2018
DOI: 10.1016/j.ultras.2018.04.002
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Design of far-infrared acousto-optic tunable filter based on backward collinear interaction

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Cited by 11 publications
(5 citation statements)
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“…The relative contributions of the two effects, for each of the acoustic cavity resonances, are plotted in Fig.8. The MB contribution dominates at all frequencies, except near the Brillouin frequency of silicon, where the AO interaction becomes phase-matched ( k acoustic = 2 k opt ) [24,25] and the optomechanical coupling can be significantly enhanced. The even-odd mode coupling can be clearly discerned in the high frequency modes (¿ 2.5 GHz) in Fig.4(a) (green and red arrows) where the modes alternate between finite and zero modulation.…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…The relative contributions of the two effects, for each of the acoustic cavity resonances, are plotted in Fig.8. The MB contribution dominates at all frequencies, except near the Brillouin frequency of silicon, where the AO interaction becomes phase-matched ( k acoustic = 2 k opt ) [24,25] and the optomechanical coupling can be significantly enhanced. The even-odd mode coupling can be clearly discerned in the high frequency modes (¿ 2.5 GHz) in Fig.4(a) (green and red arrows) where the modes alternate between finite and zero modulation.…”
Section: Discussionmentioning
confidence: 99%
“…8. The MB contribution dominates at all frequencies, except near the Brillouin frequency of silicon, where the AO interaction becomes phase-matched ( k acoustic = 2 k opt ) [24,25] and the optomechanical coupling can be significantly enhanced. The even-odd mode coupling can be clearly discerned in the high frequency modes (¿ 2.5 GHz) in Fig.…”
Section: Discussionmentioning
confidence: 99%
“…For conventional acousto-optic spectral systems, the collimating scheme is the most common and structurally simple scheme, and the optical path diagram is shown in Figure 1B. The adopted scheme is to filter the light directly using a single AOTF, which is also the basis of other schemes [26,27]. The light entering the optical system from the object under test is collimated by L0, the mutually parallel light is filtered by the AOTF, and then be focused on the CCD by the focusing lens L1.…”
Section: Collimating Schemementioning
confidence: 99%
“…It is analytically shown that, with decreasing thickness of the first layer, the frequency range broadens, in which the phase of the reflected light does not change and the reflectance approaches 100% [19]. The PPAM properties can also be observed in acousto-optical cells [26] as well as in chiral thin structured films [27].…”
Section: Introductionmentioning
confidence: 98%