To evaluate the normalization coefficient for the radial wavefunction of the hydrogen atom, the generating function for Laguerre polynomials can be utilized, as referenced in Pauling and Wilson's text. There is a discussion about the presence of a minus sign in the normalized wavefunction, with clarification that wavefunctions can be multiplied by a phase factor without affecting observables. The transformation of the function f(ρ) is explored, specifically replacing ρ with (2ρ) and incorporating a factor of (-1)^{2l+1}, which is connected to the associated Laguerre polynomial's properties. The confusion regarding the normalization coefficient and the Condon-Shortley phase factor is addressed, emphasizing that multiplying by constants not dependent on ρ is permissible. Understanding these aspects is crucial for accurately determining the shape and normalization of the wavefunction.