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Displaying similar documents to “Computation of bifurcated branches in a free boundary problem arising in combustion theory”

On the asymptotic properties of a simple estimate of the Mode

Christophe Abraham, Gérard Biau, Benoît Cadre (2010)

ESAIM: Probability and Statistics

Similarity:

We consider an estimate of the mode of a multivariate probability density with support in d using a kernel estimate drawn from a sample . The estimate is defined as any in {} such that f n ( x ) = max i = 1 , , n f n ( X i ) . It is shown that behaves asymptotically as any maximizer θ ^ n of . More precisely, we prove that for any sequence ( r n ) n 1 of positive real numbers such that r n and r n d log n / n 0 , one has r n θ n - θ ^ n 0 in probability. The asymptotic normality of follows without further work.

Penultimate approximation for the distribution of the excesses

Rym Worms (2010)

ESAIM: Probability and Statistics

Similarity:

Let be a distribution function (d.f) in the domain of attraction of an extreme value distribution H γ ; it is well-known that , where is the d.f of the excesses over , converges, when tends to , the end-point of , to G γ ( x σ ( u ) ) , where G γ is the d.f. of the Generalized Pareto Distribution. We provide conditions that ensure that there exists, for γ > - 1 , a function which verifies lim u s + ( F ) Λ ( u ) = γ and is such that Δ ( u ) = sup x [ 0 , s + ( F ) - u [ | F ¯ u ( x ) - G ¯ Λ ( u ) ( x / σ ( u ) ) | converges to faster than d ( u ) = sup x [ 0 , s + ( F ) - u [ | F ¯ u ( x ) - G ¯ γ ( x / σ ( u ) ) | .

How to get a conservative well-posed linear system out of thin air. Part I. Well-posedness and energy balance

George Weiss, Marius Tucsnak (2010)

ESAIM: Control, Optimisation and Calculus of Variations

Similarity:

Let be a possibly unbounded positive operator on the Hilbert space , which is boundedly invertible. Let be a bounded operator from 𝒟 A 0 1 2 to another Hilbert space . We prove that the system of equations z ¨ ( t ) + A 0 z ( t ) + 1 2 C 0 * C 0 z ˙ ( t ) = C 0 * u ( t ) y ( t ) = - C 0 z ˙ ( t ) + u ( t ) , determines a well-posed linear system with input and output . The state of this system is x ( t ) = z ( t ) z ˙ ( t ) 𝒟 A 0 1 2 × H = X , where is the state space. Moreover, we have the energy identity x ( t ) X 2 - x ( 0 ) X 2 = 0 T u ( t ) U 2 d t - 0 T y ( t ) U 2 d t . We show that the system described above is isomorphic to its dual, so that...