Optical constants
Refractive index of As2S3 (Arsenic trisulfide)
Slavich et al. 2024: Ab initio; n,k(β) 0.299–2.07 µm
- Data
- tabulated nk
- Range
- 0.2988–2.071 µm
- Points
- 80
- Optical axis
- beta
- State
- crystalline
- Licence
- CC0-1.0
Plot
Click the plot to set the calculator wavelength.
At one wavelength
- Refractive index n
- 2.77533
- Extinction coefficient k
- 0.00674057
- Permittivity ε1
- 7.70239
- Permittivity ε2
- 0.0374146
- Absorption coefficient α
- 1441.53 cm⁻¹
- Penetration depth δ = λ/(2πk)
- 13874.1 nm
- Abbe number Vd
- —
- Chromatic dispersion dn/dλ
- -0.903644 µm⁻¹
- Group index ng
- 3.30631
- 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(β) 0.299–2.07 µm
as2s3 = ls.fetch_refractiveindex("main", "As2S3", "Slavich-abinitio-beta", 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_e79bef4e386b/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-beta).
# ... 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
- beta
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 | 3.48991 | 0.98646 |
| 0.30191 | 3.49974 | 0.96294 |
| 0.30514 | 3.54744 | 0.88781 |
| 0.30844 | 3.52197 | 0.77871 |
| 0.31182 | 3.47842 | 0.73525 |
| 0.31527 | 3.4471 | 0.68791 |
| 0.31882 | 3.41528 | 0.65891 |
| 0.32244 | 3.3791 | 0.62826 |
| 0.32614 | 3.34932 | 0.62678 |
| 0.32995 | 3.33672 | 0.626 |
| 0.33384 | 3.35165 | 0.63329 |
| 0.33784 | 3.39067 | 0.59696 |
| 0.34194 | 3.37906 | 0.52883 |
| 0.34613 | 3.36087 | 0.51412 |
| 0.35043 | 3.38391 | 0.47333 |
| 0.35485 | 3.35773 | 0.3881 |
| 0.3594 | 3.29167 | 0.35997 |
| 0.36405 | 3.26264 | 0.36228 |
| 0.36884 | 3.25029 | 0.33439 |
| 0.37376 | 3.17049 | 0.31165 |
| 0.37882 | 3.14849 | 0.41603 |
| 0.38402 | 3.26181 | 0.43188 |
| 0.38937 | 3.29217 | 0.32343 |
| 0.39487 | 3.25271 | 0.29623 |
| 0.40056 | 3.28845 | 0.28199 |
| 0.4064 | 3.28854 | 0.18086 |
| 0.41243 | 3.23369 | 0.13588 |
| 0.41862 | 3.1981 | 0.10641 |
| 0.42502 | 3.16952 | 0.0811 |
| 0.43165 | 3.13326 | 0.04499 |
| 0.43847 | 3.08559 | 0.02805 |
| 0.44553 | 3.04719 | 0.02192 |
| 0.4528 | 3.01529 | 0.01856 |
| 0.46035 | 2.98754 | 0.0163 |
| 0.46815 | 2.96279 | 0.01463 |
| 0.47623 | 2.94039 | 0.01331 |
| 0.48458 | 2.91987 | 0.01224 |
| 0.49324 | 2.90094 | 0.01134 |
| 0.50225 | 2.88326 | 0.01056 |
| 0.51159 | 2.86676 | 0.00989 |
| 0.52129 | 2.85128 | 0.00929 |
| 0.53137 | 2.83672 | 0.00876 |
| 0.54184 | 2.82295 | 0.00827 |
| 0.55278 | 2.8099 | 0.00783 |
| 0.56415 | 2.79753 | 0.00744 |
| 0.57602 | 2.78579 | 0.00705 |
| 0.58837 | 2.77463 | 0.00672 |
| 0.6013 | 2.76397 | 0.0064 |
| 0.61484 | 2.7538 | 0.0061 |
| 0.62899 | 2.74411 | 0.00583 |
| 0.64382 | 2.73485 | 0.00556 |
| 0.65936 | 2.72601 | 0.00532 |
| 0.67571 | 2.71754 | 0.00508 |
| 0.69293 | 2.70943 | 0.00485 |
| 0.71101 | 2.70169 | 0.00465 |
| 0.73006 | 2.69428 | 0.00444 |
| 0.7502 | 2.68718 | 0.00426 |
| 0.77148 | 2.68038 | 0.00407 |
| 0.79406 | 2.67386 | 0.00389 |
| 0.81794 | 2.66764 | 0.00373 |
| 0.84337 | 2.66167 | 0.00357 |
| 0.87042 | 2.65598 | 0.00341 |
| 0.89933 | 2.65051 | 0.00324 |
| 0.93016 | 2.6453 | 0.0031 |
| 0.96326 | 2.64032 | 0.00297 |
| 0.99871 | 2.63557 | 0.00283 |
| 1.03705 | 2.63103 | 0.0027 |
| 1.07835 | 2.62671 | 0.00257 |
| 1.12319 | 2.6226 | 0.00244 |
| 1.1718 | 2.6187 | 0.00231 |
| 1.22493 | 2.61498 | 0.0022 |
| 1.28311 | 2.61146 | 0.00209 |
| 1.34709 | 2.60812 | 0.00197 |
| 1.41795 | 2.60498 | 0.00186 |
| 1.4965 | 2.60202 | 0.00175 |
| 1.58446 | 2.59923 | 0.00164 |
| 1.68318 | 2.59661 | 0.00154 |
| 1.79528 | 2.59417 | 0.00143 |
| 1.92338 | 2.59191 | 0.00133 |
| 2.07115 | 2.58979 | 0.00124 |
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
- —
β-axis. Ab initio calculations.