2025, Online
Utilizing the simultaneous existence of TE and TM surface modes, polarization-resolved spectroscopy was performed during the growth of single-stranded DNA via Rolling Surface Amplification
DNA Sensing with 1DPC - Overview
Dipartimento di Fisica - Università di Pavia
Spiral Meeting, 21 February 2025, Online
S = \frac{d \lambda}{d n}
We can improve data processing by calculating a more realistic sensitivity for our specific photonic crystal design
Simulating the Photonic Crystal Design
Dipartimento di Fisica - Università di Pavia
Spiral Meeting, 21 February 2025, Online
Theoretical sensitivity values depend strongly on the exact photonic crystal structure
Using experimental angular reflectivity spectra and the genetic optimization Giovanni found the experimental values for the photonic crystal's:
- Thickness for each layer
- Absorption values for SIO2 and Ta2O5
Sensitivity as a Function of Wavelength
Dipartimento di Fisica - Università di Pavia
Spiral Meeting, 21 February 2025, Online
TE Mode:
TM Mode:
Sensitivity depends strongly on the refractive index at the top of the crystal:
S \rightarrow S(\lambda)
Sensitivity as a Function of Wavelength
Dipartimento di Fisica - Università di Pavia
Spiral Meeting, 21 February 2025, Online
The sensitivity will strongly depend on the thickness of this "fixed thickness" layer
We will focus on performing an analysis with a 10nm "surface" layer
Analysis of Results with Sensitivity
Dipartimento di Fisica - Università di Pavia
Spiral Meeting, 21 February 2025, Online
Factoring into account the wavelength dependent sensitivity:
Sensitivity as a Function of DNA Thickness
Dipartimento di Fisica - Università di Pavia
Spiral Meeting, 21 February 2025, Online
Experimental Setup at Polimi
Dipartimento di Fisica - Università di Pavia
Spiral Meeting, 21 February 2025, Online
Experimental setup to measure angular reflectivity spectrum and circular dichroism measurements at Polimi:
Total Internal Reflection Verification
Dipartimento di Fisica - Università di Pavia
Spiral Meeting, 21 February 2025, Online
TE-Mode:
TM-Mode:
Spiral - Modeling of Waves in Photonic Crystals
J. Barolak, P. Biagioni, G. Pellegrini
Spiral Meeting 21_02_2024
By Giovanni Pellegrini
