2010
DOI: 10.1109/lpt.2010.2052098
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Adiabatic Mode Conversion in Multimode Waveguides Using Computer-Generated Planar Holograms

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Cited by 22 publications
(14 citation statements)
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“…From Eqs. (16), (17), (22) and (23) the most general solution to Eqs. (1-9), from t = t i to t = t f , can be then readily calculated.…”
Section: Ctap In Rectangular Latticesmentioning
confidence: 99%
See 1 more Smart Citation
“…From Eqs. (16), (17), (22) and (23) the most general solution to Eqs. (1-9), from t = t i to t = t f , can be then readily calculated.…”
Section: Ctap In Rectangular Latticesmentioning
confidence: 99%
“…As a final note, we mention that the STIRAP scheme discussed so far for the rectangular lattice of Fig.1(a) can be implemented, for example, in an array of 3 × 3 optical waveguides with controlled separation distances, generalizing the optical set ups discussed in Refs. [15,16].…”
Section: Ctap In Rectangular Latticesmentioning
confidence: 99%
“…Assuming the CGPH only couples the nearest-neighboring modes, the evolution of mode amplitudes obey the coupled mode equations [3] j d dz…”
Section: Invariant-based Inverse Engineeringmentioning
confidence: 99%
“…The similarities also allow a straightforward adaptation of schemes developed for quantum system manipulation to the design of waveguide-based devices. We have previously proposed adiabatic mode splitting devices using computer-generated planar holograms (CGPHs) [3] in multimode waveguides based on fractional stimulated Raman adiabatic passage (f-STIRAP) [4] in a 5-level system. This scheme allows adiabatic mode conversion/splitting in multimode waveguides without strict restrictions on the coupling parameters, but the device length is long in order to satisfy the adiabatic criterion.…”
Section: Introductionmentioning
confidence: 99%
“…The similarities allow a straightforward adaptation of schemes developed for quantum system manipulation to the design of waveguide based devices. We have previously proposed adiabatic mode conversion devices using computer-generated planar holograms (CGPHs) [13] in multimode waveguides based on stimulated Raman adiabatic passage (STIRAP) [14] in a three-level system. Figure 1 shows a three-level system and the schematic of a corresponding CGPH loaded multimode waveguide, where multiplexed longperiod gratings with coupling coefficient variations along the propagation direction are used to mimic the delayed laser pulses in STIRAP.…”
mentioning
confidence: 99%