Optical constants
Refractive index of C12H14O4 (Diethyl phthalate, DEP)
Querry 1987: Near-infrared; n,k 0.81–2.5 µm
- Data
- tabulated nk
- Range
- 0.8095–2.499 µm
- Points
- 170
- Licence
- CC0-1.0
Plot
Click the plot to set the calculator wavelength.
At one wavelength
- Refractive index n
- 1.49695
- Extinction coefficient k
- 5.95000e-06
- Permittivity ε1
- 2.24086
- Permittivity ε2
- 1.78137e-05
- Absorption coefficient α
- 0.526549 cm⁻¹
- Penetration depth δ = λ/(2πk)
- 3.79832e+07 nm
- Abbe number Vd
- —
- Chromatic dispersion dn/dλ
- -0.1 µm⁻¹
- Group index ng
- 1.63895
- Group velocity dispersion
- — fs²/mm
- Dispersion parameter D
- — ps/(nm·km)
- Photon energy
- 0.873128 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
# C12H14O4 (Diethyl phthalate, DEP): Querry 1987: Near-infrared; n,k 0.81–2.5 µm
c12h14o4 = ls.fetch_refractiveindex("organic", "diethyl_phthalate", "Querry-NIR", ref="c5c2f188e848453def5970e347399d653df2ffc2")
print(c12h14o4.range_nm) # (809.5, 2499.5) nm
eps = c12h14o4.eps([1420]) # 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_9070b48c2a61/lightsmith"
c12h14o4 = ls.Tabulated.model_validate(json.load(urllib.request.urlopen(url)))
print(c12h14o4.source) # citation and provenance travel with the data
Any dataset here, as the library's Tabulated material (diethyl-phthalate/querry-1987-nir).
# ... load c12h14o4 as above, then:
sim = ls.Simulation(
particles=[ls.Particle(shape=ls.Sphere(radius_nm=50), material=c12h14o4)],
medium_index=1.0,
wavelengths=ls.WavelengthRange(start_nm=810, 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
Cite
M. R. Querry. Optical constants of minerals and other materials from the millimeter to the ultraviolet. Contractor Report CRDEC-CR-88009 (1987); Data from the refractiveindex.info database (M. N. Polyanskiy, Sci. Data 11, 94 (2024), doi:10.1038/s41597-023-02898-2)
Data
170 rows as published| λ (µm) | n | k |
|---|---|---|
| 0.8095 | 1.499 | 0.0 |
| 0.8195 | 1.499 | 0.0 |
| 0.8295 | 1.499 | 0.0 |
| 0.8395 | 1.499 | 0.0 |
| 0.8495 | 1.499 | 0.0 |
| 0.8595 | 1.499 | 0.0 |
| 0.8695 | 1.499 | 0.0 |
| 0.8795 | 1.498 | 0.0 |
| 0.8895 | 1.498 | 0.0 |
| 0.8995 | 1.498 | 1e-06 |
| 0.9095 | 1.498 | 1e-06 |
| 0.9195 | 1.498 | 0.0 |
| 0.9295 | 1.498 | 0.0 |
| 0.9395 | 1.498 | 0.0 |
| 0.9495 | 1.498 | 0.0 |
| 0.9595 | 1.498 | 0.0 |
| 0.9695 | 1.498 | 0.0 |
| 0.9795 | 1.498 | 0.0 |
| 0.9895 | 1.498 | 0.0 |
| 0.9995 | 1.498 | 1e-06 |
| 1.0095 | 1.498 | 1e-06 |
| 1.0195 | 1.498 | 1e-06 |
| 1.0295 | 1.498 | 1e-06 |
| 1.0395 | 1.498 | 1e-06 |
| 1.0495 | 1.498 | 0.0 |
| 1.0595 | 1.498 | 0.0 |
| 1.0695 | 1.498 | 0.0 |
| 1.0795 | 1.498 | 0.0 |
| 1.0895 | 1.498 | 1e-06 |
| 1.0995 | 1.498 | 1e-06 |
| 1.1095 | 1.498 | 1e-06 |
| 1.1195 | 1.498 | 3e-06 |
| 1.1295 | 1.498 | 6e-06 |
| 1.1395 | 1.498 | 7e-06 |
| 1.1495 | 1.497 | 4e-06 |
| 1.1595 | 1.497 | 5e-06 |
| 1.1695 | 1.497 | 7e-06 |
| 1.1795 | 1.497 | 1e-05 |
| 1.1895 | 1.497 | 6e-06 |
| 1.1995 | 1.497 | 3e-06 |
| 1.2095 | 1.497 | 2e-06 |
| 1.2195 | 1.497 | 1e-06 |
| 1.2295 | 1.497 | 1e-06 |
| 1.2395 | 1.497 | 1e-06 |
| 1.2495 | 1.497 | 1e-06 |
| 1.2595 | 1.497 | 1e-06 |
| 1.2695 | 1.497 | 1e-06 |
| 1.2795 | 1.497 | 1e-06 |
| 1.2895 | 1.497 | 1e-06 |
| 1.2995 | 1.497 | 1e-06 |
| 1.3095 | 1.497 | 1e-06 |
| 1.3195 | 1.497 | 1e-06 |
| 1.3295 | 1.497 | 1e-06 |
| 1.3395 | 1.497 | 2e-06 |
| 1.3495 | 1.497 | 5e-06 |
| 1.3595 | 1.497 | 7e-06 |
| 1.3695 | 1.497 | 9e-06 |
| 1.3795 | 1.497 | 1e-05 |
| 1.3895 | 1.497 | 1e-05 |
| 1.3995 | 1.497 | 9e-06 |
| 1.4095 | 1.497 | 7e-06 |
| 1.4195 | 1.497 | 6e-06 |
| 1.4295 | 1.496 | 5e-06 |
| 1.4395 | 1.496 | 4e-06 |
| 1.4495 | 1.496 | 4e-06 |
| 1.4595 | 1.496 | 4e-06 |
| 1.4695 | 1.496 | 3e-06 |
| 1.4795 | 1.496 | 3e-06 |
| 1.4895 | 1.496 | 2e-06 |
| 1.4995 | 1.496 | 2e-06 |
| 1.5095 | 1.496 | 2e-06 |
| 1.5195 | 1.496 | 2e-06 |
| 1.5295 | 1.496 | 1e-06 |
| 1.5395 | 1.496 | 1e-06 |
| 1.5495 | 1.496 | 1e-06 |
| 1.5595 | 1.496 | 2e-06 |
| 1.5695 | 1.496 | 2e-06 |
| 1.5795 | 1.496 | 2e-06 |
| 1.5895 | 1.496 | 3e-06 |
| 1.5995 | 1.496 | 5e-06 |
| 1.6095 | 1.496 | 6e-06 |
| 1.6195 | 1.496 | 1.1e-05 |
| 1.6295 | 1.496 | 1.6e-05 |
| 1.6395 | 1.496 | 1.8e-05 |
| 1.6495 | 1.496 | 4e-05 |
| 1.6595 | 1.496 | 9.8e-05 |
| 1.6695 | 1.496 | 0.000112 |
| 1.6795 | 1.496 | 0.000137 |
| 1.6895 | 1.496 | 0.000102 |
| 1.6995 | 1.496 | 5.2e-05 |
| 1.7095 | 1.495 | 5.6e-05 |
| 1.7195 | 1.495 | 7.8e-05 |
| 1.7295 | 1.495 | 7.3e-05 |
| 1.7395 | 1.495 | 4.4e-05 |
| 1.7495 | 1.495 | 3.8e-05 |
| 1.7595 | 1.495 | 4.4e-05 |
| 1.7695 | 1.495 | 2.9e-05 |
| 1.7795 | 1.495 | 2.4e-05 |
| 1.7895 | 1.495 | 2.7e-05 |
| 1.7995 | 1.495 | 2.7e-05 |
| 1.8095 | 1.495 | 2.4e-05 |
| 1.8195 | 1.495 | 2.2e-05 |
| 1.8295 | 1.495 | 2.1e-05 |
| 1.8395 | 1.495 | 1.9e-05 |
| 1.8495 | 1.495 | 1.6e-05 |
| 1.8595 | 1.495 | 1.6e-05 |
| 1.8695 | 1.495 | 1.6e-05 |
| 1.8795 | 1.495 | 1.7e-05 |
| 1.8895 | 1.495 | 2e-05 |
| 1.8995 | 1.495 | 2.7e-05 |
| 1.9095 | 1.495 | 2.7e-05 |
| 1.9195 | 1.495 | 2.1e-05 |
| 1.9295 | 1.495 | 2.2e-05 |
| 1.9395 | 1.494 | 2.9e-05 |
| 1.9495 | 1.494 | 3.2e-05 |
| 1.9595 | 1.494 | 2.6e-05 |
| 1.9695 | 1.494 | 1.9e-05 |
| 1.9795 | 1.494 | 1.8e-05 |
| 1.9895 | 1.494 | 2e-05 |
| 1.9995 | 1.494 | 1.9e-05 |
| 2.0095 | 1.494 | 1.9e-05 |
| 2.0195 | 1.494 | 2e-05 |
| 2.0295 | 1.494 | 2.2e-05 |
| 2.0395 | 1.494 | 2.4e-05 |
| 2.0495 | 1.494 | 2.5e-05 |
| 2.0595 | 1.494 | 2.8e-05 |
| 2.0695 | 1.494 | 3.5e-05 |
| 2.0795 | 1.494 | 4.7e-05 |
| 2.0895 | 1.494 | 4.6e-05 |
| 2.0995 | 1.494 | 4.7e-05 |
| 2.1095 | 1.494 | 6.2e-05 |
| 2.1195 | 1.494 | 8.6e-05 |
| 2.1295 | 1.493 | 0.000108 |
| 2.1395 | 1.493 | 0.000197 |
| 2.1495 | 1.493 | 0.000128 |
| 2.1595 | 1.493 | 0.000152 |
| 2.1695 | 1.493 | 0.000119 |
| 2.1795 | 1.493 | 8.6e-05 |
| 2.1895 | 1.493 | 0.000109 |
| 2.1995 | 1.493 | 9.8e-05 |
| 2.2095 | 1.493 | 0.000119 |
| 2.2195 | 1.493 | 0.000119 |
| 2.2295 | 1.493 | 0.00017 |
| 2.2395 | 1.493 | 0.00027 |
| 2.2495 | 1.493 | 0.000508 |
| 2.2595 | 1.493 | 0.000799 |
| 2.2695 | 1.493 | 0.000515 |
| 2.2795 | 1.493 | 0.000394 |
| 2.2895 | 1.493 | 0.000507 |
| 2.2995 | 1.493 | 0.000691 |
| 2.3095 | 1.493 | 0.000605 |
| 2.3195 | 1.493 | 0.000419 |
| 2.3295 | 1.493 | 0.000441 |
| 2.3395 | 1.493 | 0.000473 |
| 2.3495 | 1.493 | 0.000465 |
| 2.3595 | 1.493 | 0.000389 |
| 2.3695 | 1.493 | 0.000339 |
| 2.3795 | 1.492 | 0.000351 |
| 2.3895 | 1.492 | 0.000428 |
| 2.3995 | 1.492 | 0.000487 |
| 2.4095 | 1.492 | 0.000628 |
| 2.4195 | 1.492 | 0.000559 |
| 2.4295 | 1.492 | 0.000575 |
| 2.4395 | 1.492 | 0.000639 |
| 2.4495 | 1.492 | 0.000585 |
| 2.4595 | 1.492 | 0.0005 |
| 2.4695 | 1.492 | 0.000437 |
| 2.4795 | 1.492 | 0.000393 |
| 2.4895 | 1.492 | 0.000324 |
| 2.4995 | 1.492 | 0.00026 |
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
- —