Optical constants
Refractive index of Ge (Germanium)
Jellison 1992: n,k 0.234–0.840 µm
- Data
- tabulated nk
- Range
- 0.234–0.84 µm
- Points
- 187
- Licence
- CC0-1.0
Plot
Click the plot to set the calculator wavelength.
At one wavelength
- Refractive index n
- 5.76624
- Extinction coefficient k
- 1.62336
- Permittivity ε1
- 30.6142
- Permittivity ε2
- 18.7214
- Absorption coefficient α
- 347171 cm⁻¹
- Penetration depth δ = λ/(2πk)
- 57.6086 nm
- Abbe number Vd
- —
- Chromatic dispersion dn/dλ
- 12.4 µm⁻¹
- Group index ng
- -1.52
- 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
# Ge (Germanium): Jellison 1992: n,k 0.234–0.840 µm
ge = ls.fetch_refractiveindex("main", "Ge", "Jellison", ref="c5c2f188e848453def5970e347399d653df2ffc2")
print(ge.range_nm) # (234, 840) nm
eps = ge.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_564c05b4c296/lightsmith"
ge = ls.Tabulated.model_validate(json.load(urllib.request.urlopen(url)))
print(ge.source) # citation and provenance travel with the data
Any dataset here, as the library's Tabulated material (ge/jellison-1992).
# ... load ge as above, then:
sim = ls.Simulation(
particles=[ls.Particle(shape=ls.Sphere(radius_nm=50), material=ge)],
medium_index=1.0,
wavelengths=ls.WavelengthRange(start_nm=400, stop_nm=840, 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
References
- doi:10.1016/0925-3467(92)90022-f Optical functions of GaAs, GaP, and Ge determined by two-channel polarization modulation ellipsometry, Optical Materials (1992)
Cite
G.E. Jellison. Optical functions of GaAs, GaP, and Ge determined by two-channel polarization modulation ellipsometry. Optical Materials, 1, 151-160 (1992), doi:10.1016/0925-3467(92)90022-f; Data from the refractiveindex.info database (M. N. Polyanskiy, Sci. Data 11, 94 (2024), doi:10.1038/s41597-023-02898-2)
Data
187 rows as published| λ (µm) | n | k |
|---|---|---|
| 0.234 | 1.444 | 3.009 |
| 0.236 | 1.474 | 3.036 |
| 0.238 | 1.421 | 3.047 |
| 0.24 | 1.413 | 3.085 |
| 0.242 | 1.431 | 3.144 |
| 0.244 | 1.441 | 3.181 |
| 0.246 | 1.457 | 3.232 |
| 0.248 | 1.472 | 3.286 |
| 0.25 | 1.488 | 3.343 |
| 0.252 | 1.507 | 3.394 |
| 0.254 | 1.529 | 3.455 |
| 0.256 | 1.552 | 3.521 |
| 0.258 | 1.576 | 3.584 |
| 0.26 | 1.608 | 3.66 |
| 0.262 | 1.647 | 3.729 |
| 0.264 | 1.684 | 3.806 |
| 0.266 | 1.724 | 3.885 |
| 0.268 | 1.783 | 3.977 |
| 0.27 | 1.842 | 4.069 |
| 0.272 | 1.902 | 4.172 |
| 0.274 | 1.999 | 4.292 |
| 0.276 | 2.107 | 4.412 |
| 0.278 | 2.263 | 4.545 |
| 0.28 | 2.468 | 4.665 |
| 0.282 | 2.72 | 4.731 |
| 0.284 | 2.996 | 4.731 |
| 0.286 | 3.248 | 4.656 |
| 0.288 | 3.461 | 4.53 |
| 0.29 | 3.624 | 4.385 |
| 0.292 | 3.756 | 4.234 |
| 0.294 | 3.831 | 4.087 |
| 0.296 | 3.891 | 3.954 |
| 0.298 | 3.926 | 3.836 |
| 0.3 | 3.957 | 3.725 |
| 0.302 | 3.973 | 3.627 |
| 0.304 | 3.986 | 3.541 |
| 0.306 | 3.989 | 3.466 |
| 0.308 | 3.993 | 3.398 |
| 0.31 | 4.002 | 3.333 |
| 0.312 | 4.01 | 3.273 |
| 0.314 | 4.016 | 3.222 |
| 0.316 | 4.009 | 3.18 |
| 0.318 | 4.016 | 3.135 |
| 0.32 | 4.019 | 3.098 |
| 0.322 | 4.024 | 3.062 |
| 0.324 | 4.031 | 3.025 |
| 0.326 | 4.031 | 2.993 |
| 0.328 | 4.035 | 2.96 |
| 0.33 | 4.038 | 2.932 |
| 0.332 | 4.046 | 2.904 |
| 0.334 | 4.057 | 2.876 |
| 0.336 | 4.056 | 2.853 |
| 0.338 | 4.064 | 2.828 |
| 0.34 | 4.067 | 2.802 |
| 0.342 | 4.076 | 2.779 |
| 0.344 | 4.082 | 2.758 |
| 0.346 | 4.082 | 2.74 |
| 0.348 | 4.091 | 2.72 |
| 0.35 | 4.101 | 2.697 |
| 0.352 | 4.107 | 2.679 |
| 0.354 | 4.112 | 2.663 |
| 0.356 | 4.118 | 2.645 |
| 0.358 | 4.128 | 2.627 |
| 0.36 | 4.137 | 2.609 |
| 0.362 | 4.147 | 2.592 |
| 0.364 | 4.161 | 2.57 |
| 0.366 | 4.172 | 2.553 |
| 0.368 | 4.184 | 2.533 |
| 0.37 | 4.19 | 2.514 |
| 0.372 | 4.201 | 2.494 |
| 0.374 | 4.211 | 2.471 |
| 0.376 | 4.223 | 2.446 |
| 0.378 | 4.23 | 2.423 |
| 0.38 | 4.232 | 2.401 |
| 0.382 | 4.238 | 2.375 |
| 0.384 | 4.238 | 2.355 |
| 0.386 | 4.242 | 2.332 |
| 0.388 | 4.245 | 2.309 |
| 0.39 | 4.247 | 2.285 |
| 0.392 | 4.245 | 2.263 |
| 0.394 | 4.239 | 2.239 |
| 0.396 | 4.234 | 2.218 |
| 0.398 | 4.231 | 2.195 |
| 0.4 | 4.223 | 2.181 |
| 0.402 | 4.215 | 2.165 |
| 0.404 | 4.203 | 2.151 |
| 0.406 | 4.193 | 2.14 |
| 0.408 | 4.181 | 2.129 |
| 0.41 | 4.169 | 2.122 |
| 0.412 | 4.16 | 2.116 |
| 0.414 | 4.155 | 2.108 |
| 0.416 | 4.146 | 2.106 |
| 0.418 | 4.138 | 2.102 |
| 0.42 | 4.13 | 2.102 |
| 0.422 | 4.125 | 2.102 |
| 0.424 | 4.12 | 2.103 |
| 0.426 | 4.101 | 2.111 |
| 0.428 | 4.097 | 2.113 |
| 0.43 | 4.099 | 2.116 |
| 0.432 | 4.097 | 2.122 |
| 0.434 | 4.095 | 2.127 |
| 0.436 | 4.097 | 2.132 |
| 0.438 | 4.1 | 2.136 |
| 0.44 | 4.102 | 2.143 |
| 0.442 | 4.104 | 2.15 |
| 0.444 | 4.106 | 2.157 |
| 0.446 | 4.111 | 2.163 |
| 0.448 | 4.114 | 2.171 |
| 0.45 | 4.121 | 2.177 |
| 0.455 | 4.138 | 2.195 |
| 0.46 | 4.158 | 2.214 |
| 0.465 | 4.182 | 2.234 |
| 0.47 | 4.208 | 2.256 |
| 0.475 | 4.241 | 2.273 |
| 0.48 | 4.273 | 2.291 |
| 0.485 | 4.318 | 2.309 |
| 0.49 | 4.359 | 2.331 |
| 0.495 | 4.407 | 2.348 |
| 0.5 | 4.46 | 2.366 |
| 0.505 | 4.521 | 2.382 |
| 0.51 | 4.592 | 2.395 |
| 0.515 | 4.667 | 2.408 |
| 0.52 | 4.756 | 2.414 |
| 0.525 | 4.857 | 2.404 |
| 0.53 | 4.957 | 2.378 |
| 0.535 | 5.062 | 2.314 |
| 0.54 | 5.136 | 2.242 |
| 0.545 | 5.186 | 2.166 |
| 0.55 | 5.226 | 2.106 |
| 0.555 | 5.26 | 2.056 |
| 0.56 | 5.3 | 2.019 |
| 0.565 | 5.349 | 1.988 |
| 0.57 | 5.42 | 1.964 |
| 0.575 | 5.521 | 1.925 |
| 0.58 | 5.635 | 1.837 |
| 0.585 | 5.734 | 1.705 |
| 0.59 | 5.796 | 1.548 |
| 0.595 | 5.811 | 1.389 |
| 0.6 | 5.791 | 1.241 |
| 0.605 | 5.759 | 1.119 |
| 0.61 | 5.71 | 1.011 |
| 0.615 | 5.66 | 0.924 |
| 0.62 | 5.608 | 0.851 |
| 0.625 | 5.552 | 0.791 |
| 0.63 | 5.494 | 0.734 |
| 0.635 | 5.449 | 0.691 |
| 0.64 | 5.403 | 0.651 |
| 0.645 | 5.36 | 0.614 |
| 0.65 | 5.318 | 0.585 |
| 0.655 | 5.278 | 0.556 |
| 0.66 | 5.245 | 0.532 |
| 0.665 | 5.203 | 0.508 |
| 0.67 | 5.173 | 0.49 |
| 0.675 | 5.141 | 0.47 |
| 0.68 | 5.114 | 0.454 |
| 0.685 | 5.086 | 0.439 |
| 0.69 | 5.06 | 0.424 |
| 0.695 | 5.035 | 0.411 |
| 0.7 | 5.008 | 0.397 |
| 0.705 | 4.985 | 0.386 |
| 0.71 | 4.965 | 0.376 |
| 0.715 | 4.944 | 0.367 |
| 0.72 | 4.932 | 0.356 |
| 0.725 | 4.913 | 0.348 |
| 0.73 | 4.894 | 0.342 |
| 0.735 | 4.876 | 0.332 |
| 0.74 | 4.856 | 0.324 |
| 0.745 | 4.845 | 0.319 |
| 0.75 | 4.826 | 0.312 |
| 0.755 | 4.812 | 0.305 |
| 0.76 | 4.797 | 0.298 |
| 0.765 | 4.782 | 0.293 |
| 0.77 | 4.769 | 0.289 |
| 0.775 | 4.758 | 0.283 |
| 0.78 | 4.74 | 0.276 |
| 0.785 | 4.734 | 0.271 |
| 0.79 | 4.718 | 0.266 |
| 0.795 | 4.709 | 0.263 |
| 0.8 | 4.699 | 0.259 |
| 0.805 | 4.691 | 0.252 |
| 0.81 | 4.679 | 0.255 |
| 0.815 | 4.67 | 0.253 |
| 0.82 | 4.655 | 0.245 |
| 0.825 | 4.649 | 0.237 |
| 0.83 | 4.644 | 0.237 |
| 0.835 | 4.628 | 0.24 |
| 0.84 | 4.626 | 0.237 |
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
- —
Crysal orientation: <100>; Room temperature