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Description
How water behaves at interfaces is relevant to many scientific and technological applications; however, many subtle phenomena are unknown in aqueous solutions. In this work, interfacial structural transition in hydration shells of a polarizable solute at critical polarizabilities is discovered. The transition is manifested in maximum water response, the reorientation

How water behaves at interfaces is relevant to many scientific and technological applications; however, many subtle phenomena are unknown in aqueous solutions. In this work, interfacial structural transition in hydration shells of a polarizable solute at critical polarizabilities is discovered. The transition is manifested in maximum water response, the reorientation of the water dipoles at the interface, and an increase in the density of dangling OH bonds. This work also addresses the role of polarizability of the active site of proteins in biological catalytic reactions. For proteins, the hydration shell becomes very heterogeneous and involves a relatively large number of water molecules. The molecular dynamics simulations show that the polarizability, along with the atomic charge distribution, needs to be a part of the picture describing how enzymes work. Non Gaussian dynamics in time-resolved linear and nonlinear (correlation) 2D spectra are also analyzed.



Additionally, a theoretical formalism is presented to show that when preferential orientations of water dipoles exist at the interface, electrophoretic charges can be produced without free charge carriers, i.e., neutral solutes can move in a constant electric field due to the divergence of polarization at the interface. Furthermore, the concept of interface susceptibility is introduced. It involves the fluctuations of the surface charge density caused by thermal motion and its correlation over the characteristic correlation length with the fluctuations of the solvent charge density. Solvation free energy and interface dielectric constant are formulated accordingly. Unlike previous approaches, the solvation free energy scales quite well in a broad range of ion sizes, namely in the range of 2-14 A° . Interface dielectric constant is defined such that the boundary conditions in the Laplace equation describing a micro- or mesoscopic interface are satisfied. The effective dielectric constant of interfacial water is found to be significantly lower than its bulk value. Molecular dynamics simulation results show that the interface dielectric constant for a TIP3P water model changes from nine to four when the effective solute radius is increased from 5 A° to 18 A° . The small value of the interface dielectric constant of water has potentially dramatic consequences for hydration.
ContributorsDinpajooh, Mohammadhasan (Author) / Matyushov, Dmitry V (Thesis advisor) / Richert, Ranko (Committee member) / Beckstein, Oliver (Committee member) / Arizona State University (Publisher)
Created2016
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Description
The bonding and electrostatic properties of gold containing molecules are highly influenced by relativistic effects. To understand this facet on bonding, a series of simple diatomic AuX (X=F, Cl, O and S) molecules, where upon bond formation the Au atom donates or accepts electrons, was investigated and discussed in this

The bonding and electrostatic properties of gold containing molecules are highly influenced by relativistic effects. To understand this facet on bonding, a series of simple diatomic AuX (X=F, Cl, O and S) molecules, where upon bond formation the Au atom donates or accepts electrons, was investigated and discussed in this thesis.

First, the optical field-free, Stark, and Zeeman spectroscopic studies have been performed on AuF and AuCl. The simple polar bonds between Au and typical halogens (i.e. F and Cl) can be well characterized by the electronic structure studies and the permanent electric dipole moments, el. The spectroscopic parameters have been precisely determined for the [17.7]1, [17.8]0+ and X1+ states of AuF, and the [17.07]1, [17.20]0+ and X1+ states of AuCl. The el have been determined for ground and excited states of AuF and AuCl. The results from the hyperfine analysis and Stark measurement support the assignments that the [17.7]1 and [17.8]0+ states of AuF are the components of a 3 state. Similarly, the analysis demonstrated the [19.07]1 and [19.20]0+ states are the components of the 3 state of AuCl.

Second, my study focused on AuO and AuS because the bonding between gold and sulfur/oxygen is a key component to numerous established and emerging technologies that have applications as far ranging as medical imaging, catalysis, electronics, and material science. The high-resolution spectra were record and analyzed to obtain the geometric and electronic structural data for the ground and excited states. The electric dipole moment, el, and the magnetic dipole moment, m, has been the precisely measured by applying external static electric and magnetic fields. el andm are used to give insight into the unusual complex bonding in these molecules.

In addition to direct studies on the gold-containing molecules, other studies of related molecules are included here as well. These works contain the pure rotation measurement of PtC, the hyperfine and Stark spectroscopic studies of PtF, and the Stark and Zeeman spectroscopic studies of MgH and MgD.

Finally, a perspective discussion and conclusion will summarize the results of AuF, AuCl, AuO, and AuS from this work (bond lengths, dipole moment, etc.). The highly quantitative information derived from this work is the foundation of a chemical description of matter and essential for kinetic energy manipulation via Stark and Zeeman interactions. This data set also establishes a synergism with computation chemists who are developing new methodologies for treating relativistic effects and electron correlation.
ContributorsZhang, Ruohan (Author) / Steimle, Timothy C. (Thesis advisor) / Williams, Peter (Committee member) / Richert, Ranko (Committee member) / Arizona State University (Publisher)
Created2017
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Description
We studied the relationship between the polarizability and the molecular conductance

that arises in the response of a molecule to an external electric field. To illustrate

the plausibility of the idea, we used Simmons' tunneling model, which describes image

charge and dielectric effects on electron transport through a barrier. In such a

model, the

We studied the relationship between the polarizability and the molecular conductance

that arises in the response of a molecule to an external electric field. To illustrate

the plausibility of the idea, we used Simmons' tunneling model, which describes image

charge and dielectric effects on electron transport through a barrier. In such a

model, the barrier height depends on the dielectric constant of the electrode-molecule-electrode junction, which in turn can be approximately expressed in terms of the

molecular polarizability via the classical Clausius-Mossotti relation. In addition to

using the tunneling model, the validity of the relationships between the molecular

polarizability and the molecular conductance was tested by comparing calculated

and experimentally measured conductance of different chemical structures ranging

from covalent bonded to non-covalent bonded systems. We found that either using

the tunneling model or the first-principle calculated quantities or experimental data,

the conductance decreases as the molecular polarizability increases. In contrast to

this strong correlation, our results showed that in some cases there was a weaker or

none correlation between the conductance and other molecular electronic properties

including HOMO-LUMO gap, chemical geometries, and interactions energies. All

these results together suggest that using the molecular polarizability as a molecular

descriptor for conductance can offer some advantages compared to using other

molecular electronic properties and can give additional insight about the electronic

transport property of a junction.

These results also show the validity of the physically intuitive picture that to a first

approximation a molecule in a junction behaves as a dielectric that is polarized in the

opposite sense of the applied bias, thereby creating an interfacial barrier that hampers

tunneling. The use of the polarizability as a descriptor of molecular conductance offers

signicant conceptual and practical advantages over a picture based in molecular

orbitals. Despite the simplicity of our model, it sheds light on a hitherto neglected

connection between molecular polarizability and conductance and paves the way for

further conceptual and theoretical developments.

The results of this work was sent to two publications. One of them was accepted

in the International Journal of Nanotechnology (IJNT) and the other is still under

review in the Journal of Physical Chemistry C.
ContributorsVatan Meidanshahi, Reza (Author) / Mujica, Vladimiro (Thesis advisor) / Chizmeshya, Andrew (Committee member) / Richert, Ranko (Committee member) / Arizona State University (Publisher)
Created2014