Step 1: Understanding the Question:
The problem provides the specific charge (charge-to-mass ratio, $\frac{e}{m_e}$) of an electron as a constant '$A$'. We need to express the gyromagnetic ratio of an atomically bound orbiting electron in terms of this constant.
Step 2: Detailed Explanation:
Let's look at the definitions of the quantities involved:
• The specific charge of an electron is defined as the ratio of its charge magnitude $e$ to its rest mass $m_e$:
$$ \text{Specific Charge} = \frac{e}{m_e} = A $$
• The gyromagnetic ratio ($\gamma$) of an electron is defined as the ratio of its magnetic dipole moment ($\mu_l$) to its orbital angular momentum ($L$):
$$ \gamma = \frac{\mu_l}{L} $$
From Bohr's atomic model derivations, for a circular electron orbit of radius $r$ with speed $v$, the current is $I = \frac{ev}{2\pi r}$ and the magnetic area is $\pi r^2$, giving $\mu_l = I \cdot \text{Area} = \frac{evr}{2}$. The angular momentum is $L = m_e v r$.
Taking the ratio reveals a constant relationship:
$$ \gamma = \frac{\frac{evr}{2}}{m_e vr} = \frac{e}{2m_e} $$
Substituting our given parameter $\frac{e}{m_e} = A$ into the gyromagnetic ratio formula:
$$ \gamma = \frac{1}{2} \left(\frac{e}{m_e}\right) = \frac{A}{2} $$
Step 3: Final Answer:
The gyromagnetic ratio is $\frac{A}{2}$, which corresponds to option (D).