Ultrathin Absorbing Interference Coatings
This case study focuses on a problem that is directly relevant to thin-film design, display coatings, and structural color: a nanometre-scale absorbing film on an optically thick metallic reflector. The central result is counterintuitive but fully compatible with one-dimensional TMM: strong interference can survive even when the top film is highly absorbing, provided the film is sufficiently thin.
For Dreapex TMM, this is a valuable literature case because it links two result families that users often treat separately: spectral response and perceived color. The same stack can be evaluated through Reflection Spectrum for physics and through Reflection Color for application-facing interpretation.
Research Context
Conventional coating design often assumes that strong interference requires transparent or only weakly absorbing layers. The Kats paper is important because it demonstrates a different regime: a few to a few tens of nanometres of a highly absorbing film can still support usable interference when placed on a metallic substrate.
This is a direct TMM use case because the structure remains a layered stack and the primary observables are reflectance, absorptance, and color. The problem stays within the one-dimensional boundary of the solver while still capturing a visually rich engineering result.
Paper Information
- Paper: Nanometre optical coatings based on strong interference effects in highly absorbing media
- Authors: Mikhail A. Kats, Romain Blanchard, Patrice Genevet, and Federico Capasso et al.
- Journal: Nature Materials 12, 20-24 (2013)
- DOI: 10.1038/nmat3443
- Target phenomenon in the paper: thickness-dependent spectral selectivity and color change in an ultrathin absorbing film on a metallic substrate
The Nature Materials abstract states that the relevant thickness scale is only a few to tens of nanometres and that visible-light implementations can use absorbing material as thin as 5-20 nm, which is the correct order-of-magnitude target for this reproduction.
Mapping the Paper to a TMM Model
This case uses the canonical thin-absorber-on-metal geometry:
| Item | TMM model used in this case | Rationale |
|---|---|---|
| Incidence medium | Air | Standard reflection geometry |
| Top film | Ultrathin absorbing dielectric or semiconductor film | This is the active interference layer |
| Thickness range | A few nanometres to a few tens of nanometres | Matches the scale emphasized in the paper abstract |
| Back reflector | Optically thick metal layer | Suppresses transmission and makes reflection the main observable |
| Material model | main/Ge/nk/Aspnes.yml for the absorbing film and main/Au/nk/Johnson.yml for the back reflector | Uses explicit database entries that already cover the visible-band regime relevant to the first pass |
| Main variable | Top-film thickness | The paper's central design lever is thickness-controlled spectral selection |
For the Dreapex TMM workflow in this chapter, use the built-in database directly: Ge / Aspnes for the ultrathin absorbing layer and Au / Johnson for the metal reflector. This keeps the first pass anchored to a real absorbing semiconductor file and a real noble-metal file without introducing a custom imported dataset.
Reproduction Target and Acceptance Criteria
The reproduction target is not a single narrow spectral line. It is the systematic movement of spectral response and color with thickness.
This case is considered successful when:
- Small thickness changes produce clear changes in the reflection spectrum.
- The spectrum shift is monotonic or at least ordered across the chosen thickness sweep.
Reflection Colorchanges in a visually consistent sequence rather than randomly.- The stack remains reflection-dominated because the metal reflector is optically thick.
The following are not required in the first implementation:
- exact colorimetric agreement with the publication
- exact reproduction of the original film chemistry
- exact match of every local spectral shoulder
Reproduction Workflow in Dreapex TMM
The screenshots in this chapter are page-type references from the live app. They show which Dreapex TMM pages to use during the reproduction workflow. The exact published trend depends on the absorbing-film material model and thickness range you choose.
Use the following workflow:
- In
Structure, define an ultrathin absorbing top film above an optically thick metallic reflector. - Select
main/Ge/nk/Aspnes.ymlfor the top film andmain/Au/nk/Johnson.ymlfor the reflector. - Keep the metal layer thick enough that transmission is negligible over the target band.
- In
Optics, use a visible-light wavelength sweep. - Enable
Incident SpectrumandEnable Color Calculation. - Enable
Reflection SpectrumandReflection Color. - In
Sweep, use the top-film thickness as the single primary variable.



Representative Result Pages to Inspect
This case should always be interpreted through both the spectral and color views:
Reflection Spectrumtells you how the reflected energy distribution shifts with thickness.Reflection Colortells you how that spectral shift appears in a color space or summary table.


Visual Comparison with the Paper
The paper's central claim is that the absorbing film does not merely add loss; it reshapes the reflected spectrum in a thickness-sensitive way. Your TMM reproduction should therefore be judged by ordered spectral migration and corresponding color migration.
The visual comparison is successful when:
- the reflected spectral envelope changes materially when the top film thickness changes
- the thickness order produces a consistent progression instead of arbitrary spectral noise
- the color output shifts with the same ordering implied by the spectrum
- the response remains plausible for a reflective stack rather than behaving like a transmissive filter
If the color barely changes across the full sweep, the thickness range is likely too narrow, the film is too weakly absorbing, or the metal is not acting as an effective reflector.
Deviation Analysis
The most common deviation sources are:
- the specific Ge and Au database entries used for the first pass
- uncertainty in the original paper's exact deposited film stack
- metal thickness not yet fully in the optically opaque regime
- roughness, oxidation, or interfacial layers not represented in the 1D stack
- different incident spectrum or color-matching settings than the published comparison
Because the perceived color is sensitive to both material data and illumination assumptions, visible differences are expected unless those inputs are matched carefully.
Further Experiments
- Sweep the absorbing-film thickness more finely inside the
5-20 nmrange to locate the most sensitive region. - Compare
Reflection SpectrumandAbsorptanceto separate spectral shaping from simple loss increase. - Repeat the same thickness sweep under different incident-spectrum presets to test illumination sensitivity.
- Export the color table and compare
xyorHexvalues across thickness candidates for design screening.
Tamm Plasmon at a Metal-DBR Interface
Reconstruct the reflectance resonance reported by Kaliteevski et al. in Dreapex TMM, using a real front-end workflow and stating explicitly which parts of the paper are matched and which parts still remain outside the current model fit.
Data Import and Export
Material files, spectra, and result export