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The problem of uniqueness of such measures is also partially solved.
(15) The problem of uniqueness of the null solution of (15) was studied by Gripenberg in [37].
Next, we deal with the problem of uniqueness versus non-uniqueness for (1.1 - 1.3 1.1 - 1.3ase on vanishing inithel data (u0i(x) = 0, i = 1, 2,..., k).
Hence by the Hopf bifurcation theorem [12], the system enters into a Hopf-type small amplitude periodic solution at the parametric value α = α ∗ near the positive interior equilibrium point P 2. Now we consider the problem of uniqueness of the limit cycle arising from Hopf bifurcation at the parametric value α = α ∗.
In relation to the problem of uniqueness, by continuity and taking into account that ε max = ε y when ( A_{c}^{prime} = 0 ) (cf. Gil-Martín et al. 2009), the actual value of ε max is that of the solution closest to the yield strain ε y, that is, the greatest one of the two positive real solutions of Eq. (2).
It can be seen that, for high values of ( A_{c}^{prime} ) (like ( A_{c}^{prime} = 0.7A_{c} ) and ( A_{c}^{prime} = 0.9A_{c} )), the curve G [f ct, ε max ] = 0 presents a knee that breaks the bijection between f ct and ε max (problem of uniqueness), or even, no solutions exists for ε max (problem of existence), as it occurs by taking ( A_{c}^{prime} = A_{c} ) in this specimen.
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Some problems of uniqueness of the associated partial differential equations were investigated.
Enforcing uncorrelatedness rather than independence poses problems of uniqueness, but has often proved to give very useful results [9, 11].
We provide additional results on the problems of uniqueness, efficiency of the equilibrium, and convergence of a best-response-based dynamics to the equilibrium.
We address the problem of the uniqueness of the solution of problem (13), which relies on the formal Euler-Lagrange equation of (13): Proof of Theorem 2. Let us denote (A.15).
The problem of population uniqueness estimation then becomes a problem of parameter estimation.
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