Abstract
We use a Laguerre-Gaussian laser mode within an optical tweezers arrangement to demonstrate the transfer of the orbital angular momentum of a laser mode to a trapped particle. The particle is optically confined in three dimensions and can be made to rotate; thus the apparatus is an optical spanner. We show that the spin angular momentum of +/- (h) over bar per photon associated with circularly polarized light can add to, or subtract from, the orbital angular momentum to give a total angular momentum. The observed cancellation of the spin and orbital angular momentum shows that, as predicted, a Laguerre-Gaussian mode with an azimuthal mode index l = 1 has a well-defined orbital angular momentum corresponding to (h) over bar per photon. (C) 1997 Optical Society of America
| Original language | English |
|---|---|
| Pages (from-to) | 52-54 |
| Number of pages | 3 |
| Journal | Optics Letters |
| Volume | 22 |
| Publication status | Published - 1 Jan 1997 |
Keywords
- LASER-BEAMS
- PHASE SINGULARITIES
- PARTICLES
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