Optical constants
Refractive index of Si (Silicon)
Jellison 1992: n,k 0.234–0.840 µm
- Data
- tabulated nk
- Range
- 0.234–0.84 µm
- Points
- 186
- State
- crystalline
- Licence
- CC0-1.0
Plot
Click the plot to set the calculator wavelength.
At one wavelength
- Refractive index n
- 3.96528
- Extinction coefficient k
- 0.022
- Permittivity ε1
- 15.723
- Permittivity ε2
- 0.174472
- Absorption coefficient α
- 4704.9 cm⁻¹
- Penetration depth δ = λ/(2πk)
- 4250.88 nm
- Abbe number Vd
- —
- Chromatic dispersion dn/dλ
- -2.2 µm⁻¹
- Group index ng
- 5.258
- 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
# Si (Silicon): Jellison 1992: n,k 0.234–0.840 µm
si = ls.fetch_refractiveindex("main", "Si", "Jellison", ref="c5c2f188e848453def5970e347399d653df2ffc2")
print(si.range_nm) # (234, 840) nm
eps = si.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_750b75523c30/lightsmith"
si = ls.Tabulated.model_validate(json.load(urllib.request.urlopen(url)))
print(si.source) # citation and provenance travel with the data
Any dataset here, as the library's Tabulated material (si/jellison-1992).
# ... load si as above, then:
sim = ls.Simulation(
particles=[ls.Particle(shape=ls.Sphere(radius_nm=50), material=si)],
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)90015-f Optical functions of silicon determined by two-channel polarization modulation ellipsometry, Optical Materials (1992)
Cite
G.E. Jellison. Optical functions of silicon determined by two-channel polarization modulation ellipsometry. Optical Materials, 1, 41-47 (1992), doi:10.1016/0925-3467(92)90015-f; Data from the refractiveindex.info database (M. N. Polyanskiy, Sci. Data 11, 94 (2024), doi:10.1038/s41597-023-02898-2)
Data
186 rows as published| λ (µm) | n | k |
|---|---|---|
| 0.234 | 1.688 | 3.444 |
| 0.236 | 1.701 | 3.424 |
| 0.238 | 1.691 | 3.435 |
| 0.24 | 1.683 | 3.452 |
| 0.242 | 1.678 | 3.453 |
| 0.244 | 1.683 | 3.5 |
| 0.246 | 1.683 | 3.552 |
| 0.248 | 1.683 | 3.609 |
| 0.25 | 1.693 | 3.668 |
| 0.252 | 1.706 | 3.732 |
| 0.254 | 1.734 | 3.805 |
| 0.256 | 1.742 | 3.89 |
| 0.258 | 1.773 | 3.977 |
| 0.26 | 1.799 | 4.074 |
| 0.262 | 1.838 | 4.181 |
| 0.264 | 1.889 | 4.29 |
| 0.266 | 1.953 | 4.416 |
| 0.268 | 2.025 | 4.553 |
| 0.27 | 2.129 | 4.695 |
| 0.272 | 2.265 | 4.84 |
| 0.274 | 2.432 | 4.972 |
| 0.276 | 2.61 | 5.09 |
| 0.278 | 2.825 | 5.189 |
| 0.28 | 3.055 | 5.263 |
| 0.282 | 3.279 | 5.311 |
| 0.284 | 3.545 | 5.348 |
| 0.286 | 3.834 | 5.356 |
| 0.288 | 4.142 | 5.303 |
| 0.29 | 4.435 | 5.164 |
| 0.292 | 4.688 | 4.959 |
| 0.294 | 4.861 | 4.727 |
| 0.296 | 4.966 | 4.506 |
| 0.298 | 5.024 | 4.304 |
| 0.3 | 5.059 | 4.126 |
| 0.302 | 5.076 | 3.973 |
| 0.304 | 5.079 | 3.845 |
| 0.306 | 5.078 | 3.734 |
| 0.308 | 5.072 | 3.639 |
| 0.31 | 5.077 | 3.555 |
| 0.312 | 5.073 | 3.482 |
| 0.314 | 5.078 | 3.419 |
| 0.316 | 5.086 | 3.362 |
| 0.318 | 5.088 | 3.315 |
| 0.32 | 5.104 | 3.266 |
| 0.322 | 5.11 | 3.227 |
| 0.324 | 5.12 | 3.189 |
| 0.326 | 5.137 | 3.151 |
| 0.328 | 5.161 | 3.116 |
| 0.33 | 5.181 | 3.083 |
| 0.332 | 5.194 | 3.053 |
| 0.334 | 5.22 | 3.021 |
| 0.336 | 5.245 | 2.997 |
| 0.338 | 5.269 | 2.974 |
| 0.34 | 5.295 | 2.951 |
| 0.342 | 5.327 | 2.935 |
| 0.344 | 5.359 | 2.921 |
| 0.346 | 5.393 | 2.912 |
| 0.348 | 5.435 | 2.905 |
| 0.35 | 5.486 | 2.904 |
| 0.352 | 5.548 | 2.907 |
| 0.354 | 5.625 | 2.918 |
| 0.356 | 5.729 | 2.923 |
| 0.358 | 5.856 | 2.929 |
| 0.36 | 6.018 | 2.912 |
| 0.362 | 6.212 | 2.849 |
| 0.364 | 6.421 | 2.732 |
| 0.366 | 6.617 | 2.555 |
| 0.368 | 6.773 | 2.319 |
| 0.37 | 6.871 | 2.049 |
| 0.372 | 6.909 | 1.758 |
| 0.374 | 6.88 | 1.484 |
| 0.376 | 6.792 | 1.236 |
| 0.378 | 6.676 | 1.033 |
| 0.38 | 6.548 | 0.875 |
| 0.382 | 6.406 | 0.742 |
| 0.384 | 6.282 | 0.645 |
| 0.386 | 6.173 | 0.57 |
| 0.388 | 6.069 | 0.509 |
| 0.39 | 5.972 | 0.457 |
| 0.392 | 5.88 | 0.415 |
| 0.394 | 5.803 | 0.38 |
| 0.396 | 5.726 | 0.348 |
| 0.398 | 5.651 | 0.321 |
| 0.4 | 5.585 | 0.296 |
| 0.402 | 5.522 | 0.275 |
| 0.404 | 5.461 | 0.258 |
| 0.406 | 5.406 | 0.242 |
| 0.408 | 5.352 | 0.227 |
| 0.41 | 5.301 | 0.215 |
| 0.412 | 5.254 | 0.203 |
| 0.414 | 5.21 | 0.192 |
| 0.416 | 5.168 | 0.182 |
| 0.418 | 5.125 | 0.173 |
| 0.42 | 5.087 | 0.165 |
| 0.422 | 5.052 | 0.158 |
| 0.424 | 5.015 | 0.151 |
| 0.426 | 4.983 | 0.145 |
| 0.428 | 4.95 | 0.138 |
| 0.43 | 4.921 | 0.133 |
| 0.432 | 4.893 | 0.127 |
| 0.434 | 4.865 | 0.123 |
| 0.436 | 4.841 | 0.118 |
| 0.438 | 4.815 | 0.115 |
| 0.44 | 4.79 | 0.109 |
| 0.442 | 4.766 | 0.107 |
| 0.444 | 4.742 | 0.103 |
| 0.446 | 4.718 | 0.099 |
| 0.448 | 4.695 | 0.096 |
| 0.45 | 4.673 | 0.092 |
| 0.455 | 4.622 | 0.085 |
| 0.46 | 4.574 | 0.079 |
| 0.465 | 4.529 | 0.074 |
| 0.47 | 4.488 | 0.068 |
| 0.475 | 4.45 | 0.064 |
| 0.48 | 4.413 | 0.06 |
| 0.485 | 4.379 | 0.057 |
| 0.49 | 4.345 | 0.053 |
| 0.495 | 4.317 | 0.05 |
| 0.5 | 4.29 | 0.047 |
| 0.505 | 4.262 | 0.045 |
| 0.51 | 4.237 | 0.042 |
| 0.515 | 4.214 | 0.04 |
| 0.52 | 4.19 | 0.038 |
| 0.525 | 4.168 | 0.036 |
| 0.53 | 4.148 | 0.034 |
| 0.535 | 4.129 | 0.033 |
| 0.54 | 4.108 | 0.031 |
| 0.545 | 4.092 | 0.03 |
| 0.55 | 4.075 | 0.029 |
| 0.555 | 4.059 | 0.028 |
| 0.56 | 4.042 | 0.026 |
| 0.565 | 4.027 | 0.025 |
| 0.57 | 4.013 | 0.025 |
| 0.575 | 3.998 | 0.023 |
| 0.58 | 3.984 | 0.023 |
| 0.585 | 3.971 | 0.022 |
| 0.59 | 3.96 | 0.022 |
| 0.595 | 3.948 | 0.021 |
| 0.6 | 3.937 | 0.019 |
| 0.605 | 3.926 | 0.019 |
| 0.61 | 3.914 | 0.019 |
| 0.615 | 3.904 | 0.018 |
| 0.62 | 3.893 | 0.017 |
| 0.625 | 3.885 | 0.017 |
| 0.63 | 3.877 | 0.016 |
| 0.635 | 3.869 | 0.016 |
| 0.645 | 3.85 | 0.015 |
| 0.65 | 3.842 | 0.014 |
| 0.655 | 3.834 | 0.014 |
| 0.66 | 3.828 | 0.014 |
| 0.665 | 3.819 | 0.013 |
| 0.67 | 3.813 | 0.013 |
| 0.675 | 3.804 | 0.012 |
| 0.68 | 3.798 | 0.013 |
| 0.685 | 3.791 | 0.012 |
| 0.69 | 3.785 | 0.012 |
| 0.695 | 3.779 | 0.01 |
| 0.7 | 3.772 | 0.011 |
| 0.705 | 3.766 | 0.011 |
| 0.71 | 3.76 | 0.01 |
| 0.715 | 3.756 | 0.009 |
| 0.72 | 3.75 | 0.01 |
| 0.725 | 3.744 | 0.01 |
| 0.73 | 3.738 | 0.011 |
| 0.735 | 3.736 | 0.008 |
| 0.74 | 3.731 | 0.009 |
| 0.745 | 3.725 | 0.008 |
| 0.75 | 3.72 | 0.007 |
| 0.755 | 3.719 | 0.008 |
| 0.76 | 3.712 | 0.008 |
| 0.765 | 3.706 | 0.007 |
| 0.77 | 3.706 | 0.006 |
| 0.775 | 3.699 | 0.007 |
| 0.78 | 3.695 | 0.006 |
| 0.785 | 3.691 | 0.005 |
| 0.79 | 3.686 | 0.007 |
| 0.795 | 3.683 | 0.009 |
| 0.8 | 3.682 | 0.006 |
| 0.805 | 3.676 | 0.007 |
| 0.81 | 3.673 | 0.007 |
| 0.815 | 3.669 | 0.007 |
| 0.82 | 3.666 | 0.005 |
| 0.825 | 3.662 | 0.005 |
| 0.83 | 3.663 | 0.006 |
| 0.835 | 3.656 | 0.005 |
| 0.84 | 3.659 | 0.004 |
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>; n-type, 0.2-0.3 Ω·cm; Room temperature