Transverse orbital angular momentum of amplitude perturbed fields

We measure the change in transverse orbital angular momentum (tOAM) per photon, Δ⟨<i>L</i> _<i>y</i> ⟩, applied to an optical pulse by a pure amplitude perturbation. The results are in excellent agreement with calculations and simulations of the spatiotemporal torque based on our tOAM theory [Phys. Rev. Lett. <b>127</b>, 193901 (2021)]. The crucial factor in determining Δ⟨<i>L</i> _<i>y</i> ⟩ is the spatiotemporal distribution of tOAM density in the pulse. We show that even Gaussian pulses with zero total tOAM can have net tOAM induced by an amplitude perturbation stationary in the lab frame. As a prelude to the paper, we review and clarify several recent theoretical approaches to tOAM and reemphasize several fundamental principles needed for the correct analysis of experiments and simulations.