364 research outputs found

    On a fourth order nonlinear Helmholtz equation

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    In this paper, we study the mixed dispersion fourth order nonlinear Helmholtz equation Δ2u−ÎČΔu+αu=Γ∣u∣p−2u\Delta^2 u -\beta \Delta u + \alpha u= \Gamma|u|^{p-2} u in RN\mathbb R^N for positive, bounded and ZN\mathbb Z^N-periodic functions Γ\Gamma. Using the dual method of Evequoz and Weth, we find solutions to this equation and establish some of their qualitative properties

    Existence of positive solutions of a superlinear boundary value problem with indefinite weight

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    We deal with the existence of positive solutions for a two-point boundary value problem associated with the nonlinear second order equation uâ€Čâ€Č+a(x)g(u)=0u''+a(x)g(u)=0. The weight a(x)a(x) is allowed to change its sign. We assume that the function g ⁣:[0,+∞[→Rg\colon\mathopen{[}0,+\infty\mathclose{[}\to\mathbb{R} is continuous, g(0)=0g(0)=0 and satisfies suitable growth conditions, so as the case g(s)=spg(s)=s^{p}, with p>1p>1, is covered. In particular we suppose that g(s)/sg(s)/s is large near infinity, but we do not require that g(s)g(s) is non-negative in a neighborhood of zero. Using a topological approach based on the Leray-Schauder degree we obtain a result of existence of at least a positive solution that improves previous existence theorems.Comment: 12 pages, 4 PNG figure

    Compactness and existence results in weighted Sobolev spaces of radial functions. Part II: Existence

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    We prove existence and multiplicity results for finite energy solutions to the nonlinear elliptic equation −△u+V(∣x∣)u=g(∣x∣,u)in Ω⊆RN, N≄3, -\triangle u+V\left( \left| x\right| \right) u=g\left( \left| x\right| ,u\right) \quad \textrm{in }\Omega \subseteq \mathbb{R}^{N},\ N\geq 3, where Ω\Omega is a radial domain (bounded or unbounded) and uu satisfies u=0u=0 on ∂Ω\partial \Omega if Ω≠RN\Omega \neq \mathbb{R}^{N} and u→0u\rightarrow 0 as ∣x∣→∞\left| x\right| \rightarrow \infty if Ω\Omega is unbounded. The potential VV may be vanishing or unbounded at zero or at infinity and the nonlinearity gg may be superlinear or sublinear. If gg is sublinear, the case with g(∣⋅∣,0)≠0g\left( \left| \cdot \right| ,0\right) \neq 0 is also considered.Comment: 29 pages, 8 figure

    First escaping fast ion mesurements in ITER-like geometry using an activation probe

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    More research is needed to develop suitable diagnostics for measuring alpha particle confinement in ITER and techniques relevant for fusion reactor conditions need further development. Based on nuclear reactions, the activation probe is a novel concept first tested in JET. It may offer a more robust solution for performing alpha particle measurements in ITER. This paper describes the first escaping fast ion measurements performed at ASDEX Upgrade (AUG) tokamak using an activation probe. A detailed analysis, outside the scope of this contribution, will be published in a journal paper.JRC.D.4-Standards for Nuclear Safety, Security and Safeguard

    Combination of fast-ion diagnostics in velocity-space tomographies:Paper

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    Fast-ion Dα (FIDA) and collective Thomson scattering (CTS) diagnostics provide indirect measurements of fastion velocity distribution functions in magnetically confined plasmas. Here we present the first prescription for velocity-space tomographic inversion of CTS and FIDA measurements that can use CTS and FIDA measurements together and that takes uncertainties in such measurements into account. Our prescription is general and could be applied to other diagnostics. We demonstrate tomographic reconstructions of an ASDEX Upgrade beam ion velocity distribution function. First, we compute synthetic measurements from two CTS views and two FIDA views using a TRANSP/NUBEAM simulation, and then we compute joint tomographic inversions in velocity-space from these. The overall shape of the 2D velocity distribution function and the location of the maxima at full and half beam injection energy are well reproduced in velocity-space tomographic inversions, if the noise level in the measurements is below 10%. Our results suggest that 2D fast-ion velocity distribution functions can be directly inferred from fast-ion measurements and their uncertainties, even if the measurements are taken with different diagnostic methods
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