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Francesco Marino

Publications and source records attributed to Francesco Marino.

5 recordsLinked to original sources

Excitable optical waves in semiconductor microcavities.

We demonstrate experimentally and theoretically the existence of excitable optical waves in semiconductor microcavities. Although similar to those observed in biological and chemical systems, these excitable optical waves are self-confined. This is due to a new dynamical scenario, where a stationary Turning pattern controls the propagation of waves in an excitable medium, thus bringing together the two paradigms of dynamical behavior (waves and patterns) in active media.

Models, Theoretical↗

Dynamical mechanism of anticipating synchronization in excitable systems.

We analyze the phenomenon of anticipating synchronization of two excitable systems with unidirectional delayed coupling which are subject to the same external forcing. We demonstrate for different paradigms of excitable system that, due to the coupling, the excitability threshold for the slave system is always lower than that for the master. As a consequence the two systems respond to a common external forcing with different response times. This allows us to explain in a simple way the mechanism behind the phenomenon of anticipating synchronization in excitable systems.

Journal Article↗

Thermo-optical "canard orbits" and excitable limit cycles.

We demonstrate experimentally and theoretically the existence of canard orbits and excitable quasiharmonic limit cycles in the thermo-optical dynamics of semiconductor optical amplifiers. We also observe the phase locking of the noise-induced spikes to the small-amplitude Hopf quasiharmonic oscillations, recently predicted by Makarov, Nekorkin, and Velarde [Phys. Rev. Lett. 86, 3431 (2001)]].

Biological Clocks↗

Can young adult patients with proteinuric IgA nephropathy perform physical exercise?

BACKGROUND: It is not known whether physical exercise increases daily proteinuria in patients with proteinuric nephropathies, thus accelerating progression of the renal lesion. This study evaluates the acute effects of physical exercise on proteinuria in young adults with immunoglobulin A (IgA) nephropathy. METHODS: Changes induced by intense physical exercise on quantitative and qualitative proteinuria were evaluated in basal conditions and after 10 days of ramipril therapy in 10 patients with IgA nephropathy, normal glomerular filtration rate (GFR), proteinuria between 0.8 and 1.49 g/24 h, and "glomerular" microhematuria before and after the end of a maximal treadmill Bruce test (B-test). The basal study also was performed in 10 age- and sex-matched healthy volunteers. RESULTS: At rest, GFR averaged 141 +/- 23 mL/min; it increased by 16.3% +/- 3.3% (P < 0.005) and 7.1% +/- 1.6% at 60 and 120 minutes after the B-test, respectively. At rest, GFR-corrected proteinuria averaged protein of 0.76 +/- 0.21 mg/min/100 mL GFR; it increased to 1.55 +/- 0.28 mg/min/100 mL GFR after 60 minutes (P < 0.001) and declined to 0.60 +/- 0.11 mg/min/100 mL GFR at 120 minutes after the end of the B-test. The pattern of urinary proteins remained unchanged, as did microhematuria. Daily proteinuria was not different from the basal value on the day of the B-test. After ramipril therapy, patients showed a reduction in GFR, but no change in daily GFR-corrected proteinuria, pattern of urinary proteins, or hematuria. CONCLUSION: The increase in proteinuria after exercise in our patients is significant and is not prevented by ramipril therapy, but lasts less than 120 minutes. Therefore, it cannot modify daily proteinuria. Thus, these data do not support the need to reduce acute physical activity in patients with nonnephrotic renal diseases.

Adult↗

Experimental evidence of stochastic resonance in an excitable optical system.

Experimental evidence of stochastic resonance in an excitable optical system is reported. We apply a sinusoidal forcing to the system and, for a finite external noise level, we find a frequency for which the excitable pulsing occurs periodically at the frequency imposed by the modulation. This resonant frequency matches the inverse of the average escape time of the stochastically driven system (i.e., without forcing). The same resonance is found by varying the noise level for fixed forcing frequencies. We discuss different indicators in order to describe quantitatively the degree of resonance.

Journal Article↗