Step 1: Simplify the given expression.
We are given the limit:
\[
\lim_{x \to 0} \frac{1 - \sec^2(\alpha x)}{\alpha x^2} = -3
\]
To solve this, first use the identity \( \sec^2 \theta = 1 + \tan^2 \theta \). Hence,
\[
\sec^2(\alpha x) = 1 + \tan^2(\alpha x)
\]
Substitute this into the limit expression:
\[
\lim_{x \to 0} \frac{1 - (1 + \tan^2(\alpha x))}{\alpha x^2} = -3
\]
This simplifies to:
\[
\lim_{x \to 0} \frac{- \tan^2(\alpha x)}{\alpha x^2} = -3
\]
Step 2: Use the approximation for small angles.
For small angles, \( \tan(\theta) \approx \theta \), so:
\[
\tan(\alpha x) \approx \alpha x
\]
Thus,
\[
\tan^2(\alpha x) \approx (\alpha x)^2
\]
Substitute this approximation into the expression:
\[
\lim_{x \to 0} \frac{- (\alpha x)^2}{\alpha x^2} = -3
\]
Simplify the expression:
\[
\lim_{x \to 0} -\alpha^2 = -3
\]
Step 3: Solve for \( \alpha \).
This gives:
\[
\alpha^2 = 3
\]
Hence,
\[
\alpha = \pm \sqrt{3}
\]