2010
DOI: 10.1063/1.3475415
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Ultrafast all-optical modulator for 1.5 μm controlled by Ti:Al2O3 laser

Abstract: The concept of ultrafast light modulator for wavelength ∼1.5 μm controlled by fundamental harmonic of a Ti:Al2O3 laser has been demonstrated. The possibility of realization of this concept was experimentally confirmed. We have demonstrated strong spectrally wide nonlinear response in multilayer heterostructures based on GaAs/(AlGa)xOy with the relaxation time of 1–3 ps in the spectral range where both materials have negligible absorption.

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Cited by 11 publications
(4 citation statements)
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“…As an additional advantage, MIM resonators can be easily engineered to work in the NIR-MIR range, being this the spectral region of interest of this paper. The spectral modulation performances of a device can be evaluated in terms of the differential transmissivity , where T ( t ) is the transmittance at a time t after the application of the modulation stimulus that, in our case, is a variation of the chemical potential, and T ( t 0 ) is the reference transmissivity at the starting point. , It is worth noticing that analogous figures of merit can be considered, associated to the other scattering parameters (i.e., differential reflectivity and absorbance), but for our purposes, detecting transmissivity is very convenient since it allows one to minimize the insertion loss and maximize the extinction ratio. Therefore, by considering a time-dependent modulation of the applied chemical potential, we can redefine the differential transmissivity as a function of the chemical potential rather than time as , where μ c 0 is the starting chemical potential and μ ci is the chemical potential at the i th instant.…”
Section: Resultsmentioning
confidence: 99%
“…As an additional advantage, MIM resonators can be easily engineered to work in the NIR-MIR range, being this the spectral region of interest of this paper. The spectral modulation performances of a device can be evaluated in terms of the differential transmissivity , where T ( t ) is the transmittance at a time t after the application of the modulation stimulus that, in our case, is a variation of the chemical potential, and T ( t 0 ) is the reference transmissivity at the starting point. , It is worth noticing that analogous figures of merit can be considered, associated to the other scattering parameters (i.e., differential reflectivity and absorbance), but for our purposes, detecting transmissivity is very convenient since it allows one to minimize the insertion loss and maximize the extinction ratio. Therefore, by considering a time-dependent modulation of the applied chemical potential, we can redefine the differential transmissivity as a function of the chemical potential rather than time as , where μ c 0 is the starting chemical potential and μ ci is the chemical potential at the i th instant.…”
Section: Resultsmentioning
confidence: 99%
“…This resonance is highly sensitive to structural parameters such as size and shape, as well as to the refractive index changes of the surrounding environment [14,15]. Because of its unique optical properties, fano resonance can be applied to light modulators, all-optical switches, sensors and other fields, which is why it has obtained a lot of attentions [16,17]. Multiple Fano resonances are caused by the collective behaviors of the total plasmonic systems, so it is difficult to be obtained and controled independently [18].…”
Section: Introductionmentioning
confidence: 99%
“…Generally, the effect of the switching in photonic crystals is usually based on the bandgap shift effect. Such all‐optical modulators and switchers utilize Kerr nonlinear response of solid materials, especially semiconductors, such as GaAs, zinc chalcogenides, InGaAsP, and doped metal oxides . The dynamics of charge carriers in the semiconductors provide picosecond response times of such switching systems.…”
Section: Introductionmentioning
confidence: 99%