Abstract

Because of strong hydrogen bonding in liquid water, intermolecular interactions between water molecules are highly delocalized. Previous two-dimensional infrared spectroscopy experiments have indicated that this delocalization smears out the structural heterogeneity of neat H2O. Here we report on a systematic investigation of the ultrafast vibrational relaxation of bulk and interfacial water using time-resolved infrared and sum-frequency generation spectroscopies. These experiments reveal a remarkably strong dependence of the vibrational relaxation time on the frequency of the OH stretching vibration of liquid water in the bulk and at the air/water interface. For bulk water, the vibrational relaxation time increases continuously from 250 to 550 fs when the frequency is increased from 3,100 to 3,700 cm−1. For hydrogen-bonded water at the air/water interface, the frequency dependence is even stronger. These results directly demonstrate that liquid water possesses substantial structural heterogeneity, both in the bulk and at the surface.

Highlights

  • Because of strong hydrogen bonding in liquid water, intermolecular interactions between water molecules are highly delocalized

  • There is evidence from scattering experiments that liquid water exhibits substantial structural heterogeneity[3], the quantum nature of the hydrogen bond (H-bond), in particular for light water, results in significant delocalization of the intermolecular interaction[4,5], which may smear out the structural heterogeneity

  • It has remained elusive whether the extremely broad bandwidth of the OH stretching band is a sole result of the delocalized nature[11] and originates from strong intra- and intermolecular coupling[12] or that the delocalization occurs on a smaller length scale than the structural heterogeneity, which implies that the OH stretching band is inhomogeneously broadened

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Summary

Introduction

Because of strong hydrogen bonding in liquid water, intermolecular interactions between water molecules are highly delocalized. The signals recorded at oprobe 1⁄4 3,100 cm À 1 (Fig. 2b) directly reveal, at the interface, a pronounced frequency dependence of the vibrational relaxation dynamics: the transient signals decay with a time constant at 3,300 and o3f,t11001⁄4c(m35À0±1, 2r0e)spfsecatnivdel(y1.60F±or30t)hfes for excitation excitation at

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