Optical constants
Refractive index of Te (Tellurium)
Guo et al. 2022: n,k(o) 0.400–0.900 µm
- Data
- tabulated nk
- Range
- 0.4–0.9 µm
- Points
- 102
- Optical axis
- o
- Licence
- CC0-1.0
Uniaxial crystal, axes: oe
Plot
Click the plot to set the calculator wavelength.
At one wavelength
- Refractive index n
- 2.26334
- Extinction coefficient k
- 3.11299
- Permittivity ε1
- -4.568
- Permittivity ε2
- 14.0915
- Absorption coefficient α
- 665742 cm⁻¹
- Penetration depth δ = λ/(2πk)
- 30.0417 nm
- Abbe number Vd
- —
- Chromatic dispersion dn/dλ
- 9.828 µm⁻¹
- Group index ng
- -3.51159
- 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(o) 0.400–0.900 µm
te = ls.fetch_refractiveindex("main", "Te", "Guo-o", 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_f6c6be694605/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-o).
# ... 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
- o
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 | 1.06337 | 2.15703 |
| 0.405 | 1.08186 | 2.18582 |
| 0.41 | 1.10076 | 2.21468 |
| 0.415 | 1.12006 | 2.24363 |
| 0.42 | 1.13982 | 2.27265 |
| 0.425 | 1.16004 | 2.30176 |
| 0.43 | 1.18077 | 2.33093 |
| 0.435 | 1.20203 | 2.36019 |
| 0.44 | 1.22385 | 2.3895 |
| 0.445 | 1.24627 | 2.41887 |
| 0.45 | 1.26931 | 2.44828 |
| 0.455 | 1.29302 | 2.47771 |
| 0.46 | 1.31743 | 2.50715 |
| 0.465 | 1.34257 | 2.53659 |
| 0.47 | 1.36849 | 2.56598 |
| 0.475 | 1.39521 | 2.59531 |
| 0.48 | 1.42278 | 2.62454 |
| 0.485 | 1.45123 | 2.65363 |
| 0.49 | 1.48059 | 2.68255 |
| 0.495 | 1.51091 | 2.71125 |
| 0.5 | 1.54222 | 2.73967 |
| 0.505 | 1.57454 | 2.76777 |
| 0.51 | 1.60791 | 2.79548 |
| 0.515 | 1.64236 | 2.82274 |
| 0.52 | 1.6779 | 2.84946 |
| 0.525 | 1.71455 | 2.87559 |
| 0.53 | 1.75233 | 2.90102 |
| 0.532 | 1.76854 | 2.91148 |
| 0.535 | 1.79124 | 2.92568 |
| 0.54 | 1.83129 | 2.94948 |
| 0.545 | 1.87245 | 2.97231 |
| 0.55 | 1.91472 | 2.99408 |
| 0.555 | 1.95807 | 3.01468 |
| 0.56 | 2.00245 | 3.03401 |
| 0.565 | 2.04783 | 3.05197 |
| 0.57 | 2.09413 | 3.06845 |
| 0.575 | 2.14128 | 3.08334 |
| 0.58 | 2.1892 | 3.09656 |
| 0.585 | 2.23779 | 3.10801 |
| 0.59 | 2.28693 | 3.11759 |
| 0.595 | 2.33651 | 3.12525 |
| 0.6 | 2.38639 | 3.13091 |
| 0.605 | 2.43642 | 3.13452 |
| 0.61 | 2.48645 | 3.13604 |
| 0.615 | 2.53633 | 3.13546 |
| 0.62 | 2.58589 | 3.13276 |
| 0.625 | 2.63497 | 3.12797 |
| 0.63 | 2.68341 | 3.12111 |
| 0.635 | 2.73104 | 3.11223 |
| 0.64 | 2.77772 | 3.1014 |
| 0.645 | 2.82329 | 3.0887 |
| 0.65 | 2.86762 | 3.07424 |
| 0.655 | 2.91058 | 3.05811 |
| 0.66 | 2.95207 | 3.04045 |
| 0.665 | 2.99199 | 3.0214 |
| 0.67 | 3.03026 | 3.00108 |
| 0.675 | 3.06682 | 2.97965 |
| 0.68 | 3.10163 | 2.95725 |
| 0.685 | 3.13465 | 2.93404 |
| 0.69 | 3.16586 | 2.91015 |
| 0.695 | 3.19528 | 2.88574 |
| 0.7 | 3.22292 | 2.86094 |
| 0.705 | 3.2488 | 2.83587 |
| 0.71 | 3.27295 | 2.81067 |
| 0.715 | 3.29544 | 2.78545 |
| 0.72 | 3.31631 | 2.76032 |
| 0.725 | 3.33562 | 2.73536 |
| 0.73 | 3.35345 | 2.71067 |
| 0.735 | 3.36985 | 2.68632 |
| 0.74 | 3.38492 | 2.66238 |
| 0.745 | 3.39871 | 2.63891 |
| 0.75 | 3.41131 | 2.61596 |
| 0.755 | 3.42279 | 2.59357 |
| 0.76 | 3.43322 | 2.57178 |
| 0.765 | 3.44268 | 2.55061 |
| 0.77 | 3.45124 | 2.53008 |
| 0.775 | 3.45896 | 2.51021 |
| 0.78 | 3.46591 | 2.49101 |
| 0.785 | 3.47216 | 2.47249 |
| 0.79 | 3.47775 | 2.45464 |
| 0.795 | 3.48276 | 2.43746 |
| 0.8 | 3.48723 | 2.42096 |
| 0.805 | 3.4912 | 2.40512 |
| 0.81 | 3.49474 | 2.38994 |
| 0.815 | 3.49788 | 2.37539 |
| 0.82 | 3.50065 | 2.36148 |
| 0.825 | 3.50311 | 2.34818 |
| 0.83 | 3.50528 | 2.33547 |
| 0.835 | 3.5072 | 2.32336 |
| 0.84 | 3.5089 | 2.3118 |
| 0.845 | 3.5104 | 2.3008 |
| 0.85 | 3.51173 | 2.29033 |
| 0.855 | 3.51291 | 2.28038 |
| 0.86 | 3.51397 | 2.27092 |
| 0.865 | 3.51493 | 2.26195 |
| 0.87 | 3.51579 | 2.25343 |
| 0.875 | 3.51659 | 2.24537 |
| 0.88 | 3.51733 | 2.23773 |
| 0.885 | 3.51802 | 2.23051 |
| 0.89 | 3.51869 | 2.22368 |
| 0.895 | 3.51934 | 2.21724 |
| 0.9 | 3.51998 | 2.21116 |
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. Ordinary ray (o).