Step 1: Substitute the trial solution into the equation.
We are told \(y = e^{Ax}\) is a solution of \(\dfrac{d^2y}{dx^2} - y = 0\). Differentiate once: \(\dfrac{dy}{dx} = A e^{Ax}\). Differentiate again: \(\dfrac{d^2y}{dx^2} = A^2 e^{Ax}\).
Step 2: Substitute back into the differential equation.
\[
A^2 e^{Ax} - e^{Ax} = 0
\]
Factor out \(e^{Ax}\), which is never zero for any finite \(A\) and \(x\):
\[
e^{Ax}(A^2 - 1) = 0
\]
Step 3: Solve the resulting algebraic equation.
Since \(e^{Ax} \neq 0\), we need
\[
A^2 - 1 = 0
\]
\[
A^2 = 1
\]
\[
A = \pm 1
\]
This is the characteristic equation of the differential equation, and its two roots give the two independent exponential solutions.
Step 4: Check each option against \(A = \pm 1\).
\(A = 0\) gives \(y = e^{0} = 1\), a constant. Substituting back: \(\dfrac{d^2}{dx^2}(1) - 1 = 0 - 1 = -1 \neq 0\), so \(A=0\) fails. \(A = 1\) gives \(A^2 - 1 = 1 - 1 = 0\), which satisfies the equation. \(A = -1\) gives \(A^2 - 1 = 1 - 1 = 0\), which also satisfies the equation. \(A \to -\infty\) is not a finite value and does not satisfy \(A^2=1\), so it fails.
Final Answer:
Both \(A=1\) and \(A=-1\) satisfy the equation.
\[ \boxed{A = 1 \text{ and } A = -1} \]