Optical constants
Refractive index of GeS2 (Germanium disulfide)
Slavich et al. 1989: n,k(γ) 0.299–2.04 µm
- Data
- tabulated nk
- Range
- 0.2994–2.042 µm
- Points
- 31
- Optical axis
- gamma
- Licence
- CC0-1.0
Biaxial crystal, axes: gamma
Plot
Click the plot to set the calculator wavelength.
At one wavelength
- Refractive index n
- 2.02134
- Extinction coefficient k
- 0.00986217
- Permittivity ε1
- 4.08573
- Permittivity ε2
- 0.0398696
- Absorption coefficient α
- 2109.12 cm⁻¹
- Penetration depth δ = λ/(2πk)
- 9482.65 nm
- Abbe number Vd
- —
- Chromatic dispersion dn/dλ
- -0.478405 µm⁻¹
- Group index ng
- 2.30245
- 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
# GeS2 (Germanium disulfide): Slavich et al. 1989: n,k(γ) 0.299–2.04 µm
ges2 = ls.fetch_refractiveindex("main", "GeS2", "Slavich-abinitio-γ", ref="c5c2f188e848453def5970e347399d653df2ffc2")
print(ges2.range_nm) # (299.45, 2042.16) nm
eps = ges2.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_8c209ab0ce29/lightsmith"
ges2 = ls.Tabulated.model_validate(json.load(urllib.request.urlopen(url)))
print(ges2.source) # citation and provenance travel with the data
Any dataset here, as the library's Tabulated material (ges2/slavich-1989-abinitio-3).
# ... load ges2 as above, then:
sim = ls.Simulation(
particles=[ls.Particle(shape=ls.Sphere(radius_nm=50), material=ges2)],
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/s41377-025-01886-y Germanium disulfide as an alternative high refractive index and transparent material for UV-visible nanophotonics, Light: Science & Applications (2025)
Cite
Aleksandr S. Slavich et al.. Germanium disulfide as an alternative high refractive index and transparent material for UV-visible nanophotonics. Light: Science & Applications, 14, 213 (2025), doi:10.1038/s41377-025-01886-y; Data from the refractiveindex.info database (M. N. Polyanskiy, Sci. Data 11, 94 (2024), doi:10.1038/s41597-023-02898-2)
Data
31 rows as published| λ (µm) | n | k |
|---|---|---|
| 0.29945 | 1.92573 | 0.37155 |
| 0.30785 | 1.93402 | 0.44457 |
| 0.31676 | 2.00167 | 0.49376 |
| 0.32624 | 2.07341 | 0.49802 |
| 0.33633 | 2.14576 | 0.48228 |
| 0.34711 | 2.2155 | 0.42995 |
| 0.35864 | 2.24937 | 0.35548 |
| 0.371 | 2.25325 | 0.28727 |
| 0.38431 | 2.25041 | 0.23338 |
| 0.39862 | 2.23554 | 0.17904 |
| 0.41412 | 2.22085 | 0.13959 |
| 0.43091 | 2.19639 | 0.09024 |
| 0.44916 | 2.1626 | 0.0621 |
| 0.46913 | 2.13175 | 0.03678 |
| 0.49099 | 2.09783 | 0.02255 |
| 0.51506 | 2.07007 | 0.01647 |
| 0.5417 | 2.0478 | 0.01292 |
| 0.5713 | 2.02914 | 0.01064 |
| 0.60441 | 2.0133 | 0.00906 |
| 0.64169 | 1.99967 | 0.00785 |
| 0.68395 | 1.98777 | 0.00684 |
| 0.73234 | 1.97731 | 0.00602 |
| 0.78815 | 1.96808 | 0.00531 |
| 0.85329 | 1.95993 | 0.00469 |
| 0.93037 | 1.95272 | 0.00412 |
| 1.02293 | 1.94636 | 0.00362 |
| 1.13605 | 1.94078 | 0.00317 |
| 1.27756 | 1.93593 | 0.00274 |
| 1.45951 | 1.93174 | 0.00236 |
| 1.70213 | 1.92816 | 0.00197 |
| 2.04216 | 1.92518 | 0.00164 |
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
- —
n(γ),k(γ). Ab initio calculations.