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For multilayered plates, we derive the solution in terms of the propagator matrices.
In Section 2 we derive the solution formula of our semi-linear problem.
Firstly, we derive the solution formula for the problem (1.1), (1.2).
For multilayered hybrid plates, we derive the solution in terms of the propagator matrices.
For (0< y<hat{y}), similar to the proof of Proposition 3.1, we derive the solution (v cdot)) in (3.16).
In this subsection, we derive the solution to each subproblem given in (16) in concrete setting with (λBS, μ) fixed.
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We derive the solutions for the rotation angles of the single half-wave plates depending on the desired polarization rotation angle.
By introducing a new stable set we derive the result that certain solutions with arbitrarily positive initial energy exist globally.
We will derive the solution of Problem (3) for source term f ( x, y ) ∈ L 2 ( 0, 1 ; L 2 ( 0, π ) ).
In the following, we theoretically derive the solution in the time domain for the sea-bottom deformation given by the arbitrary function of χ (t).
We will derive the solution to the RHBVP with boundary data belonging to a Hölder space in terms of an integral representation.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com