Amplifying properties of a synchronized generator

The amplifying properties of a synchronized generator are explained on the basis of an autoparametric model of the synchronization phenomenon.Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Fizika, No. 12, pp. 59–63, December, 1981.     

Experimental investigation of autoparametric phenomena in the harmonic synchronization of thomson oscillators

The amplifier properties of a synchronized oscillator and the reason for the large spread in the time taken for the synchronous mode to become established can be explained by an autoparametric mechanism of the phenomenon of synchronization for weak external emf's.Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Fizika, No. 10, pp. 59–63, October, 1976.     

Synchronization in systems with bimodal dynamics

Considering a prototypic model of a bimodal oscillator we investigate the synchronization of the internal time scales for a system with interacting fast and slow oscillatory modes. Particular emphasis is given to the transition between mode-locked and mode-unlocked chaos. It is shown that this transition involves a homoclinic bifurcation in which the synchronized chaotic attractor loses its band structure. For two coupled bimodal oscillators we illustrate the presence of separate synchronization regions for the fast and the slow modes. The dependence of these regions on the mismatch and coupling parameters is studied.     

Synchronization of a self-excited oscillator with a biharmonic external signal

The effect of a weak external signal on the change in the limits of the harmonic synchronization band is studied. The regions of synchronization at combination frequencies are found.Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Fizika, No. 5, pp. 58–63, May, 1988.     

Comparison of the influences of nodal dynamics on network synchronized regions

A new piecewise linear unified chaotic (PLUC) system is firstly presented, and then its fundamental dynamical behaviors are analyzed. This modified chaotic system, as well as the unified chaotic (UC) one, is taken as network nodal oscillators for investigating the difference of influences of nodal dynamics on the bifurcation of network synchronized regions. It is found that beyond the greatly similar bifurcation modes between PLUC and UC networks, the synchronized regions in PLUC networks are far narrower at almost each parameter a than those in UC networks for most of inner coupling matrices, indicating the PLUC node makes the network more difficult to synchronization. Our numerical investigations show that this phenomenon is closely related with nodal dynamical properties, such as the boundary of attractors, the largest Lyapunov exponent and Lyapunov dimension.     

All-optical synchronization of a 40 GHz self-pulsating distributed Bragg reflector laser to return-to-zero 10, 20 and 40 Gbit/s data streams

This paper presents experimental investigations of the all-optical synchronization of a distributed Bragg reflector (DBR) laser self-pulsating at 40 GHz on various injected bit-rate signals. Even though there is no modulation applied to this laser, it exhibits a modulation of its output emission, measured at 39.7 GHz with a linewidth of 30 MHz. Such performance is exploited in all-optical clock recovery for a return-to-zero data stream at 40 Gbit/s. The SP-DBR laser wavelength and the injected signal wavelength are 10 nm apart. All-optical synchronization is demonstrated at 40 Gbit/s with a linewidth of less than 20 MHz for injected signals at 10 and 20 Gbit/s, respectively. Thus the SP-DBR laser proves to be very versatile and can be synchronized on various bit-rate data signals.     

Systematic experimental study of instabilities in the sealed CO2 laser

A systematic pressure-current experimental study of the wave instability regions in glow-discharge of different CO₂ laser mixtures has been accomplished. The forward ionization wave F^– has been found to be the main instability. At low currents (< 30 mA) and higher pressures (> 550 Pa) the laser discharge becomes stable. The highest output power at a given mixture ratio was achieved in these quiet regions. The normalized electric field dependences of wavenumber, phase and group velocities of the F^– wave are presented.     

Sum-frequency spectroscopy of physisorbed and chemisorbed molecules at liquid and solid surfaces using band-width-limited picosecond pulses

We studied the vibrational Sum-Frequency (SF) spectra of long chain fatty alcohols and amines physisorbed at liquid/air interfaces and of OctadecylTrichlorSilan (OTS) chemisorbed on glass/air interfaces in situ, i. e., in normal laboratory environment. The intense, band-width-limited IR pulses generated by our laser system are tunable from 2600 to 4000 cm^–1 with a constant pulse duration of 3 ps and a band width of 5 cm^–1 (FWHM) over the entire tuning range, thus covering the CH-, NH-, and OH-stretching regions.Using suitable polarization geometries, information on the molecular orientation is obtained from the amplitudes of the symmetric and degenerate methyl-stretching modes. Opposite phase of adjacent vibrational modes can lead to destructive interference in the SF signal, as analyzed theoretically. This interference effect is observed experimentally for the first time, due to the superior spectral resolution and signal-to-noise ratio of our spectra.     

Generation of cyclotron radiation by light holes in germanium

The properties of the light hole cyclotron resonance laser are studied in detail. The emission spectrum and the tuning characteristics are analysed. Two regions of continuously tunable stimulated emission between 30 to 50 cm^–1 and 70 to 90 cm^–1 are found. Besides the time behaviour of the emission the spectral gain is measured for the first time with the help of a secondp-Ge laser, A gain value of 0.2 cm^–1 is found, which is significantly larger than the value found for the light to heavy hole laser. An application of the tunable laser is demonstrated by measuring the central cell splitting the photoconductivity signal of shallow donors inn-GaAs.     

Temperature dependence of the raman spectra of carbon nanotubes with 1064 nm excitation

In this report, the near infrared 1064 nm line of an Nd:YAG laser, which has strong thermal effect, was used as the excitation. A temperature dependence of the Raman spectra of carbon nanotubes was observed at different temperatures by varying the incident laser power. The results show that the relative Raman intensities to the tangential stretching mode (G mode) of the higher-order Raman modes within 2500–3500 cm⁻¹ increase with increasing excitation laser power at the sample and the changes in the relative Raman intensities are linear in the excitation laser power. This has not been reported elsewhere. Thorough analysis shows that this is a temperature dependence of double-phonon Raman scattering and maybe provide important information for the studying of CNTs and double-phonon Raman scattering.     

Densities and velocity distributions of atomic hydrogen and carbon,measured by laser-induced fluorescence with frequency tripling into the vacuum UV

By focussing a commercial dye laser pumped with a XeCl excimer laser into phase matched Xe-A or Kr-A gas mixtures, radiation at the third-harmonic frequency has been generated in the wavelength regions: 1142–1165, 1178–1186, 1203–1224, and 1268–1290 Å. VUV powers up to about 200 W have been detected by a calibrated Au-photodiode. The vacuum uv radiation has been used for the fluorescence excitation of H and C atoms produced by thermal dissociation or by a gas discharge. Absolute densities have been derived by a comparison of fluorescence intensities with intensities from Rayleigh scattering in argon. As a further application, velocity distributions of C atoms sputtered from a graphite target by 1.5 keV argon ions have been measured. These data are in good agreement with a Thompson distribution corresponding to a surface energy of 8.2 eV.     

Anticipation in the synchronization of chaotic semiconductor lasers with optical feedback

The synchronization of chaotic semiconductor lasers with optical feedback is studied numerically in a one-way coupling configuration, in which a small amount of the intensity of one laser (master laser) is injected coherently into the other (slave laser). A regime of anticipated synchronization is found, in which the intensity of the slave laser is synchronized to the future chaotic intensity of the master laser. Anticipation is robust to small noise and parameter mismatches, but in this case the synchronization is not complete. It is also shown that anticipated synchronization occurs in coupled time-delay systems, when the coupling has a delay that is less than the delay of the systems.     

Fields of apertured polychromatic laser beams with Gaussian and Hermite–Gaussian transverse modes

Starting from the Huygens–Fresnel diffraction integral, the field expressions of apertured polychromatic laser beams with Gaussian and Hermite–Gaussian transverse modes are derived. Influence of the bandwidth on the intensity distributions of the laser beams is analyzed. It is found that when the bandwidth increases, the amplitudes and numbers of the intensity spikes decrease and beam uniformity is improved in the near field and the width of transverse intensity distribution of the apertured beams decreases in the far field. Thus, the smoothing and narrowing effects can be achieved by increasing the bandwidth. Also, these effects are found in the laser beams with Hermite–Gaussian transverse modes as the bandwidth increases.     

Instantaneous gain and excited state absorption in two carbocyanine dyes

The single-pass gain of 4 · 10^–5 mole/liter solutions of 3,3-diethylthiatricarbocyanine iodide (DTTC) in methanol and 3,3-diethylthiadicarbocyanine iodide (DTDC) in acetone, optically pumped by a giant pulse ruby laser, were measured as a function of pump power, wavelength, and time. The transverse pumping laser pulse was synchronized with a probing pulse from a dye laser. Both low-signal and saturated gain measurements were made in the wavelength range 7860–8066 Å for DTTC and 7059–7412 Å for DTDC dye. The pumping pulse widths at half-power were 15 ± 5 nsec, and the pumping power density was varied over a range of 0–7 MW/cm². Using a steady-state theory, lifetime and cross sections for excited states were determined.This research is supported by the National Research Council of Canada. A summary of the present work was reported at the First All-Union Conference on Complex Organic Dye Lasers, Minsk, USSR, October 22–24, 1975.Published in Zhurnal Prikladnoi Spektroskopii, Vol. 26, No. 3, pp. 487–496, March, 1977.     

Study of the beat spectrum between modes of a gas laser with confocal resonator

The beat spectrum between modes of a gas laser having a resonator with a plane-and-sphere mirror system was studied. Intense beats were detected in the 0–1.5 Mc range. It is shown that the presence of low-frequency beats can be associated with the nonideality of the resonator. The intensity of the beats was found to depend on their spectral composition and on the degree of beam limiting. This effect is related to the presence of antiphase oscillation zones in the laser beam for azimuthal modes and to the variation of the interference pattern with time when the beam is limited in the focus of the objective.     

Modeling “preattention” and “attention” information processing by synchronization of neural activity

Oscillatory neural-network preattention and attention models are examined. A two-layer network of Wilson-Cowan oscillators is used to show that two-frequency oscillations can appear in response to a compound stimulus. It is shown that these oscillations can be synchronized at the low frequency, which can be interpreted as feature binding. Partial synchronization is studied in a model of a network of phased oscillators with a central element. Formulas are given for approximation of the average frequency of the central oscillator for small and large networks. The results describe the effect of a distracting stimulus on attention focus.Institute of Mathematical Problems of Biology, Russian Academy of Sciences. Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Radiofizika, Vol. 37, No. 8, pp. 933–944, August, 1994.     

Investigation of passively synchronized dual-wavelength Q-switched lasers based on V:YAG saturable absorber

In this paper the results of a theoretical and experimental investigation of synchronized passive Q-switching of two Nd:YVO₄-based solid-state lasers operating at two different wavelengths, is described. A V:YAG saturable absorbing material was used as a passive Q-switch performing the synchronization of the two laser fields. This material provides Q-switching operation at both 1064 and 1342 nm wavelengths simultaneously, saturating the same energy level. By adjusting the pump power of both lasers, it was possible to optimize the overlap of the two pulse trains and to switch between different states of synchronization. A theoretical model based on rate equations, which has been developed in order to investigate optical performance of the laser system, is in a good agreement with the experimental results. The principle of synchronized Q-switching can lead to new, pulsed all-solid-state light sources at new wavelengths based on sum-frequency mixing processes.     

Bimodal Nanoparticle Size Distributions Produced by Laser Ablation of Microparticles in Aerosols

Silver nanoparticles were produced by laser ablation of a continuously flowing aerosol of microparticles in nitrogen at varying laser fluences. Transmission electron micrographs were analyzed to determine the effect of laser fluence on the nanoparticle size distribution. These distributions exhibited bimodality with a large number of particles in a mode at small sizes (3–6-nm) and a second, less populated mode at larger sizes (11–16-nm). Both modes shifted to larger sizes with increasing laser fluence, with the small size mode shifting by 35% and the larger size mode by 25% over a fluence range of 0.3–4.2-J/cm². Size histograms for each mode were found to be well represented by log-normal distributions. The distribution of mass displayed a striking shift from the large to the small size mode with increasing laser fluence. These results are discussed in terms of a model of nanoparticle formation from two distinct laser–solid interactions. Initially, laser vaporization of material from the surface leads to condensation of nanoparticles in the ambient gas. Material evaporation occurs until the plasma breakdown threshold of the microparticles is reached, generating a shock wave that propagates through the remaining material. Rapid condensation of the vapor in the low-pressure region occurs behind the traveling shock wave. Measurement of particle size distributions versus gas pressure in the ablation region, as well as, versus microparticle feedstock size confirmed the assignment of the larger size mode to surface-vaporization and the smaller size mode to shock-formed nanoparticles.     

Efficient generation of FIR radiation by optical pumping of D2 18O

In this paper we show that D₂ ¹⁸O vapour, optically pumped with a continuously tunable high pressure CO₂ laser, is an excellent source for far infrared radiation. Both high photon conversion coefficients and broad Raman gain regions were found for a large number of new laser transitions spread over the frequency range from 25 cm^–1 to 240 cm^–1. We demonstrate that these Raman gain regions can be used to generate far infrared laser pulses with high intensity and durations of about 100 ps.     

Are the sources of natural fluctuations correlated in different laser modes?

The intensity fluctuations in multimode lasers with slow relaxing laser media are theoretically investigated. The power spectra corresponding to different correlation conditions between the noise sources inserted into individual modes are calculated in the framework of a two-level homogeneously broadened laser model with spatial hole burning. The comparison of calculated spectra with the experimental data allows us conclude that the noise sources are correlated.Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Radiofizika, Vol. 39, No. 6, pp. 771–782, June, 1996.