![Fig. 10.4 — Photonic force microscope in a rotationally symmetric potential](https://i0.wp.com/opticaltweezers.org/wp-content/uploads/2015/11/Fig10_4.png?fit=660%2C441)
(a)–(c) Photonic torque microscope with a rotationally symmetric harmonic potential, i.e., κx = κy or, equivalently, κ = 0, for various values of Ω. The shaded areas show the probability distribution function of the probe particle position in the corresponding force field (arrows). When Ω = 0, the probe movement can be separated along two orthogonal directions. When the (absolute) value of increases, the force field lines bend and the probe movements along the x– and y-directions are not independent any more. (d)-(f ) Corresponding autocorrelation functions Cx(τ) (black solid line) and cross-correlation functions Cxy(τ)(grey solid line) [Eqs. (10.6) and (10.7)]. Note that Cy(τ) = Cx(τ) and Cyx(τ) = Cxy(−τ).
Fig. 10.4 — Photonic force microscope in a rotationally symmetric potential