The temperature is inversely proportional to the square root of the atomic mass:
"T_1=\\frac k{\\sqrt{m_{a1}}},\\\\\\space\\\\\nT_2=\\frac k{\\sqrt{m_{a2}}},\\\\\\space\\\\\n\\frac{T_1}{T_2}=\\sqrt{\\frac{m_{a2}}{m_{a1}}},\\\\\\space\\\\\nT_2=T_1\\sqrt{\\frac{m_{a1}}{m_{a2}}}=4.14\\text{ K}."
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