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AFM and STM: Tip-Surface Interaction

The two workhorses of nanoscale imaging. A sharp tip scans an atomically corrugated surface. In atomic force microscopy the tip feels the Lennard-Jones interaction V(d)=4ε[(σ/d)12(σ/d)6]V(d)=4\varepsilon[(\sigma/d)^{12}-(\sigma/d)^6]: strongly repulsive when it touches, weakly attractive further out, zero force at d=21/6σd=2^{1/6}\sigma. In scanning tunnelling microscopy the tip draws a current that decays exponentially with the gap, IVe2κdI\propto V\,e^{-2\kappa d} with κ=2mϕ/\kappa=\sqrt{2m\phi}/\hbar; for a metallic work function (ϕ5\phi\sim5 eV) that is roughly a factor of ten in current per angstrom of gap, which is why STM resolves single atoms. Pick AFM (force curve and scan), STM constant-height (atomic-contrast current map) or STM constant-current (the topograph that reproduces the surface). The tip sweeps across the lattice and the bottom panel traces the signal. Everything is closed form (gate-tested).

Figure 1. A scanning probe over an atomically corrugated surface (top), the interaction law (Lennard-Jones force for AFM, or the exponential tunnelling decay for STM, middle), and the scan signal versus tip position (bottom). Method: closed-form Lennard-Jones potential/force and the STM tunnelling law I ~ V exp(-2 kappa d) (gate-tested sim.js), Canvas2D; the live readouts are the gap, kappa, the per-angstrom current factor, and the instantaneous signal.
mode
gap / setpoint5.00
work fn phi (eV)5.00
gap d0 kappa0 per A0 signal0

WHAT TO TRY

  • Vary each control and watch the rail readouts respond.
  • Compare the diagnostic plot against the live scene.