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This case along with all other possible cases of the asymptotic behaviour of the solution (Z(m)) is discussed in Lemma 1, Section 3.
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This restriction to the antenna setup due to the need for d k to be greater than or equal to m k is discussed in more detail in the section on feasibility conditions, in Section 4.2.
This restriction to the antenna setup due to the need for d k to be greater than or equal to m k is discussed in more detail in the section on feasibility conditions, Section 4.2.
The general trends of thermodynamic stabilities versus atomic number of M were discussed for {Sc,Ti}2M3Si.
The procedure for obtaining a higher order approximation is described, and in particular two criteria for chosing the elliptic function parameter m are discussed.
The values of k and m are discussed in Section 5.
They will be discussed later when Alpine fold belts lower than 3000 m. are discussed.
Part of the discrepancy perhaps results from the fact that the ms is discussing the "existence" of the tree of life - if it does not "exist" (sensu Woese), then we should forget about it.
In addition, ranking of asphalt mastics based on various parameters (i.e. CTOD and m(t)) is discussed in this paper.
The influence of electron (hole) doping on the electronic structure of metallic single-walled carbon nanotubes (m-SWCNTs) is discussed by first principles calculations.
The nonlinear case ( m ≠ 1 ) is discussed in Example 3.4 on p.181, and the linear case ( m = 1 ) in Examples 4.2-4.3 4.2-4.325-227.
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