Due to the bug reported here, the following method actually gets the wrong answer. However, the method is a good one for proving the relation in the OP.
One way to check is to take advantage of the fact that Mathematica's symbolic Fourier transform functionality can deal with these things. Note:
FourierTransform[DiracDelta[Sin[x]], x, k]
(* DiracComb[k]/Sqrt[2 π] *)
and
InverseFourierTransform[DiracComb[k]/Sqrt[2 π], k, x]
(* DiracComb[x/(2 π)]/(2 π) *)
which illustrate the fact that DiracDelta[Sin[x]]
and DiracComb[x/(2 π)]/(2 π)
are the same. Evidently,
$$
\delta(\sin(x)) = \frac{1}{2\pi}\sum_{n=-\infty}^{\infty}\delta\left(\frac{x}{2\pi}-n\right),
$$
according to the definition of DiracComb
in the documentation. This then simplifies to
$$
\delta(\sin(x)) = \sum_{n=-\infty}^{\infty}\delta\left(x-2\pi n\right).
$$
===
is not the correct thing to use because that checks to see if the expressions are structurally identical, not mathematically equal. Secondly,InverseFourierTransform[FourierTransform[DiracDelta[Sin[x]], x, k], k, x]
seems to disagree with your statement. $\endgroup$Sin[2 x] === 2 Sin[x] Cos[x]
; theHead
of the lhs isSin
and theHead
of the rhs isTimes
, which are not identical. $\endgroup$