ABSTRACT
INTRODUCTION The structural and dynamic properties of bulk water are now mostly well understood in some ranges of temperatures and pressures. In particular, in many investigations using different techniques, such as X-ray diffraction, neutron scattering, nuclear magnetic resonance (NMR), differential scanning calorimetry (DSC), molecular dynamics (MD), and Monte Carlo (MC), simulations have been performed in the deeply supercooled regime (1-10), and in a situation where the effects due to the hydrogen bonding are dominant.
