One-click electromagnetism at the nanoscale

Aluminum nanoparticle plasmon calculator

Questions & answers

Where is the plasmon resonance of aluminum nanoparticles?

In the ultraviolet. Aluminum's free electrons are dense, so small spheres resonate in the deep UV (below 200 nm in water). Larger particles red-shift strongly: about 212 nm at 30 nm, 252 nm at 50 nm, 332 nm at 80 nm and 394 nm at 100 nm, reaching the visible above about 120 nm (table above).

Why use aluminum for plasmonics?

It is the only common metal with a strong plasmon in the UV, it is cheap and CMOS-compatible, and its few-nanometre native oxide makes it stable. It suits UV spectroscopy, UV-SERS, photocatalysis and full-colour structural printing.

How does the native oxide change the spectrum?

Aluminum always carries 2–4 nm of Al2O3 (refractive index about 1.65–1.77). It red-shifts the resonance by several nanometres and slightly damps it. Add a shell of that thickness with a custom refractive index in the calculator to include it.

Why do aluminum particles absorb near 800 nm?

Bulk aluminum has an interband transition at about 1.5 eV (around 800 nm). It shows up as a weak, broad absorption band in the spectra of larger particles, independent of the plasmon.

Do aluminum nanoparticles scatter or absorb?

Above about 30 nm mostly scatter: 70 % of the extinction at 30 nm and 85–90 % from 50 nm up (table above). Their low absorption makes them good UV scatterers and poor heaters.

Can I compute aluminum nanospheres, core–shell nanoparticles, arrays, near fields, heating or substrates?

Yes: aluminum nanospheres and core–shell nanoparticles (add a shell) are available in every calculator, from spectra to optical properties: near-field enhancement maps, dimers and hot spots, nanoparticle arrays and lattice resonances, particles on a substrate, emitters and the Purcell factor, nanorods and laser heating.

The UV plasmon of aluminum nanospheres: extinction, absorption and scattering for any size, in any medium, with or without the native oxide, in one click, from exact Mie theory.

Aluminum nanoparticle size vs plasmon peak

Aluminum spheres in water, from exact Mie theory with this site's solver. The calculator above covers any size, medium or oxide shell.

DiameterPlasmon peak (dipole)Molar extinction coefficientScattering share
5 nmbelow 200 nm (deep UV)6.85 × 105 M−1 cm−1< 1 %
10 nmbelow 200 nm (deep UV)5.72 × 106 M−1 cm−12 %
20 nmbelow 200 nm (deep UV)5.68 × 107 M−1 cm−113 %
30 nm212 nm2.05 × 1010 M−1 cm−170 %
40 nm231 nm2.83 × 1010 M−1 cm−180 %
50 nm252 nm3.59 × 1010 M−1 cm−185 %
60 nm277 nm4.39 × 1010 M−1 cm−188 %
80 nm332 nm6.21 × 1010 M−1 cm−190 %
100 nm394 nm8.40 × 1010 M−1 cm−191 %
150 nm561 nm1.56 × 1011 M−1 cm−190 %
200 nm752 nm2.56 × 1011 M−1 cm−186 %

Aluminum optical constants: Rakić (1995); water: Hale & Querry (1973), from 200 nm. Plasmon peak: the dipole (longest-wavelength) extinction maximum; for small particles it lies below the 200 nm edge of the water data. Molar extinction coefficient at the peak (at 400 nm when the peak lies deeper in the UV). Clean aluminum without its native oxide (see the questions below).

Related