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Spatial Characterization Of Two-Photon States - GAP-Optique

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APPENDIX C<br />

Methods for OAM<br />

measurements<br />

A real world oam application will require a compact tool able to separate the<br />

different modes at the single photon level. A tool analogous to the beam splitter<br />

for polarization, or to a diffraction grating for frequency. Such a tool probably<br />

will be based on the two current methods to determine the oam of photons:<br />

holographic and interferometric methods.<br />

In a very simplistic way, an hologram is a record of the interference pattern<br />

of two beams. When the hologram is illuminated with one of the beams,<br />

the other beam can be reconstructed. Based on this principle, a computer<br />

generated hologram of the interference of a lg mode with a Gaussian beam,<br />

in conjunction with a single mode fiber can be used to detect that particular<br />

lg mode [7, 51]. Even though this method works at single photon level, it<br />

is restricted to a two-value response, reducing the effective dimensions of the<br />

oam to two, as shown in figure C.1.<br />

Reference [15] introduced an analyzer able to sort photons into even and<br />

odd oam modes, using a Mach-Zender interferometer. With a phase shift in<br />

one of the interferometer arms, the constructive and destructive interference<br />

were so that odd modes go to one of the outputs, and even modes to the other,<br />

as figure C.2 shows. By nesting several interferometers, and using holograms,<br />

the authors proved that was possible to separate up to 2 n modes with (2 n − 1)<br />

interferometers. This method works at single photon level, and can distinguish<br />

many different oam modes, but it relies on the simultaneous stabilization of<br />

different interferometers, which is challenging experimentally.<br />

71

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