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The second term in (28) can be considered as interference and its characteristics are similar to the third and fourth terms when the difference between each term is large enough.
The first term in Eq. 3, G SIN = ∂ P SIN / ∂ T, is the cooling thermal conductance of the SIN junction that gives the negative electrothermal feedback (ETF); when this term is large, it reduces the temperature response, δT, because the cooling power, PSIN, compensates for the change of signal power in the bolometer.
where cov [ Ŝ k ( f ) Ŝ l ( f ) ] = | h k T Φ H ( f ) R x Φ ( f ) h l | 2 + | h k T Φ ( f ) R x Φ ( f ) h l | 2. The second term is large only for frequencies close to f=0 or to the Nyquist frequency, where the function h k T Φ ( f ) R x Φ ( f ) h l overlaps its conjugate.
Following expectations, the second-order dispersion term is large and also increases with increasing number of nitrogen atoms with the exception of B0T and B1T in group a of the T-shaped dimers.
Similar(56)
The crystal nucleation in a-SiNW is affected easily by the nanowire surface, and therefore, the second term is larger than the first term.
Messaoudi [7] considered the semilinear Petrovsky equation with the damping and the source term, showed that the solution blows up in finite time if the growth order of damping term is larger than the growth order of source term and the energy is negative, whereas the solution is global if the growth order of damping term is not larger than the growth order of source term.
However, as described in [3], only when the removal term is larger than the entry in the use matrix from which it is being removed that is, when u i j is lower than the negative term on the right-hand side of (5), scaling down is applied to leave a zero balance.
As an example, -6 + 4 = -2; because -6 and 4 have different signs, their absolute values are subtracted, and since the negative term is larger, the answer is negative.
When the P value of domain and GO term is larger than the given significance threshold, it is considered that the domain can be annotated with the GO term, and vice versa.
The simulation results show that the truncation error is negligible if the number of terms is large than 50.
The truncation error is negligible if the number of terms is large enough: Reference [31] shows that when the number of terms is as large as 50, the finite-order approximation is good.
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