Step 1: Understand the condition of parallel resonance.
In a parallel RLC circuit at resonance, the inductive susceptance and capacitive susceptance are equal in magnitude and opposite in sign. Hence,
\[
I_L = I_C \quad \text{(equal magnitude, opposite phase)}
\]
Therefore, the net reactive current drawn from the source is zero.
Step 2: Identify the source current.
Since the reactive currents cancel each other, the source current flows only through the resistive branch.
Thus,
\[
I_{\text{source}} = I_R = 1 \text{ mA}
\]
Step 3: Analyze the branch currents.
Although the source current is only $1\,\text{mA}$, the individual branch currents $I_L$ and $I_C$ can be much larger due to resonance. This is known as current magnification in parallel resonance.
Step 4: Evaluate the options.
(A) $\lvert I_R \rvert<1\,\text{mA}$ is incorrect because $I_R = 1\,\text{mA}$.
(B) $\lvert I_R + I_L \rvert>1\,\text{mA}$ is correct because $I_L$ is large and adds vectorially with $I_R$.
(C) $\lvert I_R + I_C \rvert<1\,\text{mA}$ is incorrect because $I_C$ is also large.
(D) $\lvert I_L + I_C \rvert>1\,\text{mA}$ is incorrect since $I_L$ and $I_C$ cancel each other at resonance.
Step 5: Conclusion.
Hence, the correct statement for a parallel RLC circuit at resonance is
\[
\boxed{\lvert I_R + I_L \rvert>1 \text{ mA}}
\]