We can reach the same result by reasoning from the physical mechanism of Zener breakdown rather than a direct ratio equation. In a Zener diode, avalanche/Zener breakdown occurs once the electric field across the depletion region reaches a fixed critical value \( E_c \) that depends only on the semiconductor material, not on the diode's geometry. Since the field across a depletion region of width \( W \) under a reverse voltage \( V \) is \( E = \dfrac{V}{W} \), breakdown happens exactly when \[ \dfrac{V}{W} = E_c \ (\text{constant}) \] which means \( V \) must be directly proportional to \( W \).
Using the first (original) condition to fix this constant: \[ E_c = \dfrac{V_1}{W_1} = \dfrac{100}{20} = 5 \ \text{V per unit width} \] Applying this same critical field to the new, narrower depletion region of width \( W_2 = 1 \): \[ V_2 = E_c \times W_2 = 5 \times 1 = 5\text{V} \]
Therefore, the correct answer is 5V.