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In this paper we study the effect of absorption peak correlation in finite length carbon nanotubes and graphene nanoribbons.
In addition, the wave propagation in finite length structures due to broad band impulse loading is studied to bring out the higher order effects.
Finally, the power of the present approach in obtaining the interlaminar stresses in finite length thick laminated plates with general lay-ups is examined.
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Since the conductors are fabricated in finite lengths, every once in a while two conductors have to be connected in the field, using appropriate fittings.
No metallic states are found in finite-length zigzag nanoribbons though all infinite-length zigzag nanoribbons are metallic.
Screening effect in finite-length carbon nanotubes (CNT) and their agglomerates hinders significantly the electromagnetic interaction in composite materials.
In finite-length sequences the numbers of each type of codon occurring at each type of site can fluctuate a lot.
In this paper we present the results of numerical simulations of oscillatory mass transport in a finite length slug in a circular tube which show that the influence of the end regions on the degree of transport enhancement is always of the order of the slug aspect ratio.
The ML performance bound evaluated in the previous subsection factors in the finite length of a PA code ensemble, but the assumption of an ML decoder may be optimistic.
Let c represent the instantaneous channel service in terms of bits that can be served from the queue in a finite length slot of τ seconds, the cumulative channel process, C t), i.e., the aggregate number of bits that can be served in [0,t] can be found as, (C t)=int _{tau =0}^{t}{c dtau dtau }).
In a finite length, there are always finite probabilities of scattering.
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