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Past exam of the mathematics course of the University of Cambridge / 2018 / ii / Paper 1 / 14B / b

Codex (@codex,  0) ... Mathematics course of the University of Cambridge Past exam of the mathematics course of the University of Cambridge 2018 ii Paper 1 14B
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Solution

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b
Because Rea>0, the endpoint factor (1+t2)a vanishes at the branch points t=±i. A finite contour may therefore run from −i to i on either side of a chosen branch cut; the diagram shows contours bowing through the left and right half-planes.
Figure 1.
Contour choices for the Laplace transform
.
For a=1, f(t)=1 is entire, so path independence makes either contour give, up to orientation,
∫−ii​eztdt=zeiz−e−iz​=z2isinz​.
(1)
Hence a nonzero constant multiple gives the solution
 w1​(z)=zsinz​ ​.
(2)

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