In Young's double-slit experiment, light intensity through a slit is directly proportional to its width. Let the slit widths be \( w_1 \) and \( w_2 \). If one slit's width is half the other's, let \( w_1 = w \) and \( w_2 = 2w \). The intensities, \( I_1 \) and \( I_2 \), are proportional to these widths: \( I_1 \propto w_1 = w \implies I_1 = I_0 \) and \( I_2 \propto w_2 = 2w \implies I_2 = 2I_0 \). The maximum intensity \( I_{max} \) in the interference pattern, resulting from constructive interference, is \( I_{max} = (\sqrt{I_1} + \sqrt{I_2})^2 \). Substituting the intensity values yields: \( I_{max} = (\sqrt{I_0} + \sqrt{2I_0})^2 = (\sqrt{I_0} (1 + \sqrt{2}))^2 = I_0 (1 + \sqrt{2})^2 = I_0 (1 + 2 + 2\sqrt{2}) = I_0 (3 + 2\sqrt{2}) \). The minimum intensity \( I_{min} \), from destructive interference, is \( I_{min} = (\sqrt{I_1} - \sqrt{I_2})^2 \). Substituting the intensity values yields: \( I_{min} = (\sqrt{I_0} - \sqrt{2I_0})^2 = (\sqrt{I_0} (1 - \sqrt{2}))^2 = I_0 (1 - \sqrt{2})^2 = I_0 (1 + 2 - 2\sqrt{2}) = I_0 (3 - 2\sqrt{2}) \). The ratio of maximum to minimum intensity is \( \frac{I_{max}}{I_{min}} = \frac{I_0 (3 + 2\sqrt{2})}{I_0 (3 - 2\sqrt{2})} = \frac{3 + 2\sqrt{2}}{3 - 2\sqrt{2}} \). Therefore, the ratio \( I_{max} : I_{min} \) is \( (3 + 2\sqrt{2}) : (3 - 2\sqrt{2}) \).