Fig. 1: Concept of a dynamic 3D rotation by time-varying 3D SAM transfer. | Nature Communications

Fig. 1: Concept of a dynamic 3D rotation by time-varying 3D SAM transfer.

From: Time-varying 3D optical torque via a single beam

Fig. 1

a Transverse spin (T-spin) by two-wave interference (classic). The superposition of the left-hand and right-hand circularly polarized beams (LCP and RCP) leads to a T-spin (yellow arrow), which can be transferred to particles to drive transverse rotation (red arrow). b Time-varying 3D SAM control via a single-beam configuration (our work). The incident beam is 45° linearly polarized (LP), and its x-polarized component is shaped with asymptotic spiral phases to manipulate various SAM vectors (yellow arrows). The spiral phase masks labeled t1, t2, and t3 correspond to a sequence of phase masks at times t1, t2, and t3, resulting in SAM1, SAM2, and SAM3, respectively. c Dynamic 3D optical spanner via time-varying vectorial transfer of the SAM to microparticles in an optical trap. Experimental images of a spinning cubic calcite particle demonstrate controlled rotations around an arbitrary axis in 3D space. The rotation axes are defined by the corresponding SAM1, SAM2, and SAM3 in (b).

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