Sentence examples for mode of frequency from inspiring English sources

When electrons pass through the quantum dot, they are coupled to a single phonon mode of frequency ω 0. The dc conductance of the system has been investigated theoretically before, leading to some distinct hallmarks of the electron- phonon (e-ph) interaction [3 6].

According to CMT [12, 42, 43], the spectral transmittance of the system supporting a resonant mode of frequency ω 0 can be written as T=frac{{left omega -{omega}_0right)}{2+{left omegau}_iright)}^2}{{left(omega -{omega}_0right)}^2+{left(1/{tau}_i+1/{tau}_eright)}^2} (5).

PSDF shows that wind forces do not practically affect the bending moment, which is predominantly governed by the second mode of frequency; however, the other response parameters like deck displacement, hinge rotation and hinge shear were affected in significant manner under the action of wind forces.

When electrons pass through the quantum dot, they are coupled to a single phonon mode of frequency ω 0. In its simplest formulation, the Hamiltonian of the electron-phonon (e-ph) interaction can be written as, where b (c 0) and b † are the annihilation and the creation operators of phonons (electrons in the dot), and γ is the coupling strength of the e-ph interaction.

Indeed, taking into account the known relation [20] {gamma}_i=-frac{partial ln {omega}_i}{partial ln V}=frac{B_0}{omega}_i}{partialial {omega}_i}{P}rtial P} (1 where γ i is the Gruneisen parameter for a quasiharmonic mode of frequency ω i (ω 0 marks the one at zero pressure, B 0 is bulk modulus); we obtain the bulk modulus from the dependence ω(P).

The requirement that the quantum theory should go over to the classical description for low modes of frequency, is not at all a principle.

By using FSWT, the filtering under high noise, and the segmenting of signal with high damping and close modes of frequency, will be discussed.

We assume perfect phase matching and restrict this analysis to spectral single field modes of frequency ω S and ω I, respectively, which is experimentally realized by the narrow spectral filter.

To optimize conventional phase locked loop (PLL) performance through enhancement of drive mode stability of frequency and amplitude, enhanced phase locked loop (EPLL) and quadrature phase locked loop (QPLL) algorithms were investigated.

The red curve of Fig. 3(b) predicts a global ((q=0)) mode of temporal frequency (fsimeq47mbox{ HZ}).

Secondary outcomes were the time from induction to delivery, need for oxytocin augmentation, mode of delivery, frequency of side effects, and neonatal and maternal outcome.