Optical constants
Refractive index of PtSe2 (Platinum diselenide)
Tharrault et al. 2025: 1L film; n,k 0.416–0.939 µm
- Data
- tabulated nk
- Range
- 0.416–0.9393 µm
- Points
- 84
- State
- crystalline
- Licence
- CC0-1.0
Plot
Click the plot to set the calculator wavelength.
At one wavelength
- Refractive index n
- 7.98829
- Extinction coefficient k
- 2.36346
- Permittivity ε1
- 58.2269
- Permittivity ε2
- 37.76
- Absorption coefficient α
- 505447 cm⁻¹
- Penetration depth δ = λ/(2πk)
- 39.5689 nm
- Abbe number Vd
- —
- Chromatic dispersion dn/dλ
- 18.982 µm⁻¹
- Group index ng
- -3.16556
- 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
# PtSe2 (Platinum diselenide): Tharrault et al. 2025: 1L film; n,k 0.416–0.939 µm
ptse2 = ls.fetch_refractiveindex("main", "PtSe2", "Tharrault-1L", ref="c5c2f188e848453def5970e347399d653df2ffc2")
print(ptse2.range_nm) # (416.05, 939.27) nm
eps = ptse2.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_0a61b270e862/lightsmith"
ptse2 = ls.Tabulated.model_validate(json.load(urllib.request.urlopen(url)))
print(ptse2.source) # citation and provenance travel with the data
Any dataset here, as the library's Tabulated material (ptse2/tharrault-2025-1l).
# ... load ptse2 as above, then:
sim = ls.Simulation(
particles=[ls.Particle(shape=ls.Sphere(radius_nm=50), material=ptse2)],
medium_index=1.0,
wavelengths=ls.WavelengthRange(start_nm=417, stop_nm=939, 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:10.1103/physrevlett.134.066901 Optical Absorption in Indirect Semiconductor to Semimetal <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:mrow> <mml:msub> <mml:mrow> <mml:mi>PtSe</mml:mi> </mml:mrow> <mml:mrow> <mml:mn>2</mml:mn> </mml:mrow> </mml:msub> </mml:mrow> </mml:math> Arises from Direct Transitions, Physical Review Letters (2025)
Cite
Marin Tharrault et al.. Optical Absorption in Indirect Semiconductor to Semimetal <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:mrow> <mml:msub> <mml:mrow> <mml:mi>PtSe</mml:mi> </mml:mrow> <mml:mrow> <mml:mn>2</mml:mn> </mml:mrow> </mml:msub> </mml:mrow> </mml:math> Arises from Direct Transitions. Physical Review Letters, 134, 066901 (2025), doi:10.1103/physrevlett.134.066901; Data from the refractiveindex.info database (M. N. Polyanskiy, Sci. Data 11, 94 (2024), doi:10.1038/s41597-023-02898-2)
Data
84 rows as published| λ (µm) | n | k |
|---|---|---|
| 0.41605 | 6.83934 | 1.27762 |
| 0.41887 | 6.81986 | 1.29184 |
| 0.42171 | 6.79046 | 1.33146 |
| 0.4246 | 6.74693 | 1.38556 |
| 0.42753 | 6.68915 | 1.46401 |
| 0.4305 | 6.70452 | 1.48582 |
| 0.43351 | 6.7711 | 1.46152 |
| 0.43656 | 6.73889 | 1.50715 |
| 0.43966 | 6.71938 | 1.54777 |
| 0.4428 | 6.75774 | 1.5602 |
| 0.44599 | 6.79381 | 1.57026 |
| 0.44922 | 6.81591 | 1.59399 |
| 0.4525 | 6.83636 | 1.61838 |
| 0.45582 | 6.87488 | 1.62632 |
| 0.4592 | 6.89874 | 1.64101 |
| 0.46263 | 6.90922 | 1.6685 |
| 0.46611 | 6.93884 | 1.67911 |
| 0.46964 | 6.96511 | 1.68335 |
| 0.47322 | 7.00643 | 1.67882 |
| 0.47686 | 7.0326 | 1.68438 |
| 0.48056 | 7.06206 | 1.69354 |
| 0.48431 | 7.09044 | 1.69248 |
| 0.48813 | 7.11477 | 1.69997 |
| 0.492 | 7.13021 | 1.71406 |
| 0.49594 | 7.12634 | 1.74609 |
| 0.49994 | 7.12874 | 1.77271 |
| 0.504 | 7.15432 | 1.79942 |
| 0.50813 | 7.18444 | 1.82973 |
| 0.51233 | 7.20401 | 1.88201 |
| 0.5166 | 7.23551 | 1.92731 |
| 0.52094 | 7.28491 | 1.96269 |
| 0.52536 | 7.32655 | 2.01282 |
| 0.52985 | 7.38013 | 2.06346 |
| 0.53441 | 7.41259 | 2.12838 |
| 0.53906 | 7.43869 | 2.1925 |
| 0.54379 | 7.48751 | 2.24717 |
| 0.5486 | 7.53138 | 2.30955 |
| 0.5535 | 7.60363 | 2.33642 |
| 0.55849 | 7.63474 | 2.38667 |
| 0.56356 | 7.69708 | 2.40372 |
| 0.56873 | 7.74649 | 2.42519 |
| 0.574 | 7.82064 | 2.41757 |
| 0.57937 | 7.89958 | 2.38946 |
| 0.58483 | 7.93571 | 2.39527 |
| 0.5904 | 8.04144 | 2.3313 |
| 0.59608 | 8.13924 | 2.27858 |
| 0.60187 | 7.77726 | 2.25443 |
| 0.60777 | 7.89043 | 2.16576 |
| 0.61378 | 7.87121 | 2.16091 |
| 0.61992 | 7.95944 | 2.0368 |
| 0.62618 | 8.02137 | 1.9209 |
| 0.63257 | 8.09906 | 1.77442 |
| 0.63909 | 8.10485 | 1.66963 |
| 0.64575 | 8.19898 | 1.4784 |
| 0.65255 | 8.19852 | 1.35246 |
| 0.65949 | 8.06343 | 1.27362 |
| 0.66658 | 7.78243 | 1.19493 |
| 0.67383 | 7.82113 | 1.03082 |
| 0.68123 | 7.82038 | 0.89694 |
| 0.6888 | 7.77998 | 0.79489 |
| 0.69654 | 7.78598 | 0.6738 |
| 0.70446 | 7.76771 | 0.59504 |
| 0.71255 | 7.74186 | 0.52447 |
| 0.72084 | 7.7103 | 0.45484 |
| 0.72932 | 7.61078 | 0.42554 |
| 0.738 | 7.46558 | 0.44099 |
| 0.74689 | 7.45753 | 0.37287 |
| 0.756 | 7.40147 | 0.32194 |
| 0.76533 | 7.28548 | 0.31799 |
| 0.7749 | 7.22732 | 0.28574 |
| 0.78471 | 7.12559 | 0.28146 |
| 0.79477 | 7.00201 | 0.27629 |
| 0.80509 | 6.79792 | 0.27996 |
| 0.81569 | 6.68826 | 0.25804 |
| 0.82656 | 6.66258 | 0.20848 |
| 0.83773 | 6.58331 | 0.16639 |
| 0.84921 | 6.47195 | 0.18406 |
| 0.861 | 6.57131 | 0.18993 |
| 0.87313 | 6.53715 | 0.1711 |
| 0.8856 | 6.5499 | 0.11772 |
| 0.89844 | 5.45829 | 0.18954 |
| 0.91165 | 5.41622 | 0.1912 |
| 0.92526 | 5.51727 | 0.15831 |
| 0.93927 | 5.4397 | 0.13471 |
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
- —
1L CVT-grown exfoliated crystal. The optical indexes are computed from the 2D surface conductivity using σ2D·Z0 = −2πi·(t/λ)·(εr−1), where Z0 is the impedance of free space, i the imaginary unit, t the equivalent layered stack thickness and λ the free space wavelength. We use t = NL t0 with t0 = 5.1 Å the single layer thickness. The measurement method accuratly determines Im{εr} = 2nk, but only Re{εr} = n2 - k2 as long as the optical absorption is non-zero.