How can I deduce that
$$
\frac{1}{\sqrt{4\pi t}}\int_{-\infty}^{\infty}\sin(y)\,e^{-\frac{(x-y)^2}{4t} } dy = e^{-t} \sin(x)
$$
without actually evaluating the definite integral?
Answer
I will assume the following result:
The solution to the Heat Equation
$$\frac{df}{dt} = \nabla^2f$$
with initial condition $f(x,0) = g(x)$ can be written
$$f(x,t) = \frac{1}{\sqrt{4\pi t}}\int_{-\infty}^\infty e^{-\frac{(x-y)^2}{4t}}g(y) dy$$
Now by inserting
$$f(x,t) = e^{-t}\sin(x)$$
into the Heat Equation we find that it does satisfy it with the initial condition $f(x,0) = \sin(x)$. From the result above it therefore follows that
$$e^{-t}\sin(x) = \frac{1}{\sqrt{4\pi t}}\int_{-\infty}^\infty e^{-\frac{(x-y)^2}{4t}}\sin(y) dy$$
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