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Variation of **frequency** shift due to the amplitude and the rotation rate.
... Conditions for zero **frequency** shift and zero pressure difference. Broken lines indicate linear fitting lines through the origin.
... **Oscillation**... **Frequency** shift

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(a) The SNR vs noise intensity D for fs=30,15, and 100 Hz, respectively. (b) The mean synaptic input Isyn(t) vs time for fs=30 Hz and D=0.15 and 6, respectively. (c) The SNR for various **frequencies** for the cases of D=0.5 and 5, respectively, in the case of I0i=0.8 and I1=0.11, and Jij∈[−4,20]. (d) The SNR vs signal **frequency** for D=0.5 and 5, respectively, for the case of I0i∈[0,1] and I1=0.072.
... Intrinsic **oscillations**... The 40 Hz **oscillation**... The **frequency** sensitivity... The **frequency** fi and the corresponding height H of the main peak in PSD of Isyn(t) vs (a) A for the case of I0i∈[0,3.5]; (b) M in the case of Jij∈[−5,10].
... I0i∈[0,2] and Jij∈[−1,10]. (a) The spatiotemporal firing pattern is plotted by recording the firing time tni defined by Xi(tni)>0 and Xi(tni−)**frequency** fi and the corresponding height H of the main peak in PSD of Isyn(t) for different coupling strength.

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In all plots the decay rates κ/g=0.1, γr/g=4.35×10-2, and cavity factor Q=1400. The quantum dot excitonic Bohr **frequency** is assumed to be in resonance with the cavity field **frequency**, i.e., ωqd=ωc. The amplitude of the external laser field to the cavity decay rate ratio is fixed to I/κ=631. The coherence ρ01≡ρ(0,1) dynamics is plotted for: (a) Δωcl=0.4g; (b) Δωcl=g; (c) Δωcl=100g; (d) Δωcl=1000g. The cavity photons mean number is plotted in (e) and (f). We have used a logarithmic scale for the time axis and the values: (i) Δωcl=g; (ii) Δωcl=1000g, for the solid and dotted curves, respectively.
... Rabi **oscillations**

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Illustration of a linear ion trap including an axial magnetic field gradient. The static field makes individual ions distinguishable in **frequency** space by Zeeman-shifting their internal energy levels (solid horizontal lines represent **qubit** states). In addition, it mediates the coupling between internal and external degrees of freedom when a driving field is applied (dashed horizontal lines stand for vibrational energy levels of the ion string, see text).
... Rabi **oscillations** on the optical E2 transition S1/2-D5/2 in Ba + . A fit of the data (solid line) yields a Rabi **frequency** of 71.4 × 2πkHz and a transversal relaxation time of 100 μs (determined by the coherence time of the ir light used to drive the E2 resonance).
... Illustration of the coupled system ‘**qubit** ⊗ harmonic **oscillator**’ in a trap with magnetic field gradient. Internal **qubit** transitions lead to a displacement dz of the ion from its initial equilibrium position and consequently to the excitation of vibrational motion. In the formal description the usual Lamb–Dicke parameter is replaced by a new effective one (see text).
... (a) Relevant energy levels and transitions in 138Ba + . (b) Schematic drawing of major experimental elements. OPO: Optical parametric **oscillator**; YAG: Nd:YAG laser; LD: laser diode; DSP: Digital signal processing system allows for real time control of experimental parameters; AOM: Acousto-optic modulators used as optical switches and for tuning of laser light; PM: Photo multiplier tube, serves for detection of resonance fluorescence. All lasers are **frequency** and intensity stabilized (not shown).
... Schematic drawing of the resonances of **qubits** j and j + 1 with some accompanying sideband resonances. The angular **frequency** vN corresponds to the Nth axial vibrational mode, and the **frequency** separation between carrier resonances is denoted by δω.

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Nonlinear **oscillator**... He’s **frequency** formulation

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Spontaneously occurring fast ‘ripple’ **oscillations** (400–500Hz) in the neocortex of the rat during high-voltage spindles. (A) Averaged high-voltage spindles and associated unit firing histograms from layers IV–VI. (B) Wide-band (a and a′; 1Hz–5kHz), filtered field (b and b′; 200–800Hz), and filtered unit (c and c′; 0.5–5kHz) traces from layers IV and V, respectively. (C) Averaged fast waves and corresponding unit histograms. The field ripples are filtered (200–800Hz) derivatives of the wide-band signals recorded from 16 sites. Note the sudden phase-reversal of the **oscillating** waves (arrows) but locking of unit discharges (dashed lines). These phase reversed dipoles likely reflect synchronous discharge of layer 5 neurons in the vicinity of the recording electrode.
... Self-organized burst of activity in the CA3 region of the hippocampus produces a sharp wave sink in the apical dendrites of CA1 pyramidal neurons and also discharge interneurons. The interactions between the discharging pyramidal cells and interneurons give rise to a short-lived fast **oscillation** (‘ripple’; 140–200Hz), which can be detected as a field potential in the somatic layer. The strong CA1 population burst brings about strongly synchronized activity in the target populations of parahippocampal structures as well. These parahippocampal ripples are slower and less synchronous, compared to CA1 ripples.

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Comparison of the **oscillation** in Fig. 17 and the basic **frequency** component L in Fig. 23. The replacement of the feedback channel loops by open areas for vortical flow made the feedback paths slightly shorter (and therefore the **frequency** higher).... Measured **oscillation** **frequency** with different feedback tube lengths of the **oscillator** shown in Fig. 7, plotted as a function of the supplied flow rate. Surprisingly, the **frequency** is neither proportional to the flow rate (as is usual in the constant Strouhal-number **oscillators**, e.g., Tesař et al., 2006) – nor constant (as in the **oscillators** with resonator channel (Tesař et al., 2013)).
... Fluidic **oscillator**... Results of measured dependence of **oscillation** **frequency** on the supplied flow rate in the layout shown in Figs. 20 and 12. Apart from basic **frequency** L, the output spectrum exhibited a much higher **frequency** component H.
... **Frequency** of generated **oscillation** plotted as a function of the air flow rate. Similarly as in Fig. 9 this dependence does not the fit the usual (constant Strouhal number) proportionality between **frequency** and flow rate.
... Basic data on the geometry of the **oscillator** used in the high-**frequency** experiments.
... Dependence of bubble natural **oscillation** **frequency** on the size – based on the measurements in Tesař (2013b). The line is fitted for constant value of **oscillation** Weber number We0.

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PES of the **qubit** system (a) and total dipole surface (b). For both surfaces: −52.8 pm⩽rA1⩽+52.8pm and −37.4pm⩽rE⩽+37.4pm.
... Normal modes included in the quantum dynamical calculation. (a) Coordinates of the **qubit** modes, (b) coordinates of the non-**qubit** modes.
... Spectral analysis of the NOT (top) and CNOT (bottom) gate. The solid lines correspond to the spectra of the optimized pulses, the dashed lines to the spectra of the sub pulses. The vertical lines indicate the relevant **qubit** basis transition **frequencies** for the quantum gates.
... spectroscopical data of the **qubit** vibrational modes E and A1 and the non-**qubit** modes, the δ-deformation mode (E) and the dissociative mode (A1)

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