In order to improve the experimental database about the additional nonrotational broadening of vibrational line shapes observable when a simple fluid approaches its gas-liquid critical point, we improved the pioneering measurements of Clouter and Kiefte [for their own review see Phys. Rev. A 33, 2749 (1986)] on the critical behavior of the polarized Raman line of fluid nitrogen by using the isotopic mixture (N-14(2))(.975)-((NN)-N-14-N-15)(.025), giving special attention to the fact that the isotropic line shape of liquid N-2 ((ν) over tilde approximate to2327 cm(-1)) is affected by intermolecular vibrational resonance couplings. Using a highest-resolution double monochromator and modern CCD detection techniques, we were able to follow the temperature dependencies of the line shape parameters (i.e., shift, width, and asymmetry) of the coupled N-14(2) and, depending on the S/N ratio available, of the uncoupled (NN)-N-14-N-15 in the range 45 Kless than or similar toTless than or similar to300 K with up to mK resolution (1) in the beta-solid phase, (2) in the coexisting liquid and gas phases, and (3) along the critical isochore. Comparing the line shifts of both isotopic species, clear evidence was found that vibrational resonance couplings are present in all dense phases studied, the line position (ν) over tilde (0) being more density than temperature dependent. Additionally, the existence of (negative) cross correlations between resonant and nonresonant dephasing mechanisms has been confirmed by the change in sign observed for the small but non-negligible difference in the linewidths between coupled N-14(2) and uncoupled (NN)-N-14-N-15 around 90 K. The lambda-shaped dependencies of the width parameters, observed when moving along the coexistence line through the critical point, T-crit=126.192 K, and along the critical isochore, is much more evident in the line asymmetry than in the usually considered linewidth. Clear proof was found that, in accordance with theoretical predictions, the linewidth converges to a constant maximum value regardless if the critical point is reached along the coexistence line or along the critical isochore, i.e., it does not diverge approaching the critical temperature up to our closest value \T/T-crit-1\approximate to10(-5).