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1. Introduction We are going to investigate the equation ut(t, x ... - ICMS

1. Introduction We are going to investigate the equation ut(t, x ... - ICMS

1. Introduction We are going to investigate the equation ut(t, x ... - ICMS

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4result can be proved for <strong>equation</strong>s with variable continuous coefficients. However, in<strong>the</strong> main application, which we have in mind, <strong>to</strong> s<strong>to</strong>chastic partial differential <strong>equation</strong>sfrom filtering <strong>the</strong>ory, <strong>the</strong> regularity of a ij in time is hard <strong>to</strong> control. Therefore, wealways deal only with measurable coefficients and, in Sec. 6 after some additional work,we prove our main result for <strong>equation</strong>s in R × R d +in full generality.The arguments of Sec. 6 <strong>are</strong> based on Lemma 2.5, which also allows us <strong>to</strong> give adifferent proof of <strong>the</strong> result in R × R d by using <strong>the</strong> Marcinkiewicz interpolation <strong>the</strong>oremra<strong>the</strong>r than <strong>the</strong> Calderón-Zygmund <strong>the</strong>orem.The proofs of part of <strong>the</strong> results <strong>are</strong> based on a general <strong>the</strong>orem saying, roughlyspeaking that, whatever estimate is true for <strong>the</strong> heat <strong>equation</strong>, it is also true for parabolic<strong>equation</strong>s with coefficients depending only on time. This <strong>the</strong>orem is equally applicable<strong>to</strong> Sobolev and Hölder spaces.Finally, it is worth noting that we also give results for <strong>the</strong> initial value problems. Togive <strong>the</strong> reader a flavor of our results in R×R d + we state a particular case of Theorem 5.2.

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