Plasmonic Bowtie Nanoantenna: Gap Field Enhancement (2D)

Antenna Geometry

Wing (arm) length 100 nm

Gap width 8 nm

Material

Illumination

Drive wavelength 550 nm

Polarization angle 0°

Live Readouts

Resonant wavelength λ_res—

Gap field enhancement |E/E₀|—

Quality factor Q—

How it works

Each triangular "wing" of the bowtie is a metal nanostructure whose free electrons act as a driven, damped harmonic oscillator — a localized surface plasmon (LSP). Its resonance wavelength scales with the wing's length L (a nanoscale analogue of a half-wave dipole antenna, red-shifted by the metal's negative permittivity):

λ_res(L) = λ0 + k·L
Au: λ0 ≈ 120 nm, k ≈ 3.5   |   Ag: λ0 ≈ 90 nm, k ≈ 3.2

Driven at wavelength λ, the normalized response follows a Lorentzian in the fractional detuning Δ = (λ − λ_res)/λ_res, with damping ratio γ set by the metal's ohmic loss (silver is lower-loss than gold, so it resonates more sharply):

L(Δ) = γ / √(Δ² + γ²)          (peaks at 1 when λ = λ_res)
Q = 1/γ                          (Au ≈ 10, Ag ≈ 22)

The two sharp tips facing each other across the gap act like lightning rods: the same oscillating charge that spreads over a wide triangle base is funneled onto a tiny tip area, concentrating the electric field. That geometric "funneling" factor grows as the gap shrinks, and only the field component along the antenna's long axis couples in (Malus-law-style cos²θ for polarization angle θ):

gapFactor(g) = (10 nm / g)^0.7, clamped to [1, 12]
E_gap / E₀ = Q · L(Δ) · gapFactor(g) · cos²θ

Wing length — shifts λ_res; longer wings resonate at redder wavelengths, exactly like scaling a radio dipole.
Gap width — shrinking it raises the field concentration in the hot spot (visualized as the heatmap between the tips), the mechanism exploited in SERS and single-molecule biosensing. Drag the wings directly in the stage to change it.
Drive wavelength / Sweep — moves you through the Lorentzian; enhancement peaks sharply at λ_res.
Polarization angle — an antenna only couples to the field component along its own axis; at 90° the coupling vanishes.

This is a simplified oscillator model for teaching intuition, not a full electromagnetic (FDTD/BEM) solve — but the resonance-shift, damping and gap-concentration trends it reproduces match measured bowtie-nanoantenna behavior. The bottom panel plots this same enhancement formula continuously against gap width, with the current gap marked live.

Positive charge Negative charge Gap hot spot