Note: denotes the Laplace Transformation operator.
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Note that L − 1 s n = δ ( n ) ( t ) , and ∫ − ∞ ∞ δ ( n ) ( t ) d t = 0 for nonzero n , where δ ( t ) is the Dirac-Delta function. Thus the integrand simplifies to 3 × 2 δ ( t ) . Since the infinite integral is equal to 1 for the Dirac-Delta function. Then the integral is equal to 6.