Optical constants
Refractive index of MoSe2 (Molybdenum diselenide)
Beal and Huges 1979: n,k 0.044–1.16 µm
- Data
- tabulated nk
- Range
- 0.04387–1.161 µm
- Points
- 100
- Licence
- CC0-1.0
Plot
Click the plot to set the calculator wavelength.
At one wavelength
- Refractive index n
- 4.92055
- Extinction coefficient k
- 1.45312
- Permittivity ε1
- 22.1002
- Permittivity ε2
- 14.3003
- Absorption coefficient α
- 310764 cm⁻¹
- Penetration depth δ = λ/(2πk)
- 64.3575 nm
- Abbe number Vd
- —
- Chromatic dispersion dn/dλ
- -2.47788 µm⁻¹
- Group index ng
- 6.37655
- 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
# MoSe2 (Molybdenum diselenide): Beal and Huges 1979: n,k 0.044–1.16 µm
mose2 = ls.fetch_refractiveindex("main", "MoSe2", "Beal", ref="c5c2f188e848453def5970e347399d653df2ffc2")
print(mose2.range_nm) # (43.87, 1161) nm
eps = mose2.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_2edd7e47387a/lightsmith"
mose2 = ls.Tabulated.model_validate(json.load(urllib.request.urlopen(url)))
print(mose2.source) # citation and provenance travel with the data
Any dataset here, as the library's Tabulated material (mose2/beal-huges-1979).
# ... load mose2 as above, then:
sim = ls.Simulation(
particles=[ls.Particle(shape=ls.Sphere(radius_nm=50), material=mose2)],
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 |
|---|---|---|
| 0.04387 | 0.6836 | 0.1856 |
| 0.05515 | 0.5662 | 0.3514 |
| 0.06643 | 0.5705 | 0.7109 |
| 0.07771 | 0.6754 | 0.9288 |
| 0.08899 | 0.7897 | 1.083 |
| 0.1003 | 0.9104 | 1.284 |
| 0.1116 | 1.19 | 1.439 |
| 0.1228 | 1.449 | 1.311 |
| 0.1341 | 1.486 | 1.094 |
| 0.1454 | 1.348 | 0.9137 |
| 0.1567 | 0.9456 | 1.098 |
| 0.168 | 0.9233 | 1.488 |
| 0.1792 | 1.063 | 1.743 |
| 0.1905 | 1.191 | 1.9 |
| 0.2018 | 1.312 | 2.038 |
| 0.2131 | 1.452 | 2.18 |
| 0.2244 | 1.604 | 2.305 |
| 0.2357 | 1.758 | 2.34 |
| 0.2469 | 1.9 | 2.374 |
| 0.2582 | 2.01 | 2.43 |
| 0.2695 | 2.111 | 2.492 |
| 0.2808 | 2.237 | 2.536 |
| 0.2921 | 2.431 | 2.609 |
| 0.3033 | 2.573 | 2.637 |
| 0.3146 | 2.765 | 2.504 |
| 0.3259 | 2.815 | 2.432 |
| 0.3372 | 2.825 | 2.382 |
| 0.3485 | 2.787 | 2.365 |
| 0.3597 | 2.755 | 2.445 |
| 0.371 | 2.819 | 2.615 |
| 0.3823 | 2.917 | 2.752 |
| 0.3936 | 3.071 | 2.903 |
| 0.4049 | 3.259 | 2.974 |
| 0.4162 | 3.473 | 3.076 |
| 0.4274 | 3.811 | 2.95 |
| 0.4387 | 3.993 | 2.898 |
| 0.45 | 4.127 | 2.806 |
| 0.4613 | 4.23 | 2.708 |
| 0.4726 | 4.336 | 2.613 |
| 0.4838 | 4.443 | 2.521 |
| 0.4951 | 4.533 | 2.421 |
| 0.5064 | 4.619 | 2.323 |
| 0.5177 | 4.705 | 2.223 |
| 0.529 | 4.782 | 2.108 |
| 0.5403 | 4.848 | 2.001 |
| 0.5515 | 4.908 | 1.872 |
| 0.5628 | 4.918 | 1.699 |
| 0.5741 | 4.94 | 1.568 |
| 0.5854 | 4.926 | 1.465 |
| 0.5967 | 4.898 | 1.404 |
| 0.6079 | 4.869 | 1.342 |
| 0.6192 | 4.832 | 1.282 |
| 0.6305 | 4.802 | 1.248 |
| 0.6418 | 4.772 | 1.214 |
| 0.6531 | 4.741 | 1.18 |
| 0.6644 | 4.719 | 1.181 |
| 0.6756 | 4.71 | 1.234 |
| 0.6869 | 4.81 | 1.259 |
| 0.6982 | 4.94 | 1.236 |
| 0.7095 | 5.009 | 1.075 |
| 0.7208 | 4.978 | 0.9804 |
| 0.732 | 4.947 | 0.8852 |
| 0.7433 | 4.889 | 0.8568 |
| 0.7546 | 4.827 | 0.8284 |
| 0.7659 | 4.786 | 0.859 |
| 0.7772 | 4.766 | 0.9429 |
| 0.7884 | 4.787 | 1.048 |
| 0.7997 | 4.993 | 1.158 |
| 0.811 | 5.246 | 1.013 |
| 0.8223 | 5.408 | 0.6857 |
| 0.8336 | 5.467 | 0.4406 |
| 0.8449 | 5.391 | 0.3316 |
| 0.8561 | 5.318 | 0.2698 |
| 0.8674 | 5.11 | 0.2118 |
| 0.8787 | 5.008 | 0.1468 |
| 0.89 | 4.905 | 0.07925 |
| 0.9013 | 4.823 | 0.008703 |
| 0.9125 | 4.746 | 0.0 |
| 0.9238 | 4.67 | 0.0 |
| 0.9351 | 4.641 | 0.0 |
| 0.9464 | 4.611 | 0.0 |
| 0.9577 | 4.581 | 0.0 |
| 0.969 | 4.551 | 0.0 |
| 0.9802 | 4.52 | 0.0 |
| 0.9915 | 4.49 | 0.0 |
| 1.003 | 4.461 | 0.0 |
| 1.014 | 4.446 | 0.0 |
| 1.025 | 4.432 | 0.0 |
| 1.037 | 4.418 | 0.0 |
| 1.048 | 4.404 | 0.0 |
| 1.059 | 4.389 | 0.0 |
| 1.07 | 4.375 | 5.504e-05 |
| 1.082 | 4.36 | 0.000268 |
| 1.093 | 4.346 | 0.0004823 |
| 1.104 | 4.332 | 0.000698 |
| 1.116 | 4.318 | 0.0009152 |
| 1.127 | 4.303 | 0.001134 |
| 1.138 | 4.289 | 0.001354 |
| 1.149 | 4.275 | 0.001575 |
| 1.161 | 4.26 | 0.001798 |
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
- —