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Reasonable values of the transition oscillator strengths could still be demonstrated at about 5 μm.
The corresponding values of the transition lengths were computed and are reported as well.
The most general kind of SPNs with product-form solution introduced by Coleman et al. (and denoted here by SΠ-nets) suffers a serious drawback: the existence of such a solution depends on the values of the transition rates.
Table 2 provides calculated values of the transition radius '( r_{0} )', according to Eq. (4), for the main magnetic nanomaterials (Martel 2015; Kolhatkar et al. 2013).
Using Equation 4, we can estimate the DP values of the transition for the excitonic states 1H1E and 1L1E to be 0.5 % ± 0.5% and 6.3 % ± 0.5%, respectively.
It is worth noting that the higher energy values of the transition states associated with the final pathways are consistent with the strained, four cantered nature of the calculated transition state structures.
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This equilibrium is possible for all our test nodes under the higher test rates, whether or not the value of the transition rate affects which state is the most probable.
A substantial positive value of the transition heat capacity increment of PEO is detected suggesting that the transition is accompanied by an exposure of the polymer hydrophobic groups to water.
We focus on the influence of the elasticity of the trunk joints on the possibility of the transition and the allowable value of the transition velocity.
We remark that the value of the transition probability p d (i d,j d ) is the inverse of the number of outgoing links, i.e., allowed transitions, from i d.
The Φ value of the cutoff point between the saltating and the suspended component is 2, and the Φ value of the transition zone is about 2 4.25 (Fig. 4).
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