Optical constants
Refractive index of BaTiO3 (Barium titanate)
Johnston 1971: Clamped measurements; n,k 0.4–1.0 µm
- Data
- tabulated nk
- Range
- 0.4–1 µm
- Points
- 100
- State
- crystalline
- Licence
- CC0-1.0
Plot
Click the plot to set the calculator wavelength.
At one wavelength
- Refractive index n
- 2.41062
- Extinction coefficient k
- 0.176723
- Permittivity ε1
- 5.77988
- Permittivity ε2
- 0.852027
- Absorption coefficient α
- 37793.9 cm⁻¹
- Penetration depth δ = λ/(2πk)
- 529.186 nm
- Abbe number Vd
- —
- Chromatic dispersion dn/dλ
- -0.445545 µm⁻¹
- Group index ng
- 2.67243
- 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
# BaTiO3 (Barium titanate): Johnston 1971: Clamped measurements; n,k 0.4–1.0 µm
batio3 = ls.fetch_refractiveindex("main", "BaTiO3", "Johnston-x-clamped", ref="c5c2f188e848453def5970e347399d653df2ffc2")
print(batio3.range_nm) # (400, 1000) nm
eps = batio3.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_37b3103a31cd/lightsmith"
batio3 = ls.Tabulated.model_validate(json.load(urllib.request.urlopen(url)))
print(batio3.source) # citation and provenance travel with the data
Any dataset here, as the library's Tabulated material (batio3/johnston-1971-x-clamped).
# ... load batio3 as above, then:
sim = ls.Simulation(
particles=[ls.Particle(shape=ls.Sphere(radius_nm=50), material=batio3)],
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.
Comments and conditions
References
- doi:10.1063/1.1660761 Dispersion of Electro-Optic Effect in BaTiO3, Journal of Applied Physics (1971)
Cite
Alan R. Johnston. Dispersion of Electro-Optic Effect in BaTiO3. Journal of Applied Physics, 42, 3501-3507 (1971), doi:10.1063/1.1660761; 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 |
|---|---|---|
| 0.4 | 2.6122 | 0.33864 |
| 0.40606 | 2.5978 | 0.32693 |
| 0.41212 | 2.5845 | 0.31622 |
| 0.41818 | 2.5721 | 0.30639 |
| 0.42424 | 2.5606 | 0.29732 |
| 0.4303 | 2.5499 | 0.28891 |
| 0.43636 | 2.5399 | 0.2811 |
| 0.44242 | 2.5305 | 0.27381 |
| 0.44848 | 2.5218 | 0.26699 |
| 0.45455 | 2.5136 | 0.26059 |
| 0.46061 | 2.5058 | 0.25456 |
| 0.46667 | 2.4986 | 0.24888 |
| 0.47273 | 2.4917 | 0.2435 |
| 0.47879 | 2.4852 | 0.23841 |
| 0.48485 | 2.4791 | 0.23358 |
| 0.49091 | 2.4733 | 0.22898 |
| 0.49697 | 2.4678 | 0.2246 |
| 0.50303 | 2.4626 | 0.22041 |
| 0.50909 | 2.4576 | 0.21642 |
| 0.51515 | 2.4529 | 0.21259 |
| 0.52121 | 2.4484 | 0.20893 |
| 0.52727 | 2.4442 | 0.20541 |
| 0.53333 | 2.4401 | 0.20203 |
| 0.53939 | 2.4362 | 0.19879 |
| 0.54545 | 2.4325 | 0.19566 |
| 0.55152 | 2.4289 | 0.19264 |
| 0.55758 | 2.4255 | 0.18974 |
| 0.56364 | 2.4222 | 0.18693 |
| 0.5697 | 2.4191 | 0.18422 |
| 0.57576 | 2.4161 | 0.1816 |
| 0.58182 | 2.4132 | 0.17906 |
| 0.58788 | 2.4105 | 0.17661 |
| 0.59394 | 2.4078 | 0.17423 |
| 0.6 | 2.4053 | 0.17192 |
| 0.60606 | 2.4028 | 0.16968 |
| 0.61212 | 2.4004 | 0.16751 |
| 0.61818 | 2.3982 | 0.1654 |
| 0.62424 | 2.396 | 0.16335 |
| 0.6303 | 2.3938 | 0.16135 |
| 0.63636 | 2.3918 | 0.15941 |
| 0.64242 | 2.3898 | 0.15752 |
| 0.64848 | 2.3879 | 0.15568 |
| 0.65455 | 2.3861 | 0.15389 |
| 0.66061 | 2.3843 | 0.15214 |
| 0.66667 | 2.3826 | 0.15044 |
| 0.67273 | 2.3809 | 0.14877 |
| 0.67879 | 2.3793 | 0.14715 |
| 0.68485 | 2.3777 | 0.14557 |
| 0.69091 | 2.3762 | 0.14402 |
| 0.69697 | 2.3747 | 0.14251 |
| 0.70303 | 2.3733 | 0.14104 |
| 0.70909 | 2.3719 | 0.13959 |
| 0.71515 | 2.3706 | 0.13818 |
| 0.72121 | 2.3693 | 0.1368 |
| 0.72727 | 2.368 | 0.13545 |
| 0.73333 | 2.3668 | 0.13413 |
| 0.73939 | 2.3656 | 0.13284 |
| 0.74545 | 2.3644 | 0.13157 |
| 0.75152 | 2.3633 | 0.13033 |
| 0.75758 | 2.3622 | 0.12911 |
| 0.76364 | 2.3611 | 0.12792 |
| 0.7697 | 2.3601 | 0.12675 |
| 0.77576 | 2.3591 | 0.1256 |
| 0.78182 | 2.3581 | 0.12448 |
| 0.78788 | 2.3572 | 0.12338 |
| 0.79394 | 2.3562 | 0.1223 |
| 0.8 | 2.3553 | 0.12123 |
| 0.80606 | 2.3544 | 0.12019 |
| 0.81212 | 2.3536 | 0.11917 |
| 0.81818 | 2.3527 | 0.11816 |
| 0.82424 | 2.3519 | 0.11718 |
| 0.8303 | 2.3511 | 0.11621 |
| 0.83636 | 2.3503 | 0.11526 |
| 0.84242 | 2.3496 | 0.11432 |
| 0.84848 | 2.3488 | 0.1134 |
| 0.85455 | 2.3481 | 0.1125 |
| 0.86061 | 2.3474 | 0.11161 |
| 0.86667 | 2.3467 | 0.11073 |
| 0.87273 | 2.346 | 0.10987 |
| 0.87879 | 2.3454 | 0.10903 |
| 0.88485 | 2.3447 | 0.10819 |
| 0.89091 | 2.3441 | 0.10737 |
| 0.89697 | 2.3435 | 0.10657 |
| 0.90303 | 2.3429 | 0.10577 |
| 0.90909 | 2.3423 | 0.10499 |
| 0.91515 | 2.3417 | 0.10422 |
| 0.92121 | 2.3411 | 0.10347 |
| 0.92727 | 2.3406 | 0.10272 |
| 0.93333 | 2.34 | 0.10199 |
| 0.93939 | 2.3395 | 0.10126 |
| 0.94545 | 2.339 | 0.10055 |
| 0.95152 | 2.3385 | 0.099847 |
| 0.95758 | 2.338 | 0.099155 |
| 0.96364 | 2.3375 | 0.098473 |
| 0.9697 | 2.337 | 0.0978 |
| 0.97576 | 2.3365 | 0.097137 |
| 0.98182 | 2.3361 | 0.096483 |
| 0.98788 | 2.3356 | 0.095839 |
| 0.99394 | 2.3352 | 0.095203 |
| 1.0 | 2.3348 | 0.094576 |
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
- —
Crystalline BaTiO3. Clamped measurements.