Expand this Topic clickable element to expand a topic
Skip to content
Optica Publishing Group

Free-space information transfer using light beams carrying orbital angular momentum

Open Access Open Access


We demonstrate the transfer of information encoded as orbital angular momentum (OAM) states of a light beam. The transmitter and receiver units are based on spatial light modulators, which prepare or measure a laser beam in one of eight pure OAM states. We show that the information encoded in this way is resistant to eavesdropping in the sense that any attempt to sample the beam away from its axis will be subject to an angular restriction and a lateral offset, both of which result in inherent uncertainty in the measurement. This gives an experimental insight into the effects of aperturing and misalignment of the beam on the OAMmeasurement and demonstrates the uncertainty relationship for OAM.

©2004 Optical Society of America

Full Article  |  PDF Article
More Like This
Transfer of orbital angular momentum from a super-continuum, white-light beam

Amanda J Wright, John M Girkin, Graham M Gibson, Jonathan Leach, and Miles J Padgett
Opt. Express 16(13) 9495-9500 (2008)

Rapid generation of light beams carrying orbital angular momentum

Mohammad Mirhosseini, Omar S. Magaña-Loaiza, Changchen Chen, Brandon Rodenburg, Mehul Malik, and Robert W. Boyd
Opt. Express 21(25) 30196-30203 (2013)

850-nm hybrid fiber/free-space optical communications using orbital angular momentum modes

Antonio Jurado-Navas, Anna Tatarczak, Xiaofeng Lu, Juan José Vegas Olmos, José María Garrido-Balsells, and Idelfonso Tafur Monroy
Opt. Express 23(26) 33721-33732 (2015)

Cited By

Optica participates in Crossref's Cited-By Linking service. Citing articles from Optica Publishing Group journals and other participating publishers are listed here.

Alert me when this article is cited.

Figures (5)

Fig. 1.
Fig. 1. Optical configuration of the free-space optics (FSO) demonstration system. Shown here is the case of a beam with l=8.
Fig. 2.
Fig. 2. Some examples of phase-hologram designs (top) and schematic representation of the corresponding far-field diffraction patterns under plane wave illumination (bottom). The phase-hologram patterns are represented in grey-scale. (a) Horizontally shifted l=1 beam. (b) Setting the phase at each point in the hologram pattern for the horizontally shifted l=1 beam to either 0 or π (whichever is closest) gives three horizontally separated beams with l=-1, 0 and +1. (c) Similarly, we can obtain three vertically separated beams with l=-3, 0 and +3. (d) The sum of the two phase patterns that create the horizontally and vertically separated beams gives a 3×3 array of beams with l=-4, -3, …, +3, +4.
Fig. 3.
Fig. 3. A subset of results from transmitting a data set using OAM. We have used a data transmission set corresponding to the azimuthal indices -16,-12,-8,-4,0,+4,+8,+12,+16. We have defined a matrix of detectors by measuring the intensity at specific points on the CCD image.
Fig. 4.
Fig. 4. Spread – or uncertainty – in the measured values P(l) for various apertures inserted into the path of an l=1 beam. The beam immediately after the aperture is shown in the left column. The measured spread in l-values (dark bars) compares well with the power spectrum of the aperture function P(ϕ) (light bars).
Fig. 5.
Fig. 5. Spread in the values of l for various angular misalignments of an l=1 beam. Θ is the angular misalignment as a fraction of the beam divergence. The measured results (dark bars) are compared to those predicted by a decomposition of the detected beams in terms of cylindrical harmonics (light bars).
Select as filters

Select Topics Cancel
© Copyright 2024 | Optica Publishing Group. All Rights Reserved