By confining water in a nanoporous structure so narrow that the liquid could not freeze, it is possible to study properties of this previously undescribed system well below its homogeneous nucleation temperature T H ؍ 231 K. Using this trick, we were able to study, by means of a Fourier transform infrared spectroscopy, vibrational spectra (HOH bending and OH-stretching modes) of deeply supercooled water in the temperature range 183 < T < 273 K. We observed, upon decreasing temperature, the building up of a new population of hydrogen-bonded oscillators centered around 3,120 cm ؊1 , the contribution of which progressively dominates the spectra as one enters into the deeply supercooled regime. We determined that the fractional weight of this spectral component reaches 50% just at the temperature, T L Ϸ 225 K, where the confined water shows a fragile-to-strong dynamic cross-over phenomenon dynamic cross-over in water ͉ dynamic transitions in water ͉ Fourier transform infrared spectroscopy ͉ low-density liquid water ͉ Widom line in water W ater plays a fundamental and ubiquitous role on Earth and in all aspects of life phenomena. Understanding its properties is of paramount importance to mankind, and thus water is the most studied molecular system in science and technology. However, despite intense scrutiny over the years, scientists are still far from reaching a coherent understanding of all its unusual properties (1-3). Instead of behaving like other simple molecular liquids, many thermodynamic response functions of water, such as the isothermal compressibility, isobaric heat capacity, and thermal expansion coefficient, display counterintuitive trends as temperature is lowered. In particular, extrapolated from their values at moderately supercooled states, these functions all appear to diverge at a singular temperature around T S ϭ 228 K. Over the years, many plausible explanations for these strange behaviors have been proposed, starting from the two-state and the clathrate models (1-3). Three hypotheses are of active interest: (i) the stability limit (4), (ii) the percolation (5), and (iii) liquid-liquid (LL) critical point (6). The third approach has received support from various theoretical studies (7-9). However, in all three approaches, the main role is played by the local hydrogen-bond (HB) interaction pattern surrounding a typical water molecule in liquid state that governs the overall structure and dynamics (1) of water. Some of our recent experimental results (10, 11) on water confined in nanoporous structures as a function of temperature and pressure showed that the theoretical approach based on existence of the LL critical point is able to describe coherently many strange properties of water. By using the neutronscattering technique, we obtained evidence of the LL critical point (the second critical point predicted by the theory to be at T C ϳ 220 K and P C ϳ 1 kbar) located at T C ϭ 200 K and P C ϭ 1.5 kbar (10). This result was also subsequently confirmed qualitatively by an extensive molecular dynam...