The de Broglie wavelength associated with an electron accelerated through a potential difference V is \lambda_{\mathrm{e}} and the de Broglie wavelength associated with a proton accelerated through the same potential difference is \lambda_{\mathrm{p}}. If their corresponding masses are m_{\mathrm{e}} and m_{\mathrm{p}}, respectively, then the ratio of their de Broglie wavelengths \left(\frac{\lambda_e}{\lambda_p}\right) is \_\_\_\_ .