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The one-dimensional heat equation in the Alexiewicz norm

Abstract

A distribution on the real line has a continuous primitive integral if it is the distributional derivative of a function that is continuous on the extended real line. The space of distributions integrable in this sense is a Banach space that includes all functions integrable in the Lebesgue and Henstock--Kurzweil senses. The one-dimensional heat equation is considered with initial data that is integrable in the sense of the continuous primitive integral. Let Θt(x)=exp(x2/(4t))/4πt\Theta_t(x)=\exp(-x^2/(4t))/\sqrt{4\pi t} be the heat kernel. With initial data ff that is the distributional derivative of a continuous function, it is shown that ut(x):=u(x,t):=fΘt(x)u_t(x):=u(x,t):=f\ast\Theta_t(x) is a classical solution of the heat equation u11=u2u_{11}=u_2. The estimate fΘtf/πt\|f\ast\Theta_t\|_\infty\leq\|f\|/\sqrt{\pi t} holds. The Alexiewicz norm is f=supIIf\|f\|=\sup_I|\int_If|, the supremum taken over all intervals. The initial data is taken on in the Alexiewicz norm, utf0\|u_t-f\|\to 0 as t0+t\to 0^+. The solution of the heat equation is unique under the assumptions that ut\|u_t\| is bounded and utfu_t\to f in the Alexiewicz norm for some integrable ff. The heat equation is also considered with initial data that is the nnth derivative of a continuous function and in weighted spaces such that f(x)exp(ax2)dx\int_{-\infty}^\infty f(x)\exp(-ax^2)\,dx exists for some a>0a>0. Similar results are obtained

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