Optical constants
Refractive index of As2S3 (Arsenic trisulfide)
Slavich et al. 2024: Ab initio; n,k(γ) 0.299–2.07 µm
- Data
- tabulated nk
- Range
- 0.2988–2.071 µm
- Points
- 80
- Optical axis
- gamma
- State
- crystalline
- Licence
- CC0-1.0
Plot
Click the plot to set the calculator wavelength.
At one wavelength
- Refractive index n
- 3.0227
- Extinction coefficient k
- 0.00724995
- Permittivity ε1
- 9.13664
- Permittivity ε2
- 0.0438288
- Absorption coefficient α
- 1550.47 cm⁻¹
- Penetration depth δ = λ/(2πk)
- 12899.3 nm
- Abbe number Vd
- —
- Chromatic dispersion dn/dλ
- -0.97004 µm⁻¹
- Group index ng
- 3.59269
- Group velocity dispersion
- — fs²/mm
- Dispersion parameter D
- — ps/(nm·km)
- Photon energy
- 2.11001 eV
ε = (n + ik)², α = 4πk/λ, ng = n − λ dn/dλ, GVD = λ³/(2πc²) d²n/dλ², D = −(λ/c) d²n/dλ². Group-velocity dispersion is given for formula data only.
Use it in Lightsmith
Load this data in Python, simulate in one more line
pip install lightsmith
import lightsmith as ls
# As2S3 (Arsenic trisulfide): Slavich et al. 2024: Ab initio; n,k(γ) 0.299–2.07 µm
as2s3 = ls.fetch_refractiveindex("main", "As2S3", "Slavich-abinitio-gamma", ref="c5c2f188e848453def5970e347399d653df2ffc2")
print(as2s3.range_nm) # (298.75, 2071.15) nm
eps = as2s3.eps([633]) # complex permittivity
Downloads the original record once (pinned to the imported snapshot) and caches it.
import json, urllib.request
import lightsmith as ls
url = "https://materials.lightsmith.dev/v1/datasets/ds_da18fa191441/lightsmith"
as2s3 = ls.Tabulated.model_validate(json.load(urllib.request.urlopen(url)))
print(as2s3.source) # citation and provenance travel with the data
Any dataset here, as the library's Tabulated material (as2s3/slavich-2024-abinitio-gamma).
# ... load as2s3 as above, then:
sim = ls.Simulation(
particles=[ls.Particle(shape=ls.Sphere(radius_nm=50), material=as2s3)],
medium_index=1.0,
wavelengths=ls.WavelengthRange(start_nm=400, stop_nm=1000, num=81),
)
res = ls.solve(sim) # exact Mie for a sphere
print(res.q_ext) # extinction efficiency at each wavelength
Same spec runs with DDA, FDTD, BEM or T-matrix: ls.compare(sim, ["mie", "dda"]).
Lightsmith is open source (MIT): Mie, T-matrix, BEM, DDA, FDTD, RCWA, TMM, mode solvers and inverse design behind one spec, on CPU or GPU. GitHub.
Comments and conditions
Conditions
- direction
- gamma
References
- doi:10.1038/s41377-024-01407-3 Exploring van der Waals materials with high anisotropy: geometrical and optical approaches, Light: Science & Applications (2024)
Cite
Aleksandr S. Slavich et al.. Exploring van der Waals materials with high anisotropy: geometrical and optical approaches. Light: Science & Applications, 13, 68 (2024), doi:10.1038/s41377-024-01407-3; Data from the refractiveindex.info database (M. N. Polyanskiy, Sci. Data 11, 94 (2024), doi:10.1038/s41597-023-02898-2)
Data
80 rows as published| λ (µm) | n | k |
|---|---|---|
| 0.29875 | 4.03606 | 1.08155 |
| 0.30191 | 4.04109 | 1.1839 |
| 0.30514 | 4.23306 | 1.15114 |
| 0.30844 | 4.29428 | 0.89902 |
| 0.31182 | 4.15883 | 0.73277 |
| 0.31527 | 4.04297 | 0.72 |
| 0.31882 | 4.01728 | 0.71191 |
| 0.32244 | 3.98613 | 0.66164 |
| 0.32614 | 3.92871 | 0.64609 |
| 0.32995 | 3.92833 | 0.66601 |
| 0.33384 | 3.95589 | 0.634 |
| 0.33784 | 3.99318 | 0.58173 |
| 0.34194 | 3.9854 | 0.46747 |
| 0.34613 | 3.93536 | 0.40107 |
| 0.35043 | 3.88905 | 0.33647 |
| 0.35485 | 3.824 | 0.28975 |
| 0.3594 | 3.75723 | 0.27467 |
| 0.36405 | 3.73273 | 0.28873 |
| 0.36884 | 3.74355 | 0.25742 |
| 0.37376 | 3.71103 | 0.19082 |
| 0.37882 | 3.651 | 0.16973 |
| 0.38402 | 3.63518 | 0.16624 |
| 0.38937 | 3.61746 | 0.11619 |
| 0.39487 | 3.5696 | 0.08158 |
| 0.40056 | 3.52521 | 0.05862 |
| 0.4064 | 3.47997 | 0.0401 |
| 0.41243 | 3.43564 | 0.03065 |
| 0.41862 | 3.39778 | 0.02658 |
| 0.42502 | 3.36484 | 0.02282 |
| 0.43165 | 3.33387 | 0.01941 |
| 0.43847 | 3.30497 | 0.01731 |
| 0.44553 | 3.27848 | 0.01589 |
| 0.4528 | 3.25395 | 0.01477 |
| 0.46035 | 3.23102 | 0.01382 |
| 0.46815 | 3.20947 | 0.01299 |
| 0.47623 | 3.18918 | 0.01224 |
| 0.48458 | 3.17001 | 0.01159 |
| 0.49324 | 3.15186 | 0.01099 |
| 0.50225 | 3.13455 | 0.01043 |
| 0.51159 | 3.11811 | 0.00994 |
| 0.52129 | 3.10243 | 0.00946 |
| 0.53137 | 3.08749 | 0.00904 |
| 0.54184 | 3.07322 | 0.00862 |
| 0.55278 | 3.05954 | 0.00825 |
| 0.56415 | 3.04645 | 0.00789 |
| 0.57602 | 3.03393 | 0.00755 |
| 0.58837 | 3.02195 | 0.00723 |
| 0.6013 | 3.01042 | 0.00694 |
| 0.61484 | 2.99937 | 0.00665 |
| 0.62899 | 2.98877 | 0.00637 |
| 0.64382 | 2.97861 | 0.00613 |
| 0.65936 | 2.96884 | 0.00588 |
| 0.67571 | 2.95946 | 0.00564 |
| 0.69293 | 2.95045 | 0.00541 |
| 0.71101 | 2.94181 | 0.00518 |
| 0.73006 | 2.9335 | 0.00498 |
| 0.7502 | 2.92553 | 0.00479 |
| 0.77148 | 2.91788 | 0.00459 |
| 0.79406 | 2.91052 | 0.0044 |
| 0.81794 | 2.90348 | 0.00422 |
| 0.84337 | 2.89673 | 0.00404 |
| 0.87042 | 2.89024 | 0.00388 |
| 0.89933 | 2.88403 | 0.00371 |
| 0.93016 | 2.87807 | 0.00354 |
| 0.96326 | 2.87239 | 0.00339 |
| 0.99871 | 2.86695 | 0.00324 |
| 1.03705 | 2.86177 | 0.00309 |
| 1.07835 | 2.8568 | 0.00294 |
| 1.12319 | 2.85207 | 0.0028 |
| 1.1718 | 2.84758 | 0.00267 |
| 1.22493 | 2.84331 | 0.00253 |
| 1.28311 | 2.83924 | 0.0024 |
| 1.34709 | 2.8354 | 0.00227 |
| 1.41795 | 2.83177 | 0.00214 |
| 1.4965 | 2.82834 | 0.00202 |
| 1.58446 | 2.82512 | 0.00189 |
| 1.68318 | 2.82209 | 0.00177 |
| 1.79528 | 2.81927 | 0.00165 |
| 1.92338 | 2.81665 | 0.00154 |
| 2.07115 | 2.8142 | 0.00142 |
Optical transmission calculator
Free-standing sample in vacuum, normal incidence- Transmittance T
- —
- Reflectance R
- —
Fresnel reflection calculator
- Rp
- —
- Rs
- —
- R = (Rp+Rs)/2
- —
- Phase φp
- —
- Phase φs
- —
- Brewster angle θB
- —
- Critical angle θC
- —
γ-axis. Ab initio calculations.