Those two expressions, $\delta'(t)$ and $-\delta(t)/t$, are equivalent. Here is an explanation.
Let $f:\mathbb{R}\rightarrow\mathbb{R}$ be a function with compact support that is differentiable at 0. We will show that
$$
\int_{-\infty}^{\infty} tf(t)\delta'(t) dt = -\int_{-\infty}^{\infty} f(t) \delta(t) dt
$$
or in other words, $t\delta'(t) = -\delta(t)$. Let $F$ be an antiderivative of $f$ (not the Laplace transform). Since
$$
(tF\delta')' = F\delta' + tf\delta' + tF\delta'',
$$
we can say
$$
\begin{align}
\int_{-\infty}^{\infty} tf(t)\delta'(t) dt &= \left.tF(t)\delta'(t)\right|_{-\infty}^{\infty} -
\int_{-\infty}^{\infty}F(t)\delta'(t)dt - \int_{-\infty}^{\infty} tF(t)\delta''(t)dt \\
&= f(0) - (tF)''(0) \\
&= -f(0) \\
&= -\int_{-\infty}^{\infty} f(t)\delta(t) dt.
\end{align}
$$
The $tF(t)\delta'(t)$ term is zero because $F$ and $\delta'$ are identically zero for large $|t|$. The $(tF)''(0)$ term is $2f(0)$ since $(tF)'' = 2f + tf'$.
Let $g(t) = tf(t)$. Then
$$
\int_{-\infty}^{\infty} g(t)\delta'(t) dt = \int_{-\infty}^{\infty} -\frac{g(t)}{t} \delta(t) dt.
$$
So $\delta'(t) = -\delta(t)/t$ for test functions $g$ that are twice differentiable at 0 with $g(0)=0$.