HomeMaterials ScienceCarbon Nanotube Interconnect: Ballistic vs Diffusive Resistance

Carbon Nanotube Interconnect: Ballistic vs Diffusive Resistance

Dial the length of a carbon-nanotube on-chip interconnect against its electron mean free path and watch resistance transition from a flat quantum contact plateau (ballistic) to linear Ohmic growth (diffusive), per the Landauer formula.

Materials Science3DAdvanced60 FPS📱 Mobile-adapted
nanoelectronics ↗ Open standalone

This simulator models a bundle of metallic single-wall carbon nanotubes acting as an on-chip interconnect, using the real Landauer-Büttiker transport formula. Dial the interconnect length against the electron mean free path and watch resistance sit on a flat quantum-contact plateau while transport stays ballistic, then climb linearly once scattering dominates and the wire turns diffusive — with electrons rendered flowing through the tube bundle, flashing red at each scattering event so the ballistic-to-diffusive crossover is visible, not just numeric.

⚙ Under the hood

Dial the length of a carbon-nanotube on-chip interconnect against its electron mean free path and watch resistance transition from a flat quantum contact plateau (ballistic) to linear Ohmic growth (diffusive), per the Landauer formula.

nanoelectronicscarbon nanotubeballistic transportquantum resistanceinterconnectLandauer formula

3D · Three.js / WebGL renderer · 60 FPS target · runs fully client-side, no install

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