2017
DOI: 10.1038/ncomms16097
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Synthetic-lattice enabled all-optical devices based on orbital angular momentum of light

Abstract: All-optical photonic devices are crucial for many important photonic technologies and applications, ranging from optical communication to quantum information processing. Conventional design of all-optical devices is based on photon propagation and interference in real space, which may rely on large numbers of optical elements, and the requirement of precise control makes this approach challenging. Here we propose an unconventional route for engineering all-optical devices using the photon’s internal degrees of… Show more

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Cited by 66 publications
(41 citation statements)
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“…Inside such degenerate cavity, one can then introduce an auxiliary cavity, which incorporates spatial light modulators, in order to couple a small portion of the amplitude of a beam with an orbital angular moment l to a beam with an orbital angular moment l − 1 and l + 1. The system then is described by a tight-binding model [10,[60][61][62][63]]…”
Section: (B)mentioning
confidence: 99%
“…Inside such degenerate cavity, one can then introduce an auxiliary cavity, which incorporates spatial light modulators, in order to couple a small portion of the amplitude of a beam with an orbital angular moment l to a beam with an orbital angular moment l − 1 and l + 1. The system then is described by a tight-binding model [10,[60][61][62][63]]…”
Section: (B)mentioning
confidence: 99%
“…To address this issue and before discussing further the effect of lattice size and also couplings on the OAM beams here we propose an approach to build a very large lattice in the synthetic dimension. Creating lattices in the synthetic dimension with bidirectional coupling has been studied before where one uses a modulation defined via a pure real function to create an artificial dimension, such as frequency for instance, and make a synthetic lattice [27,28]. In contrast to what has been proposed so far here we are interested in a large lattice with artificial sites that its artificial sites are coupled in a unidirectional manner as needed for the observation of the continues family of solutions at the EP [29].…”
Section: Fig 1: (Main Panel)mentioning
confidence: 99%
“…Typically the FSR of the main cavity is Ω F ∼ 2π × 1GHz, and the tunneling strength, given by J s = Ω F |rs| 2 2π(1+|ts| 2 ) with r s (t s ) the reflectivity (transmissivity) of the corresponding beam splitters [13][14][15]30], can be up to tens of MHz (e.g., J 0 ∼ 2π × 20MHz and J 0 J 1 ∼ 2π × 4MHz). The pump period T ∼ 20/J 1 leads to a switching time of the order of µs.…”
Section: Experimental Considerationmentioning
confidence: 99%