2019
DOI: 10.1364/josaa.36.001064
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Vortex avalanche in the perturbed singular beams

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Cited by 23 publications
(12 citation statements)
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“…This makes the dips in the OAM spectrum more distinct. The complex amplitude (12) corresponds to the OAM in the form For large parameters Ω >>20, the OAM is doubled ℓ z ¼ 2M in range of the initial topological charges M. As was shown in [47,48], a perturbation δp causes a local distortion of the forked grating defect for the large values parameter p shown in Figure 3(a).…”
Section: Degenerate Case and Vortex Avalanchementioning
confidence: 79%
See 1 more Smart Citation
“…This makes the dips in the OAM spectrum more distinct. The complex amplitude (12) corresponds to the OAM in the form For large parameters Ω >>20, the OAM is doubled ℓ z ¼ 2M in range of the initial topological charges M. As was shown in [47,48], a perturbation δp causes a local distortion of the forked grating defect for the large values parameter p shown in Figure 3(a).…”
Section: Degenerate Case and Vortex Avalanchementioning
confidence: 79%
“…This effect is accompanied by a sharp restructuring of the vortex spectrum. For small perturbations of the singular beam, additional vortex modes arise only near the initial value of the topological charge m ¼ M (see [47]). However, in general case of the hologram perturbation, vortex modes with opposite signs of topological charges appear.…”
Section: Nondegenerate Casementioning
confidence: 99%
“…As we have shown in Ref. [19][20][21], the analysis of the vortex spectrum (dependence of the vortex mode intensity ( ) 2 , m n C α on the topological charge n ) enable us recovering the initial beam shape and finding its OAM. In our studies, we select two vortex beams with topological charges 5 m = and 15 m = that most clearly reflect properties of the sector perturbation.…”
mentioning
confidence: 94%
“…One of the possible approaches to solving this problem has been recently proposed and implemented in the articles [40][41][42][43]. The key idea of this technique is to use the intensity moments of higher-orders (see e.g.…”
Section: Introductionmentioning
confidence: 99%
“…[40] considered specifics of employing the intensity moments technique for measuring the vortex spectrum (squared amplitudes and mode phases) and using them to calculating the total OAM of the combined beam containing LG modes with different topological charges m of the same signs ( 0 m or 0 m ) but zero radial number 0 n . This technique allowed analyzing structure of the vortex avalanche [41] caused by small local perturbations of the holographic grating. The use of the astigmatic transformation of the combined beam by means of a cylindrical lens [42] has expanded this technique to the beams with different signs of topological charges ( 0 m and 0 m ), but a zero radial number.…”
Section: Introductionmentioning
confidence: 99%