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To extend the solutions globally we build on an idea due to Colliander, Holmer and Tzirakis.
Now we need estimates which allow us to extend the solutions to the whole interval ([0, T]) and pass to limit as (mrightarrowinfty) and (epsilonrightarrow0). Hence, uniform estimates with respect to m and ϵ are needed.
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It is possible to extend the solution on the right of to some where the solution will assume the value.
In order to extend the solution to a maximal interval we can apply the Theorem 2.3 [[14], p. 97].
In some cases, it is desirable to extend the solution to the interval [ 0, N ], see Remark 2.1 hereafter.
This procedure can be repeated to extend the solution to the entire interval [0, T] in finitely many steps.
Now we need to extend the solution ϕ of equation (3.1) to the domain ((-infty,xi^)) and ((xi^,+infty)).
Thus, z ( x ) can be used to extend the solution y ˆ ( x ) on [ 0 ; a 2 ].
With the help of (11) we then can extend the solution to the interval ( q a, q b ) provided ( q a, q b ) ∩ ( a, b ) = ∅.
Next, we extend the solution of RC-MCSB problem to our target problem and present a novel and efficient bottom-up solution.
Then, the same idea is in turn applied to extend the solution of a reduced matrix eigen-decomposition problem to approximate the eigenvectors of an SPSD matrix.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com