Missing boundary data reconstruction for the heat equation

Author(s):  
Amel Ben Abda ◽  
Naima Benmeghnia ◽  
Rim Guetat
2008 ◽  
Vol 2 (4) ◽  
pp. 411-426 ◽  
Author(s):  
Rajae Aboulaϊch ◽  
◽  
Amel Ben Abda ◽  
Moez Kallel ◽  
◽  
...  

1970 ◽  
Vol 11 (2) ◽  
pp. 117-125 ◽  
Author(s):  
J. W. Dettman

This paper is concerned with three basic transformsThe first of these has been studied by Widder [1], who points out that f(t) can be interpreted as the temperature u(0, t) on the time axis, where u(x, t) is the solution of the heat equation withsymmetric initial temperature u(x, 0) = g(|x|). The second has also been studied by Widder [2], where it is pointed out that f(t) can be interpreted as the value of the harmonic function u(x, t) on the t-axis arising from the boundary data u(x, 0) = g(|x|).


2009 ◽  
Vol 347 (9-10) ◽  
pp. 501-504 ◽  
Author(s):  
Amel Ben Abda ◽  
Jacques Henry ◽  
Fadhel Jday

Author(s):  
Charles L. Epstein ◽  
Rafe Mazzeo

This chapter describes the construction of a resolvent operator using the Laplace transform of a parametrix for the heat kernel and a perturbative argument. In the equation (μ‎-L) R(μ‎) f = f, R(μ‎) is a right inverse for (μ‎-L). In Hölder spaces, these are the natural elliptic estimates for generalized Kimura diffusions. The chapter first constructs the resolvent kernel using an induction over the maximal codimension of bP, and proves various estimates on it, along with corresponding estimates for the solution operator for the homogeneous Cauchy problem. It then considers holomorphic semi-groups and uses contour integration to construct the solution to the heat equation, concluding with a discussion of Kimura diffusions where all coefficients have the same leading homogeneity.


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