Philip H. Jones, Onofrio M. Maragò & Giovanni Volpe
Fig. 5.1 — Comparison of optical forces calculated in various trapping regimes
Transverse trap stiffness produced by a 10 mW laser beam of wavelength λ0 = 632 nm focused by a 1.20 NA objective on a dielectric sphere of radius a (np = 1.50) in water (nm = 1.33). The solid line represents the exact electromagnetic calculation. The dipole approximation (dotted line) works for small spheres (a ≪ λ0). The geometrical optics approximation (dashed line) works for large spheres (a ≫ λ0).
Fig. 5.1 — Comparison of optical forces calculated in various trapping regimes