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Such graphs show that the instability damping rate decreases as the plasma parameters ((k), (eta _{d}),(sigma _{i})) increase.
Indeed, it significantly enhances the insulating capacity of the mortar, increases heat diffusion damping rate and makes mortar lighter.
They noted that larger surface warming caused by the smaller radiative damping rate of λ accompanies stronger ocean stratification and less heat release from the interior of the ocean through convection at high latitudes.
In our problem, on varying beam orientation, temperature ((bar K)), or damping rate, one may increase or decrease the number of unstable modes in the system and expect similar results as in the previously mentioned finite domain case.
Analysis of combustor damping rates show a strong dependence of damping rate on staging amplitude but no strong dependence on transient duration or direction.
The work of Braginsky introduced radiation pressure dynamical backaction, in which a mechanical oscillator that is parametrically coupled to an electromagnetic mode can experience a change in its rigidity and it's damping rate.
Figure 18 Small signal modulation parameters for a 6 μm SML QD-VCSEL at 25 and 85 °C, obtained from fitting the modulation response to the three-parameter transfer function: (a) —3 dB bandwidth and (b) resonance frequency as a function of the square root of the current above threshold, (c) damping rate vs. squared resonance frequency.
In the linear analysis, the dispersion relation is obtained, and the dependence of damping rate of the waves on the carrier wave number (k), the dust kinematic viscosity coefficient (eta _{d}) and the ratio of the ions to the electrons temperatures (sigma _{i}) is discussed.
The relationship between resonance frequency and damping rate defines the K-factor, which is 0.83 ns at RT. Furthermore, the K-factor is directly related to the damping-limited bandwidth (f3dB, damping) by [16]: f 3 dB,damping = 2 2 π K (2).
Figure 18 shows small signal modulation parameters under continuous wave (cw) operation for a 6 μm SML QD-VCSEL at 25 and 85 °C, obtained from fitting the three-parameter transfer function with the unknown resonance frequency fres, damping rate γ and parasitic cutoff frequency of the RC low-pass fpar to the S21 modulation response [41].
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Since the SEE relaxation is determined by the damping rate of plasma waves with the same frequency, responsible for the SEE generation, we calculated damping rates of plasma waves with ω∼ωuh (ω is the plasma wave frequency, ωuh is the upper hybrid frequency) for frequencies close to and distant from the double resonance where ωuh∼4ωce (ωce="2πfce).
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