Photothermal-based atomic force microscopy infrared (AFM-IR) spectroscopy enables nanoscale chemical imaging and subsurface characterization, yet the fundamental mechanisms governing its probing depth remain only partially understood. Classical thermal diffusion model predicts a length scaling of f^-1/2 with modulation frequency, whereas recent experiments observed a much stronger confinement of probing depth in AFM-IR close to f^-3/2. To resolve this discrepancy, we develop a unified analytical model that quantitatively links absorbed optical energy to the detected cantilever oscillation amplitude in AFM-IR. The model integrates frequency-dependent subsurface heat deposition, thermoelastic expansion with strain attenuation, and resonance-enhanced cantilever dynamics. Our analysis reveals that the effective probing depth (dₑ₎₁₄) is not governed by thermal diffusion alone, but is strongly affected by optical and thermoelastic strain attenuation. These combined effects lead to an inverse frequency scaling (dₑ₎₁₄ f^-1), indicating that mechanical transduction processes play a dominant role in determining depth sensitivity. This framework provides a mechanistic basis for the experimentally observed strong confinement of probing depth and offers quantitative guidelines for tuning depth sensitivity through excitation frequency, pulse conditions, sample architecture, and tip–sample coupling.
Zhang et al. (2026) studied this question.