A gold nanoparticle helix — the kind assembled on DNA-origami templates in real chiroptical experiments — is modeled here as N plasmonic spheres, each a driven Lorentzian dipole oscillator with polarizability
α(λ) = α₀ / [(1 − x²) − iΓx], x = λ₀/λ
resonant near λ₀ ≈ 530 nm (a small Au nanosphere's localized surface plasmon resonance, Γ its damping). Illuminated along the helix axis by left- or right-circularly-polarized light, particle i sees
E_inc,i = E₀(x̂ ± iŷ) e^(ikz_i), k = 2π/λ
The particles also couple to each other through their near-field dipole radiation — this is a discrete-dipole approximation (DDA), solved self-consistently by relaxation:
p_i = α(λ)[E_inc,i + Σ_j≠i κ₀(a/R_ij)³ (3n̂(n̂·p_j) − p_j) e^(ikR_ij)]
σ_ext(λ) ∝ Σ_i Im[E_inc,i* · p_i] (optical theorem)
CD(λ) = A_LCP(λ) − A_RCP(λ), g = 2·CD / (A_LCP + A_RCP)
- Handedness flips the sign of the azimuthal step between particles, mirroring the whole structure — flip it and the CD signal flips sign, exactly as a real enantiomeric nanohelix does.
- N / pitch set the geometric arrangement — how tightly the near-field–coupled dipoles wind around the propagation axis, which controls how strongly the structure discriminates LCP from RCP.
- λ sweeps the driving wavelength across the plasmon resonance; CD peaks near where the coupling-induced splitting is largest, not exactly at λ₀.
- Sphere glow along the helix shows the relative magnitude of each particle's induced dipole |p_i| for whichever polarization is being animated — the chiral near-field coupling makes this pattern asymmetric between LCP and RCP.
This near-field-coupled-dipole picture is the standard simplified mechanism used to explain plasmon-induced circular dichroism in chiral metal nanostructures (helices, gammadions, DNA-templated nanoparticle assemblies): geometric chirality plus retarded dipole–dipole coupling, not molecular optical activity.