Optical constants
Refractive index of As2S3 (Arsenic trisulfide)
Slavich et al. 2024: Ab initio; n,k(α) 0.299–2.07 µm
- Data
- tabulated nk
- Range
- 0.2988–2.071 µm
- Points
- 80
- Optical axis
- alpha
- State
- crystalline
- Licence
- CC0-1.0
Plot
Click the plot to set the calculator wavelength.
At one wavelength
- Refractive index n
- 2.23114
- Extinction coefficient k
- 0.00407434
- Permittivity ε1
- 4.97798
- Permittivity ε2
- 0.0181809
- Absorption coefficient α
- 871.335 cm⁻¹
- Penetration depth δ = λ/(2πk)
- 22953.3 nm
- Abbe number Vd
- —
- Chromatic dispersion dn/dλ
- -0.548988 µm⁻¹
- Group index ng
- 2.55373
- 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(α) 0.299–2.07 µm
as2s3 = ls.fetch_refractiveindex("main", "As2S3", "Slavich-abinitio-alpha", 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_3f5258eb909f/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-alpha).
# ... 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
- alpha
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 | 2.39145 | 0.56305 |
| 0.30191 | 2.41578 | 0.54508 |
| 0.30514 | 2.40858 | 0.53071 |
| 0.30844 | 2.4207 | 0.53991 |
| 0.31182 | 2.43407 | 0.51921 |
| 0.31527 | 2.4213 | 0.51751 |
| 0.31882 | 2.4542 | 0.54007 |
| 0.32244 | 2.4941 | 0.50914 |
| 0.32614 | 2.50831 | 0.46818 |
| 0.32995 | 2.49622 | 0.43456 |
| 0.33384 | 2.49765 | 0.4261 |
| 0.33784 | 2.4992 | 0.39661 |
| 0.34194 | 2.49983 | 0.36694 |
| 0.34613 | 2.44537 | 0.32899 |
| 0.35043 | 2.40563 | 0.38863 |
| 0.35485 | 2.45626 | 0.43059 |
| 0.3594 | 2.49817 | 0.41758 |
| 0.36405 | 2.55963 | 0.39697 |
| 0.36884 | 2.58401 | 0.30296 |
| 0.37376 | 2.50601 | 0.24202 |
| 0.37882 | 2.4773 | 0.30214 |
| 0.38402 | 2.51755 | 0.30262 |
| 0.38937 | 2.54261 | 0.284 |
| 0.39487 | 2.56571 | 0.25702 |
| 0.40056 | 2.59229 | 0.2125 |
| 0.4064 | 2.59302 | 0.14877 |
| 0.41243 | 2.57122 | 0.09249 |
| 0.41862 | 2.5309 | 0.04652 |
| 0.42502 | 2.48484 | 0.02682 |
| 0.43165 | 2.44983 | 0.01951 |
| 0.43847 | 2.42232 | 0.01567 |
| 0.44553 | 2.39947 | 0.01323 |
| 0.4528 | 2.37984 | 0.01149 |
| 0.46035 | 2.36252 | 0.0102 |
| 0.46815 | 2.34699 | 0.00918 |
| 0.47623 | 2.33295 | 0.00834 |
| 0.48458 | 2.32012 | 0.00765 |
| 0.49324 | 2.3083 | 0.00706 |
| 0.50225 | 2.29731 | 0.00655 |
| 0.51159 | 2.28708 | 0.00612 |
| 0.52129 | 2.27753 | 0.00573 |
| 0.53137 | 2.26857 | 0.00538 |
| 0.54184 | 2.26014 | 0.00507 |
| 0.55278 | 2.25216 | 0.00477 |
| 0.56415 | 2.24464 | 0.00452 |
| 0.57602 | 2.2375 | 0.00429 |
| 0.58837 | 2.23072 | 0.00406 |
| 0.6013 | 2.2243 | 0.00387 |
| 0.61484 | 2.21816 | 0.00367 |
| 0.62899 | 2.21233 | 0.0035 |
| 0.64382 | 2.20676 | 0.00333 |
| 0.65936 | 2.20146 | 0.00318 |
| 0.67571 | 2.19639 | 0.00303 |
| 0.69293 | 2.19155 | 0.0029 |
| 0.71101 | 2.18692 | 0.00277 |
| 0.73006 | 2.1825 | 0.00266 |
| 0.7502 | 2.17828 | 0.00252 |
| 0.77148 | 2.17424 | 0.00241 |
| 0.79406 | 2.17037 | 0.0023 |
| 0.81794 | 2.16668 | 0.00222 |
| 0.84337 | 2.16315 | 0.0021 |
| 0.87042 | 2.15977 | 0.00201 |
| 0.89933 | 2.15653 | 0.00192 |
| 0.93016 | 2.15344 | 0.00183 |
| 0.96326 | 2.15051 | 0.00174 |
| 0.99871 | 2.1477 | 0.00168 |
| 1.03705 | 2.14502 | 0.00159 |
| 1.07835 | 2.14248 | 0.00152 |
| 1.12319 | 2.14005 | 0.00145 |
| 1.1718 | 2.13773 | 0.00136 |
| 1.22493 | 2.13556 | 0.00129 |
| 1.28311 | 2.13347 | 0.00122 |
| 1.34709 | 2.13153 | 0.00115 |
| 1.41795 | 2.12967 | 0.0011 |
| 1.4965 | 2.12793 | 0.00103 |
| 1.58446 | 2.12629 | 0.000964121 |
| 1.68318 | 2.12474 | 0.000894229 |
| 1.79528 | 2.1233 | 0.000847737 |
| 1.92338 | 2.12198 | 0.000777576 |
| 2.07115 | 2.12073 | 0.00073088 |
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
- —
α-axis. Ab initio calculations.