Concept:
In a rectangle $OACB$, the adjacent side vectors $\vec{a}$ and $\vec{b}$ are perpendicular ($\vec{a} \cdot \vec{b} = 0$), which means the angle between them is $90^\circ$. We can find the relationship between their lengths by expanding the given vector cross-product equation, and then use trigonometric identities to find the angle between the diagonals.
Step 1: Expand the vector equation using side lengths.
Let the lengths of the sides be defined as $a = |\vec{a}|$ and $b = |\vec{b}|$. Since the sides meet at a right angle, the magnitude of their cross product simplifies to:
$$|\vec{a} \times \vec{b}| = a \cdot b \cdot \sin(90^\circ) = ab$$
Substitute this back into the problem's core equation:
$$16ab = 3(a + b)^2 \quad \Rightarrow \quad 16ab = 3a^2 + 6ab + 3b^2$$
Move all terms to one side to form a quadratic equation:
$$3a^2 - 10ab + 3b^2 = 0$$
Step 2: Factor the equation to find the ratio between the sides.
Split the middle term to factor the quadratic expression:
$$3a^2 - 9ab - ab + 3b^2 = 0 \quad \Rightarrow \quad 3a(a - 3b) - b(a - 3b) = 0$$
$$(3a - b)(a - 3b) = 0 \quad \Rightarrow \quad b = 3a \quad \text{or} \quad a = 3b$$
By symmetry, let us choose $b = 3a$ without loss of generality. This means the rectangle is 3 times taller than it is wide.
Step 3: Relate the side ratio to the diagonal half-angle.
Let $\alpha$ be the angle that the main diagonal $OC$ makes with the base side vector $\vec{a}$. Using the right-triangle properties of the rectangle:
$$\tan \alpha = \frac{\text{Opposite}}{\text{Adjacent}} = \frac{b}{a} = \frac{3a}{a} = 3$$
By standard geometry, the diagonals of a rectangle are equal in length and bisect each other, splitting the shape into isosceles triangles. The acute angle $\theta$ between the intersecting diagonals satisfies the geometric identity:
$$\frac{\theta}{2} = 90^\circ - \alpha$$
Step 4: Calculate the value of $\tan(\frac{\theta}{2})$.
Apply the trigonometric complement rule to evaluate our target expression:
$$\tan\left(\frac{\theta}{2}\right) = \tan(90^\circ - \alpha) = \cot \alpha = \frac{1}{\tan \alpha}$$
Substitute our known value $\tan \alpha = 3$ into the fraction:
$$\tan\left(\frac{\theta}{2}\right) = \frac{1}{3}$$
This matches option (A) perfectly.