According to Snell's Law, "\\frac{sin \\theta_1}{\\sin \\theta_2} = \\frac{n_2}{n_1} = \\frac{\\lambda_1}{\\lambda_2}", where n is a refractive index and "\\lambda" is the wavelength. When passing from medium A into B, wavelength changes from "\\lambda_1" to "(1-\\eta)\\lambda_1", therefore "\\frac{n_2}{n_1}= \\frac{\\lambda_1}{(1-\\eta)\\lambda_1} = \\frac{1}{1-\\eta}". Substituting "\\eta = 0.22", obtain "\\frac{n_2}{n_1} \\approx 1.282".
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