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2019, Journal of Chemical Physics
Observing changes in molecular structure requires atomic-scale Ångstrom and femtosecond spatio-temporal resolution. We use the Fourier transform (FT) variant of laser-induced electron diffraction (LIED), FT-LIED, to directly retrieve the molecular structure of H2O + with picometre and femtosecond resolution without a priori knowledge of the molecular structure nor the use of retrieval algorithms or ab initio calculations. We identify a symmetrically stretched H2O + field-dressed structure that is most likely in the ground electronic state. We subsequently study the nuclear response of an isolated water molecule to an external laser field at four different field strengths. We show that upon increasing the laser field strength from 2.5 to 3.8 V/Å, the O-H bond is further stretched and the molecule slightly bends. The observed ultrafast structural changes lead to an increase in the dipole moment of water and, in turn, a stronger dipole interaction between the nuclear framework of the molecule and the intense laser field. Our results provide important insights into the coupling of the nuclear framework to a laser field as the molecular geometry of H2O + is altered in the presence of an external field. Water plays a crucial role in many physical, chemical and biological processes. In fact, modifying the geometric structure of water can, for example, influence the folding dynamics of proteins surrounded by water solvation shells. 2- 4 Such a modification of molecular structure can be accomplished by exposing molecules to strong fields with field strengths comparable to the Coulombic attraction between electrons and protons. Field-dressing the molecule can lead to a perturbation in its potential energy surfaces, and in turn could lead to a new energy minimum and possible modification of the equilibrium molecular structure on the nuclear (i.e. femtosecond; 1 fs = 10 -15 s) timescale. In fact, external fields with field strengths of around 0.5 V/Å have been theoretically reported to already cause structural changes in a water molecule. 5 Moreover, it is also reported that
The journal of physical chemistry letters, 2017
We combine classical and ring polymer molecular dynamics simulations with the molecular jump model to provide a molecular description of the nuclear quantum effects (NQEs) on water reorientation and hydrogen-bond dynamics in liquid H2O and D2O. We show that while the net NQE is negligible in D2O, it leads to a ∼13% acceleration in H2O dynamics compared to a classical description. Large angular jumps-exchanging hydrogen-bond partners-are the dominant reorientation pathway (just as in a classical description); the faster reorientation dynamics arise from the increased jump rate constant. NQEs do not change the jump amplitude distribution, and no significant tunneling is found. The faster jump dynamics are quantitatively related to decreased structuring of the OO radial distribution function when NQEs are included. This is explained, via a jump model analysis, by competition between the effects of water's librational and OH stretch mode zero-point energies on the hydrogen-bond stre...
The Journal of Physical Chemistry Letters, 2010
The molecular reorientation associated with the dynamics of the hydrogen-bond network in liquid water is investigated using quantum molecular dynamics simulations performed with the ab-initio-based TTM3-F interaction potential. The reorientation dynamics calculated at different temperatures are found to be in excellent agreement with the corresponding experimental results obtained from polarization-resolved, femtosecond mid-infrared, pump-probe spectroscopic measurements. A comparison with analogous results obtained from classical molecular dynamics simulations with the same interaction potential clearly indicates that the explicit inclusion of nuclear quantum effects is critical for reproducing the measured time dependence of the anisotropic signal.
Chemical Physics, 2013
Ionization and excitation of water molecules in intense laser pulses is studied theoretically by solving the threedimensional time-dependent electronic Schrödinger equation within the single-active-electron approximation. The possibility to image orbital densities by measurement of the orientation-dependent ionization of H 2 O in few-cycle, 800 nm linear-polarized laser pulses is investigated. While the highest-occupied molecular orbital 1 b 1 is found to dominate the overall ionization behavior, contributions from the energetically lower lying 3 a 1 orbital dominate the ionization yield in the nodal plane of the 1 b 1 orbital. The ratio of the ionization yields of the two orbitals depends on the intensity. Furthermore, even for laser pulses as long as 8 cycles the orientation-dependent ion yield depends on the carrier-envelope phase. In the interpretation of the orientation-dependent ionization as an imaging tool these effects have to be considered.
We outline a method to investigate the role of nuclear quantum effects in liquid water making use of a force field derived from ab initio simulations. Starting from a first-principles molecular dynamics simulation we obtain an effective force field for bulk liquid water using the force-matching technique. After validating that our effective model reproduces the key structural and dynamic properties of the reference system, we use it to perform path integral simulations to investigate the role played by nuclear quantum effects on bulk water, probing radial distribution functions, vibrational spectra and hydrogen bond fluctuations. Our approach offers a practical route to derive ab initio quality molecular models to study quantum effects at a low computational cost.
Proceedings of the National Academy of Sciences, 2013
The hydrogen bond is central to our understanding of the properties of water. Yet despite intense theoretical and experimental study, it continues to hold some surprises. Here we show, from an analysis of ab initio simulations that take proper account of nuclear quantum effects, that the hydrogen bonded protons in liquid water experience significant excursions in the direction of the acceptor oxygen atoms. This generates a small but non-negligible fraction of transient autoprotolysis events that are not seen in simulations with classical nuclei. These events are associated with major rearrangements of the electronic density, as revealed by an analysis of the computed Wannier centres and 1 H chemical shifts. We also show that the quantum fluctuations exhibit significant correlations between neighbouring hydrogen bonds, further enhancing the ephemeral shuttling of protons along water wires. We end by suggesting possible implications for our understanding of how perturbations (solvated ions, interfaces, confinement) might affect the hydrogen bond network in water.
Journal of Physical Chemistry A, 2007
An excitation of the OH-stretch ν OH of water has unique disruptive effects on the local hydrogen bonding. The disruption is not an immediate vibrational predissociation, which is frequently the case with hydrogenbonded clusters, but instead is a delayed disruption caused by a burst of energy from a vibrationally excited water molecule. The disruptive effects are the result of a fragile hydrogen-bonding network subjected to a large amount of vibrational energy released in a short time by the relaxation of ν OH stretching and δ H 2 O bending excitations. The energy of a single ν OH vibration distributed over one, two, or three (classical) water molecules would be enough to raise the local temperature to 1100, 700, or 570 K, respectively. Our understanding of the properties of the metastable water state having this excess energy in nearby hydrogen bonds, termed H 2 O*, has emerged as a result of experiments where a femtosecond IR pulse is used to pump ν OH , which is probed by either Raman or IR spectroscopy. These experiments show that the H 2 O* spectrum is blue-shifted and narrowed, and the spectrum looks very much like supercritical water at ∼600 K, which is consistent with the temperature estimates above. The H 2 O* is created within ∼400 fs after ν OH excitation, and it relaxes with an 0.8 ps lifetime by re-formation of the disrupted hydrogen-bond network. Vibrationally excited H 2 O* with one quantum of excitation in the stretching mode has the same 0.8 ps lifetime, suggesting it also relaxes by hydrogen-bond re-formation.
arXiv (Cornell University), 2018
Physical Review A, 2007
Proton ejection during Coulomb explosion is studied for several structure-related organic molecules ͑anthracene, anthraquinone, and octahydroanthracene͒ subjected to 800 nm, 60 fs laser pulses at intensities from 0.50 to 4.0ϫ 10 14 W cm −2 . The proton kinetic energy distributions are found to be markedly structure specific. The distributions are bimodal for anthracene and octahydroanthracene and trimodal for anthraquinone. Maximum ͑cutoff͒ energies of the distributions range from 50 eV for anthracene to 83 eV for anthraquinone. The lowenergy mode ͑ϳ10 eV͒ is most pronounced in octahydroanthracene. The dependence of the characteristic features of the distributions on the laser intensity provides insights into molecular specificity of such strongfield phenomena as ͑i͒ nonadiabatic charge localization and ͑ii͒ field-mediated restructuring of polyatomic molecules polarized by a strong laser field.
Physical Chemistry Chemical Physics, 2013
The angular anisotropy of fragments created in the dissociation of core-electron excited water molecules is studied to probe the correlation between fragmentation channels, kinematics and molecular geometry. We present fragment kinetic measurements for water molecules where the innershell oxygen electron is excited to the unoccupied 4a 1 and 2b 2 valence molecular orbitals. The kinematics of individual fragmentation channels are measured using fully three-dimensional momentum imaging of fragments. The results show that the geometry of the molecule and the kinetic energy of fragments are strongly coupled in the atomisation process. In addition we identify a fragmentation process arising from bond rearrangement evidenced by the H 2 + -O + ion pair which is accessible for resonant excitation of the 1s electron. In all of the two-body fragmentation processes the dissociation takes place along the potential-energy surface, while atomisation reveals both dissociation along the potential surface and Coulomb explosion. The angular distribution of fragments suggests that the bond rearrangement is very rapid; likely on a sub 10 fs time scale.
Faraday Discussions, 2013
We study the effects of ions and hydrophobic molecular groups on the orientational dynamics of water using THz dielectric relaxation (THz-DR) and polarization-resolved femtosecond infrared (fs-IR) pump-probe spectroscopy. We measure the dynamics of water in solutions of NaI, NaCl, CsCl, guanidinium chloride (GndCl) and tetramethyl guanidinium chloride (TMGndCl) of different concentrations. With THz-DR we observe that strongly hydrated cations align the static dipoles of their surrounding water molecules. With fs-IR we find that the OD groups that form hydrogen bonds to halide anions reorient with two distinct time constants of 2 AE 0.3 ps and 9 AE 1 ps. The fast process is assigned to a wobbling motion of the OD group that keeps the hydrogen bond with the anion intact. The amplitude of this wobbling motion depends on the nature of both the anion and the counter cation. The replacement of four of the six hydrogen atoms of the weakly hydrated cation guanidinium by hydrophobic methyl groups leads to an exceptionally strong slowing down of the water dynamics. Hydrophobic groups thus appear to have a much stronger effect on the dynamics of water than ions. These findings give new insights in the mechanism of protein denaturation by GndCl and TMGndCl.
Proceedings of the National Academy of Sciences, 2005
We present femtosecond midinfrared pump-probe measurements of the molecular motion and energy-transfer dynamics of a water molecule that is enclosed by acetone molecules. These confined water molecules show hydrogen-bond and orientational dynamics that are much slower than in bulk liquid water. This behavior is surprising because the hydrogen bonds to the CAO groups of the acetone molecules are weaker than the hydrogen bonds in bulk water. The energy transfer between the OOH groups of the confined water molecules has a time constant of 1.3 ؎ 0.2 ps, which is >20 times slower than in bulk water. We find that this energy transfer is governed completely by the rate at which hydrogen bonds are broken and reformed, and we identify the short-lived molecular complex that forms the transition state of this process. hydrogen bonding ͉ infrared pump-probe spectroscopy ͉ energy transfer W ater plays an essential role in many chemical and biological processes. Over the last decades, this notion has motivated a lot of work on the dynamical properties of bulk liquid water (1-7). However, the role of water in (bio)chemical processes is often played by a limited number of water molecules in a strongly restricted molecular environment. For example, the stability, structure, and biological function of proteins are largely determined by only a few surrounding layers of water molecules (8). When the water molecules participate directly in a reaction, the number of involved water molecules is even smaller. For example, the proton-pumping function of bacteriorhodopsin involves changes of the hydrogen network that is formed by particular amino acids of the protein and only a few confined water molecules (9-12). Recently, the dynamics of water in restricted environments was studied by comparing the spectral dynamics of an optically excited probe molecule embedded in a hydrated (bio)molecule with the spectral dynamics of the same probe molecule in bulk water (13). The spectral dynamics reflect the collective rearrangement of the solvating water, and were found to be much slower within the hydrated (bio)molecule than in bulk water. In this article, we present a study of the hydrogen-bond and energy-transfer dynamics of individual H 2 O and 1 H 2 HO molecules in a confined environment. In this study, we probed the dynamics of the water molecules directly with femtosecond midinfrared laser pulses that are resonant with the OOH stretch vibrations.
Angewandte Chemie International Edition, 2007
Accurate infrared spectroscopy of protonated water clusters that are prepared in the gas phase has become possible in recent years, thus opening the door to a deeper understanding of the properties of aqueous systems and the hydrated proton, which are of high interest in central areas of chemistry and biology. Several computational studies have appeared in parallel, providing a necessary theoretical basis for the assignment and understanding of the different spectral features. It has been recently demonstrated that the H 5 O 2 + motif, also referred to as the Zundel cation, plays an important role in protonated water clusters of six or more water molecules and, together with the Eigen cation (H 9 O 4 + ), as a limiting structure of the hydrated proton in bulk water. 11] The importance of the hydrated proton and the amount of work devoted to the problem contrast with the fact that the smallest system in which a proton is shared between water molecules, H 5 O 2 + , is not yet completely understood, and an explanation of the most important spectral signatures and the associated dynamics of the cluster is lacking.
1969
Part I Several approximate Hartree-Fock SCF wavefunctions for the ground electronic state of the water molecule have been obtained using an increasing number of multicenter s, p, and d Slater-type atomic orbitals as basis sets. The predicted charge distribution has been extensively tested at each stage by calculating the electric dipole moment, molecular quadrupole moment, diamagnetic shielding, Hellmann-Feynman forces, and electric field gradients at both the hydrogen and the oxygen nuclei. It was found that a carefully optimized minimal basis set suffices to describe the electronic charge distribution adequately except in the vicinity of the oxygen nucleus. Our calculations indicate, for example, that the correct prediction of the field gradient at this nucleus requires a more flexible linear combination of p-orbitals centered on this nucleus than that in the minimal basis set. Theoretical values for the molecular octopole moment components are also reported. Part II The perturbat...
This article is based on the master thesis (Ciftci 2014) related to our invention which is published in World Intellectual Property Organization (WO/2011/048506) as microwave water heater and the theoretical part of whole project. In this article, heating water by microwave (with steady frequency, 2.45 GHz) is analyzed from sub-molecular to Classical Mechanic results of heating. As the aim of this study, we wanted to examine Quantum Mechanical base of heating water by microwave experiments. As a result, we derived a Semi-Quantum Mechanical equation for microwave -water interactions and thus, Wien displacement law can be derived to verify experimental observations by this equation.
Journal of Mathematical Chemistry, 2005
A Gaussian function superposition is described in order to substitute the usual point charge approximation in molecular fixed frames. This procedure avoids the discontinuities at the nuclear positions which haunt first order density and EMP. Total first order density, made of the electronic and the Gaussian nuclear charge distributions, can be used to compute and compare molecular fields within quantum similarity techniques.
Chemical Reviews, 2010
Second-Harmonic Scatteringh (SHS) experiments provide a unique approach to probe non-centrosymmetric environments in aqueous media, from bulk solutions to interfaces, living cells and tissue. A central assumption made in analyzing SHS experiments is that the each molecule scatters light according to a constant molecular hyperpolarizability tensor β (2). Here, we investigate the dependence of the molecular hyperpolarizability of water on its environment and internal geometric distortions, in order to test the hypothesis of constant β (2). We use quantum chemistry calculations of the hyperpolarizability of a molecule embedded in point-charge environments obtained from simulations of bulk water. We demonstrate that both the heterogeneity of the solvent configurations and the quantum mechanical fluctuations of the molecular geometry introduce large variations in the non-linear optical response of water. This finding has the potential to change the way SHS experiments are interpreted: in particular, isotopic differences between H 2 O and D 2 O could explain recent SHG scattering observations. Finally, we show that a simple machine-learning framework can predict accurately the fluctuations of the molecular hyperpolarizability. This model accounts for the microscopic inhomogeneity of the solvent and represents a first step towards quantitative modelling of SHS experiments.
Nature Physics, 2010
1 At the transition from the gas to the liquid phase of water a wealth of new phenomena emerge, which are absent for isolated H 2 O molecules. Many of those are important for the existence of life, for astrophysics and atmospheric science. In particular the response to electronic excitation changes completely as more degrees of freedom become available. Here we report on the direct observation of an ultrafast transfer of energy across the hydrogen bridge in (H 2 O) 2 (a so called water dimer). This intermolecular Coulombic decay leads to an ejection of a low energy electron from the molecular neighbor of the initially excited molecule. We observe that this decay is faster than the proton transfer which is usually a prominent pathway in case of electronic excitation of small water clusters and leads to dissociation of the water dimer into two H 2 O + ions. As electrons of low energy (∼ 0.7 eV to 20 eV) have been recently found to efficiently breakup DNA-constituents [1, 2] the observed decay channel might contribute as a source for electrons that can cause radiation damage in biological matter.
Applied Physics B-lasers and Optics, 2004
We describe, using a semiclassical approach, the molecular dynamics of a one-dimensional H2 molecule interacting with a laser, beyond the Born–Oppenheimer approximation. We observe and discuss different molecular behaviors, such as ionization and dissociation.
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