Optical constants
Refractive index of Te (Tellurium)
Guo et al. 2022: n,k(e) 0.400–0.900 µm
- Data
- tabulated nk
- Range
- 0.4–0.9 µm
- Points
- 102
- Optical axis
- e
- Licence
- CC0-1.0
Uniaxial crystal, axes: oe
Plot
Click the plot to set the calculator wavelength.
At one wavelength
- Refractive index n
- 1.85476
- Extinction coefficient k
- 3.72751
- Permittivity ε1
- -10.4542
- Permittivity ε2
- 13.8272
- Absorption coefficient α
- 797163 cm⁻¹
- Penetration depth δ = λ/(2πk)
- 25.089 nm
- Abbe number Vd
- —
- Chromatic dispersion dn/dλ
- 7.81 µm⁻¹
- Group index ng
- -2.7344
- 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
# Te (Tellurium): Guo et al. 2022: n,k(e) 0.400–0.900 µm
te = ls.fetch_refractiveindex("main", "Te", "Guo-e", ref="c5c2f188e848453def5970e347399d653df2ffc2")
print(te.range_nm) # (400, 900) nm
eps = te.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_9efe351cb6ca/lightsmith"
te = ls.Tabulated.model_validate(json.load(urllib.request.urlopen(url)))
print(te.source) # citation and provenance travel with the data
Any dataset here, as the library's Tabulated material (te/guo-2022-e).
# ... load te as above, then:
sim = ls.Simulation(
particles=[ls.Particle(shape=ls.Sphere(radius_nm=50), material=te)],
medium_index=1.0,
wavelengths=ls.WavelengthRange(start_nm=400, stop_nm=900, 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
- e
References
- doi:10.1039/d2nr03226k Giant in-plane optical and electronic anisotropy of tellurene: a quantitative exploration, Nanoscale (2022)
Cite
Zhengfeng Guo, Honggang Gu, Mingsheng Fang, Lei Ye and Shiyuan Liu. Giant in-plane optical and electronic anisotropy of tellurene: a quantitative exploration. Nanoscale, 14, 12238-12246 (2022), doi:10.1039/d2nr03226k; Data from the refractiveindex.info database (M. N. Polyanskiy, Sci. Data 11, 94 (2024), doi:10.1038/s41597-023-02898-2)
Data
102 rows as published| λ (µm) | n | k |
|---|---|---|
| 0.4 | 0.85284 | 2.54422 |
| 0.405 | 0.87113 | 2.57785 |
| 0.41 | 0.88972 | 2.61141 |
| 0.415 | 0.90859 | 2.64492 |
| 0.42 | 0.92778 | 2.67837 |
| 0.425 | 0.94728 | 2.71177 |
| 0.43 | 0.96711 | 2.74513 |
| 0.435 | 0.98729 | 2.77844 |
| 0.44 | 1.00781 | 2.8117 |
| 0.445 | 1.02871 | 2.84492 |
| 0.45 | 1.04999 | 2.87809 |
| 0.455 | 1.07168 | 2.9112 |
| 0.46 | 1.09377 | 2.94427 |
| 0.465 | 1.1163 | 2.97728 |
| 0.47 | 1.13927 | 3.01023 |
| 0.475 | 1.16272 | 3.04311 |
| 0.48 | 1.18664 | 3.07591 |
| 0.485 | 1.21107 | 3.10863 |
| 0.49 | 1.23602 | 3.14125 |
| 0.495 | 1.26152 | 3.17377 |
| 0.5 | 1.28757 | 3.20616 |
| 0.505 | 1.31421 | 3.23842 |
| 0.51 | 1.34144 | 3.27052 |
| 0.515 | 1.3693 | 3.30245 |
| 0.52 | 1.3978 | 3.33418 |
| 0.525 | 1.42696 | 3.36569 |
| 0.53 | 1.45681 | 3.39696 |
| 0.532 | 1.46955 | 3.41001 |
| 0.535 | 1.48735 | 3.42795 |
| 0.54 | 1.51861 | 3.45863 |
| 0.545 | 1.5506 | 3.48897 |
| 0.55 | 1.58335 | 3.51893 |
| 0.555 | 1.61686 | 3.54847 |
| 0.56 | 1.65114 | 3.57755 |
| 0.565 | 1.68621 | 3.60612 |
| 0.57 | 1.72208 | 3.63414 |
| 0.575 | 1.75874 | 3.66156 |
| 0.58 | 1.7962 | 3.68832 |
| 0.585 | 1.83445 | 3.71437 |
| 0.59 | 1.8735 | 3.73964 |
| 0.595 | 1.91332 | 3.76409 |
| 0.6 | 1.9539 | 3.78764 |
| 0.605 | 1.99522 | 3.81024 |
| 0.61 | 2.03726 | 3.83182 |
| 0.615 | 2.07997 | 3.85232 |
| 0.62 | 2.12333 | 3.87168 |
| 0.625 | 2.16728 | 3.88984 |
| 0.63 | 2.21178 | 3.90673 |
| 0.635 | 2.25676 | 3.9223 |
| 0.64 | 2.30216 | 3.93649 |
| 0.645 | 2.34791 | 3.94925 |
| 0.65 | 2.39393 | 3.96054 |
| 0.655 | 2.44013 | 3.97032 |
| 0.66 | 2.48644 | 3.97856 |
| 0.665 | 2.53275 | 3.98522 |
| 0.67 | 2.57897 | 3.9903 |
| 0.675 | 2.62499 | 3.99377 |
| 0.68 | 2.67072 | 3.99565 |
| 0.685 | 2.71606 | 3.99594 |
| 0.69 | 2.76089 | 3.99466 |
| 0.695 | 2.80512 | 3.99184 |
| 0.7 | 2.84865 | 3.98751 |
| 0.705 | 2.89138 | 3.98172 |
| 0.71 | 2.93321 | 3.97454 |
| 0.715 | 2.97407 | 3.96601 |
| 0.72 | 3.01387 | 3.95621 |
| 0.725 | 3.05254 | 3.94523 |
| 0.73 | 3.09001 | 3.93314 |
| 0.735 | 3.12623 | 3.92003 |
| 0.74 | 3.16115 | 3.90599 |
| 0.745 | 3.19472 | 3.89113 |
| 0.75 | 3.22693 | 3.87553 |
| 0.755 | 3.25774 | 3.8593 |
| 0.76 | 3.28715 | 3.84252 |
| 0.765 | 3.31515 | 3.8253 |
| 0.77 | 3.34174 | 3.80773 |
| 0.775 | 3.36694 | 3.78989 |
| 0.78 | 3.39077 | 3.77188 |
| 0.785 | 3.41324 | 3.75378 |
| 0.79 | 3.4344 | 3.73566 |
| 0.795 | 3.45426 | 3.71759 |
| 0.8 | 3.47288 | 3.69965 |
| 0.805 | 3.4903 | 3.6819 |
| 0.81 | 3.50655 | 3.66439 |
| 0.815 | 3.5217 | 3.64718 |
| 0.82 | 3.53578 | 3.63031 |
| 0.825 | 3.54885 | 3.61382 |
| 0.83 | 3.56096 | 3.59775 |
| 0.835 | 3.57216 | 3.58214 |
| 0.84 | 3.5825 | 3.56699 |
| 0.845 | 3.59204 | 3.55235 |
| 0.85 | 3.60081 | 3.53823 |
| 0.855 | 3.60888 | 3.52464 |
| 0.86 | 3.61629 | 3.5116 |
| 0.865 | 3.62308 | 3.4991 |
| 0.87 | 3.6293 | 3.48717 |
| 0.875 | 3.63499 | 3.47579 |
| 0.88 | 3.64019 | 3.46498 |
| 0.885 | 3.64494 | 3.45473 |
| 0.89 | 3.64929 | 3.44503 |
| 0.895 | 3.65325 | 3.43588 |
| 0.9 | 3.65688 | 3.42728 |
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
- —
Tellurene. Extraordinary ray (e).