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    Brownian motion in attenuated or renormalized inverse-square Poisson potential

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    We consider the parabolic Anderson problem with random potentials having inverse-square singularities around the points of a standard Poisson point process in Rd\mathbb{R}^d, d3d \geq 3. The potentials we consider are obtained via superposition of translations over the points of the Poisson point process of a kernel K\mathfrak{K} behaving as K(x)θx2\mathfrak{K}(x) \approx \theta |x|^{-2} near the origin, where θ(0,(d2)2/16]\theta \in (0,(d-2)^2/16]. In order to make sense of the corresponding path integrals, we require the potential to be either attenuated (meaning that K\mathfrak{K} is integrable at infinity) or, when d=3d=3, renormalized, as introduced by Chen and Kulik in [8]. Our main results include existence and large-time asymptotics of non-negative solutions via Feynman-Kac representation. In particular, we settle for the renormalized potential in d=3d=3 the problem with critical parameter θ=1/16\theta = 1/16, left open by Chen and Rosinski in [arXiv:1103.5717].Comment: 36 page

    Gluon polarization in the nucleon demystified

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    Recently, X. Chen et al. proposed a new approach to the gauge invariant decomposition of the nucleon spin into helicity and orbital parts. The key ingredient in their construction is the separation of the gauge field into `physical' and `pure gauge' parts. We suggest a simple separation scheme and show that the resulting gluon helicity coincides with the first moment of the conventional polarized gluon distribution measurable in high energy experiments.Comment: 6 page

    Large deviations for self-intersection local times of stable random walks

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    Let (Xt,t0)(X_t,t\geq 0) be a random walk on Zd\mathbb{Z}^d. Let lT(x)=0Tδx(Xs)ds l_T(x)= \int_0^T \delta_x(X_s)ds the local time at the state xx and IT=xZdlT(x)q I_T= \sum\limits_{x\in\mathbb{Z}^d} l_T(x)^q the q-fold self-intersection local time (SILT). In \cite{Castell} Castell proves a large deviations principle for the SILT of the simple random walk in the critical case q(d2)=dq(d-2)=d. In the supercritical case q(d2)>dq(d-2)>d, Chen and M\"orters obtain in \cite{ChenMorters} a large deviations principle for the intersection of qq independent random walks, and Asselah obtains in \cite{Asselah5} a large deviations principle for the SILT with q=2q=2. We extend these results to an α\alpha-stable process (i.e. α]0,2]\alpha\in]0,2]) in the case where q(dα)dq(d-\alpha)\geq d.Comment: 22 page
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