2011
DOI: 10.1063/1.3552202
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Interference-free superposition of nonzero order light modes: Functionalized optical landscapes

Abstract: In this paper, we utilize the incoherent superposition of nonzero order light modes. We show that this approach brings an additional degree of freedom to the generation of optical fields and notably the formation of superpositions that are otherwise unattainable through the use of refractive or diffractive optical elements and coherent or incoherent light sources. We employ this technique in two exemplary cases: first to create a field with tunable orbital angular momentum whose spatial intensity distribution … Show more

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Cited by 10 publications
(6 citation statements)
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“…2 θ A(θ)e iϕ x (θ) B(θ)e iϕ y (θ) [17,[43][44][45][46][47][48][49][50][51], deformable mirrors (DMs) [51], q-plate cells [52][53][54][55] and metasurfaces [56], and spiral phase plates (SPPs) [22]. Those optical elements can change the phase distribution of a mode, where the SLM and DM are programmable and can control the phase dynamically.…”
Section: Methods For Generation Of Tunable Oammentioning
confidence: 99%
See 1 more Smart Citation
“…2 θ A(θ)e iϕ x (θ) B(θ)e iϕ y (θ) [17,[43][44][45][46][47][48][49][50][51], deformable mirrors (DMs) [51], q-plate cells [52][53][54][55] and metasurfaces [56], and spiral phase plates (SPPs) [22]. Those optical elements can change the phase distribution of a mode, where the SLM and DM are programmable and can control the phase dynamically.…”
Section: Methods For Generation Of Tunable Oammentioning
confidence: 99%
“…The first kind of generation method is shown in Figure 6, which obtains tunable OAM modes by changing the phase information imposed on the SLMs, DMs or q-plate cells. When a Gaussian beam with linear polarization is launched to a programmable phase element (SLM or DM), the topological charge can be tuned by electrically changing the phase information loaded on them, which can obtain the modes on the orbital PS, as shown the first row in Figure 6 [17,[43][44][45][46]52]. The second row of Figure 6b shows 3 sections as subsystems to control respectively three degrees of freedom in the optical field, e.g., the phase, amplitude and retardation between the x and y components [47,48].…”
Section: Methods For Generation Of Tunable Oammentioning
confidence: 99%
“…optical vortex beams). The experimental verification of the transfer of angular momentum upon a particle has been demonstrated by rotation of an absorbing particle in the dark center of the vortex beam [36,37] or orbiting of microparticles around the beam axis in the high-intensity ring of the vortex beam [19,[38][39][40][41][42][43][44][45][46][47][48][49][50][51][52]. Even though in these cases the sizes of such particles were comparable to the laser beam wavelength, no quantitative comparison between the theory and the experiment has been performed.…”
Section: Introductionmentioning
confidence: 99%
“…Both technologies were developed in parallel in the branch of optical manipulation, but only recently, they were combined into more powerful tandem system that immediately manifested itself as an extraordinary optical tool allowing fast and complex beam-shaping. 17,18 We now show how to utilize this assembly to enhance the speed of the fibre-based fluorescent imaging by two orders of magnitude.…”
Section: +++4+++ ++I+t++mentioning
confidence: 99%