Optical constants
Refractive index of MoTe2 (Molybdenum ditelluride)
Beal and Huges 1979: n,k 0.069–1.22 µm
- Data
- tabulated nk
- Range
- 0.06911–1.216 µm
- Points
- 100
- Licence
- CC0-1.0
Plot
Click the plot to set the calculator wavelength.
At one wavelength
- Refractive index n
- 3.89825
- Extinction coefficient k
- 1.51925
- Permittivity ε1
- 12.8882
- Permittivity ε2
- 11.8448
- Absorption coefficient α
- 324906 cm⁻¹
- Penetration depth δ = λ/(2πk)
- 61.5563 nm
- Abbe number Vd
- —
- Chromatic dispersion dn/dλ
- -1.81034 µm⁻¹
- Group index ng
- 4.96201
- 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
# MoTe2 (Molybdenum ditelluride): Beal and Huges 1979: n,k 0.069–1.22 µm
mote2 = ls.fetch_refractiveindex("main", "MoTe2", "Beal", ref="c5c2f188e848453def5970e347399d653df2ffc2")
print(mote2.range_nm) # (69.11, 1216) nm
eps = mote2.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_fc80d5446b4c/lightsmith"
mote2 = ls.Tabulated.model_validate(json.load(urllib.request.urlopen(url)))
print(mote2.source) # citation and provenance travel with the data
Any dataset here, as the library's Tabulated material (mote2/beal-huges-1979).
# ... load mote2 as above, then:
sim = ls.Simulation(
particles=[ls.Particle(shape=ls.Sphere(radius_nm=50), material=mote2)],
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.
References
- doi:10.1088/0022-3719/12/5/017 Kramers-Kronig analysis of the reflectivity spectra of 2H-MoS <sub>2</sub> , 2H-MoSe <sub>2</sub> and 2H-MoTe <sub>2</sub>, Journal of Physics C: Solid State Physics (1979)
Cite
A R Beal and H P Hughes. Kramers-Kronig analysis of the reflectivity spectra of 2H-MoS <sub>2</sub> , 2H-MoSe <sub>2</sub> and 2H-MoTe <sub>2</sub>. Journal of Physics C: Solid State Physics, 12, 881-890 (1979), doi:10.1088/0022-3719/12/5/017; Data from the refractiveindex.info database (M. N. Polyanskiy, Sci. Data 11, 94 (2024), doi:10.1038/s41597-023-02898-2)
Data
100 rows as published| λ (µm) | n | k |
|---|---|---|
| 0.06911 | 0.5384 | 0.5143 |
| 0.0807 | 0.577 | 0.8162 |
| 0.09228 | 0.6574 | 1.045 |
| 0.1039 | 0.7485 | 1.229 |
| 0.1155 | 0.8149 | 1.415 |
| 0.127 | 1.042 | 1.591 |
| 0.1386 | 1.423 | 1.689 |
| 0.1502 | 1.67 | 1.423 |
| 0.1618 | 1.504 | 1.115 |
| 0.1734 | 1.312 | 1.153 |
| 0.185 | 1.132 | 1.375 |
| 0.1966 | 1.088 | 1.672 |
| 0.2082 | 1.202 | 2.015 |
| 0.2197 | 1.382 | 2.211 |
| 0.2313 | 1.583 | 2.331 |
| 0.2429 | 1.793 | 2.341 |
| 0.2545 | 2.002 | 2.329 |
| 0.2661 | 2.132 | 2.262 |
| 0.2777 | 2.245 | 2.181 |
| 0.2893 | 2.276 | 2.213 |
| 0.3008 | 2.315 | 2.253 |
| 0.3124 | 2.453 | 2.361 |
| 0.324 | 2.593 | 2.409 |
| 0.3356 | 2.705 | 2.432 |
| 0.3472 | 2.814 | 2.457 |
| 0.3588 | 3.015 | 2.35 |
| 0.3704 | 3.097 | 2.251 |
| 0.382 | 3.114 | 2.203 |
| 0.3935 | 3.147 | 2.2 |
| 0.4051 | 3.182 | 2.198 |
| 0.4167 | 3.241 | 2.233 |
| 0.4283 | 3.3 | 2.269 |
| 0.4399 | 3.485 | 2.189 |
| 0.4515 | 3.567 | 2.161 |
| 0.4631 | 3.641 | 2.14 |
| 0.4747 | 3.716 | 2.121 |
| 0.4862 | 3.792 | 2.101 |
| 0.4978 | 3.926 | 2.052 |
| 0.5094 | 4.024 | 1.968 |
| 0.521 | 4.056 | 1.868 |
| 0.5326 | 4.051 | 1.673 |
| 0.5442 | 4.04 | 1.599 |
| 0.5558 | 3.982 | 1.543 |
| 0.5673 | 3.936 | 1.52 |
| 0.5789 | 3.914 | 1.52 |
| 0.5905 | 3.893 | 1.519 |
| 0.6021 | 3.877 | 1.529 |
| 0.6137 | 3.876 | 1.551 |
| 0.6253 | 3.9 | 1.563 |
| 0.6369 | 3.924 | 1.576 |
| 0.6485 | 3.948 | 1.588 |
| 0.66 | 3.976 | 1.6 |
| 0.6716 | 4.036 | 1.611 |
| 0.6832 | 4.095 | 1.622 |
| 0.6948 | 4.153 | 1.633 |
| 0.7064 | 4.211 | 1.644 |
| 0.718 | 4.276 | 1.638 |
| 0.7296 | 4.36 | 1.617 |
| 0.7412 | 4.444 | 1.597 |
| 0.7527 | 4.517 | 1.553 |
| 0.7643 | 4.558 | 1.426 |
| 0.7759 | 4.613 | 1.365 |
| 0.7875 | 4.615 | 1.32 |
| 0.7991 | 4.617 | 1.275 |
| 0.8107 | 4.62 | 1.229 |
| 0.8223 | 4.624 | 1.184 |
| 0.8338 | 4.609 | 1.143 |
| 0.8454 | 4.59 | 1.103 |
| 0.857 | 4.582 | 1.11 |
| 0.8686 | 4.583 | 1.156 |
| 0.8802 | 4.668 | 1.056 |
| 0.8918 | 4.776 | 0.9488 |
| 0.9034 | 4.783 | 0.8653 |
| 0.915 | 4.793 | 0.7936 |
| 0.9265 | 4.782 | 0.7253 |
| 0.9381 | 4.767 | 0.6601 |
| 0.9497 | 4.755 | 0.6114 |
| 0.9613 | 4.743 | 0.5624 |
| 0.9729 | 4.731 | 0.5131 |
| 0.9845 | 4.699 | 0.4655 |
| 0.9961 | 4.659 | 0.45 |
| 1.008 | 4.618 | 0.4344 |
| 1.019 | 4.577 | 0.4185 |
| 1.031 | 4.535 | 0.4023 |
| 1.042 | 4.494 | 0.3981 |
| 1.054 | 4.477 | 0.3995 |
| 1.066 | 4.466 | 0.4005 |
| 1.077 | 4.454 | 0.4015 |
| 1.089 | 4.443 | 0.4026 |
| 1.1 | 4.412 | 0.4194 |
| 1.112 | 4.381 | 0.4469 |
| 1.124 | 4.359 | 0.4739 |
| 1.135 | 4.393 | 0.4947 |
| 1.147 | 4.427 | 0.5152 |
| 1.158 | 4.461 | 0.5354 |
| 1.17 | 4.492 | 0.5277 |
| 1.181 | 4.517 | 0.4747 |
| 1.193 | 4.542 | 0.4222 |
| 1.205 | 4.568 | 0.3703 |
| 1.216 | 4.595 | 0.3189 |
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
- —