Optical constants

Refractive index of PBDB-T:ITIC

Kerremans et al. 2020: n,k 0.37–1.6 µm

Data
tabulated n + tabulated k
Range
0.3733–1.605 µm
Points
119
Licence
CC0-1.0

Plot

Click the plot to set the calculator wavelength. Note: k data cover 377.1-1600 nm only; k = 0 elsewhere in the n range 373.3-1604.5 nm.

At one wavelength

Range 0.3733–1.605 µm
Refractive index n
1.52584
Extinction coefficient k
0.921544
Permittivity ε1
1.47894
Permittivity ε2
2.81226
Absorption coefficient α
197081 cm⁻¹
Penetration depth δ = λ/(2πk)
101.481 nm
Abbe number Vd
—
Chromatic dispersion dn/dλ
5.74454 µm⁻¹
Group index ng
-1.84965
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

# PBDB-T:ITIC: Kerremans et al. 2020: n,k 0.37–1.6 µm
pbdbt_itic = ls.fetch_refractiveindex("other", "PBDBT-ITIC", "Kerremans", ref="c5c2f188e848453def5970e347399d653df2ffc2")
print(pbdbt_itic.range_nm)  # (373.3, 1604.5) nm
eps = pbdbt_itic.eps([633])  # complex permittivity

Downloads the original record once (pinned to the imported snapshot) and caches it.

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

PBDB-T:ITIC (1:1) thin film.

Notes on the source data (kept exactly as published):
  • k < 0 at some wavelengths in the source data (gain, or a sign convention issue)
  • k data cover 377.1-1600 nm only; k = 0 elsewhere in the n range 373.3-1604.5 nm

References

R Kerremans, C. Kaiser, W. Li, N. Zarrabi, P. Meredith, A. Armin. The optical constants of solution-processed semiconductors—new challenges with perovskites and non-fullerene acceptors. Adv. Opt. Mater. 8, 2000319 (2020) (Data points extracted from Figure 4, PBDB-T:ITIC, Ellipsometry)
  • doi:10.1002/adom.202000319 The Optical Constants of Solution‐Processed Semiconductors—New Challenges with Perovskites and Non‐Fullerene Acceptors, Advanced Optical Materials (2020)

Cite

Robin Kerremans et al.. The Optical Constants of Solution‐Processed Semiconductors—New Challenges with Perovskites and Non‐Fullerene Acceptors. Advanced Optical Materials, 8, 2000319 (2020), doi:10.1002/adom.202000319; Data from the refractiveindex.info database (M. N. Polyanskiy, Sci. Data 11, 94 (2024), doi:10.1038/s41597-023-02898-2)

Data

Computed on 119 wavelengths, the same grid as the API and the library
PBDB-T:ITIC, Kerremans et al. 2020: n,k 0.37–1.6 µm: n and k versus wavelength
λ (µm)nk
0.37331.626270
0.39441.606330.2756626
0.41831.572150.2742776
0.43671.552220.2756295
0.45141.518040.2802151
0.4681.483860.290478
0.481.449680.3088047
0.49371.409810.3434245
0.50571.375630.3859091
0.52321.332910.4961898
0.53051.324370.544003
0.5481.347150.6767465
0.56911.418350.8281835
0.57931.478160.8910005
0.59121.546520.9341898
0.60781.614870.9869074
0.61791.671841.037798
0.62621.740191.107121
0.63081.780061.13495
0.63631.842721.147469
0.6391.899681.150734
0.64361.968041.143016
0.64822.01931.126869
0.6512.050631.109631
0.65472.099051.071873
0.66392.141770.9869033
0.67312.124680.9243569
0.6852.090510.9616144
0.69242.093351.037706
0.69792.156011.100266
0.70162.201581.136156
0.70522.264241.15365
0.7082.298421.16101
0.70982.343991.162945
0.71262.389561.156379
0.71442.452221.150765
0.71812.492091.136254
0.72092.520571.115966
0.72362.560441.073966
0.72552.606011.052546
0.73012.640190.97392
0.73652.691460.85226
0.74022.719940.72351
0.74942.754110.4324893
0.75672.762660.21881
0.76412.742720.07490852
0.76962.714240.01153556
0.77332.68576-0.01672712
0.77882.65158-0.02975978
0.78162.62025-0.03332286
0.78522.58323-0.03790396
0.78982.5519-0.04077478
0.79352.52057-0.04180435
0.80182.47785-0.04335284
0.80642.45222-0.04171541
0.81372.42373-0.03863446
0.81832.40095-0.03598832
0.82852.36677-0.02822121
0.8342.34684-0.02445168
0.84412.3212-0.018794
0.85512.29557-0.01421727
0.86522.26994-0.01257918
0.87542.2557-0.009335246
0.88552.23576-0.006159844
0.90022.21297-0.0006831818
0.90752.207280.002750976
0.92042.187340.002766707
0.93332.17310.00413
0.94432.164560.00278
0.95722.156010.0008990411
0.97012.144620.001564452
0.98852.127530.002877755
1.00322.116140.002901918
1.01242.110440.002916
1.02522.107590.002939273
1.03812.099050.002961676
1.04822.087660.002977681
1.05832.087660.002991951
1.07312.076270.00301
1.08782.076270.004972701
1.09882.067720.004988341
1.11172.064870.003835613
1.12272.062030.001202623
1.13472.056330.00376
1.15032.047780.003896859
1.16322.044940.003962683
1.17242.044940.005062195
1.18342.036390.003946437
1.19442.036390.003206885
1.20912.03070.003301273
1.21832.03070.004394121
1.23492.03070.00520811
1.24962.022150.003499344
1.26432.0250.001830846
1.27722.016460.003095174
1.29372.013610.003368912
1.30662.013610.003210937
1.31772.007910.001554609
1.33422.010760.003380606
1.34892.002220.00503954
1.36362.002220.003982903
1.37652.002220.003502109
1.39311.996520.00225878
1.40321.999370.0021725
1.41511.990820.003467317
1.42431.990820.002401463
1.43351.990820.002447246
1.45011.985130.005551144
1.46481.985130.005556707
1.47951.985130.003844695
1.49051.985130.004798485
1.50711.985130.005644015
1.51811.982280.005663269
1.52731.979430.005680645
1.54291.976580.005700816
1.55671.979430.005719592
1.56961.976580.005744727
1.58341.976580.005769818
1.60451.968040

Optical transmission calculator

Free-standing sample in vacuum, normal incidence
Method
Transmittance T
—
Reflectance R
—

Fresnel reflection calculator

Direction
Rp
—
Rs
—
R = (Rp+Rs)/2
—
Phase φp
—
Phase φs
—
Brewster angle θB
—
Critical angle θC
—