Step 1: Understanding the transistor current relations.
The current through \( R_2 \) is given by \( I_{R_2} = 10 I_B \). The collector current \( I_C \) is related to the base current by \( I_C = \beta I_B \), so \( I_B = \frac{I_C}{\beta} = \frac{1 \, \text{mA}}{50} = 20 \, \mu\text{A} \).
Step 2: Calculating the voltage drop across \( R_2 \).
Using Ohm's law, the voltage drop across \( R_2 \) is \( V_{R_2} = I_{R_2} R_2 = 10 I_B R_2 = 10 \times 20 \, \mu\text{A} \times R_2 \).
Step 3: Calculating the voltage at the collector.
The voltage at the collector is \( V_C = 6 \, \text{V} - V_{R_2} = 3 \, \text{V} \), so solving for \( R_2 \) and then \( R_1 \), we find the ratio \( \frac{R_1}{R_2} = 0.25 \).
Step 4: Conclusion.
Thus, the correct answer is option (B).