23 research outputs found
The Role of Electrical Anharmonicity in the Association Band in the Water Spectrum
The origin of the intensity of the
feature in the spectrum of liquid
water near 2100 cm<sup>–1</sup> is investigated through calculations
of the spectra of water clusters based on low-order expansions of
the potential and dipole surfaces in internal and normal mode coordinates.
The intensity near 2100 cm<sup>–1</sup> is attributed to combination
bands involving the HOH bend and intermolecular vibrations that break
the hydrogen bonding network. Further, the leading contribution to
the intensity reflects large second derivatives of the dipole moment
with respect to the internal coordinates that are excited, or electrical
anharmonicity. This picture changes if the derivatives of the potential
and dipole surfaces are taken with respect to normal modes. In the
normal mode representation, the second derivatives of the dipole moment
are often vanishingly small, while the mixed third and fourth derivatives
of the potential become quite large. On the basis of this result,
mechanical anharmonicity appears to be responsible for the intensity
in the 2100 cm<sup>–1</sup> region. This strong dependence
of the interpretation of the origins of the intensity in the 2100
cm<sup>–1</sup> region of the water spectrum is investigated
and discussed
Investigation of the Structure and Spectroscopy of H<sub>5</sub><sup>+</sup> Using Diffusion Monte Carlo
The results of diffusion Monte Carlo
(DMC) calculations of the
ground and selected excited states of H<sub>5</sub><sup>+</sup> and its deuterated analogues are presented.
Comparisons are made between the results obtained from two recently
reported potential surfaces. Both of these surfaces are based on CCSDÂ(T)
electronic energies, but the fits display substantial differences
in the energies of low-lying stationary points. Little sensitivity
to these features is found in the DMC results, which yield zero-point
energies based on the two surfaces that differ by between 20 and 30
cm<sup>–1</sup> for all twelve isotopologues of H<sub>5</sub><sup>+</sup>. Likewise,
projections of the ground state probability amplitudes, evaluated
for the two surfaces, are virtually identical. By using the ground
state probability amplitudes, vibrationally averaged rotational constants
and dipole moments were calculated. On the basis of these calculations,
all isotopologues are shown to be near-prolate symmetric tops. Further,
in cases where the ion had a nonzero dipole moment, the magnitude
of the vibrationally averaged dipole moment was found to range from
0.33 to 1.15 D, which is comparable to the dipole moments of H<sub>2</sub>D<sup>+</sup> and HD<sub>2</sub><sup>+</sup>. Excited states with up to three quanta
in the shared proton stretch and one quantum in the in-phase stretch
of the outer H<sub>2</sub> groups were also investigated. Trends in
the energies and the properties of these states are discussed
Probing the Relationship Between Large-Amplitude Motions in H<sub>5</sub><sup>+</sup> and Proton Exchange Between H<sub>3</sub><sup>+</sup> and H<sub>2</sub>
Understanding the spectroscopy and
dynamics of H<sub>5</sub><sup>+</sup> is central in gaining insights
into the H<sub>3</sub><sup>+</sup> + H<sub>2</sub> → H<sub>5</sub><sup>+</sup> →
H<sub>2</sub> + H<sub>3</sub><sup>+</sup> proton transfer reaction.
This molecular ion exhibits large-amplitude vibrations, which allow
for the transfer of a proton between H<sub>3</sub><sup>+</sup> and
H<sub>2</sub> even in its ground vibrational state. With vibrational
excitation, the number of open channels for permutations of protons
increase. In this work, the minimized energy path variant of diffusion
Monte Carlo is used to investigate how the energetically accessible
proton permutations evolve as H<sub>5</sub><sup>+</sup> is dissociated
into H<sub>3</sub><sup>+</sup> + H<sub>2</sub>. Two mechanisms for
proton permutation are investigated. The first is the proton hop,
which correlates to large-amplitude vibrations of the central proton
in H<sub>5</sub><sup>+</sup>. The second is the exchange of a pair
of hydrogen atoms between H<sub>3</sub><sup>+</sup> and H<sub>2</sub>. This mechanism requires several proton hops along with a 120°
rotation of H<sub>3</sub><sup>+</sup> within the H<sub>5</sub><sup>+</sup> molecular ion. This analysis shows that while there is a
narrow region of configuration space over which both isomerization
processes are energetically accessible, full permutation of the five
protons in H<sub>5</sub><sup>+</sup> more likely occurs through a
stepwise mechanism. Such full permutation of the protons becomes accessible
when the shared proton stretch is excited to the <i>v</i><sub>pt</sub> = 2 or 3 excited state. The effects of deuteration
and rotational excitation of the H<sub>2</sub> and H<sub>3</sub><sup>+</sup> products are also investigated. Deuteration inhibits permutation
of protons, while rotational excitation has only a small impact on
these processes
Isotopic Effects on the Dynamics of the CH<sub>3</sub><sup>+</sup> + H<sub>2</sub> → CH<sub>5</sub><sup>+</sup> → CH<sub>3</sub><sup>+</sup> + H<sub>2</sub> Reaction
Diffusion Monte Carlo is used to investigate the anharmonic
zero-point
energy corrected energies for the CH<sub>3</sub><sup>+</sup> + H<sub>2</sub>→ CH<sub>5</sub><sup>+</sup> → CH<sub>3</sub><sup>+</sup> + H<sub>2</sub> process as a function of the center of mass separation of the two
fragments. In addition to the title reaction, all possible deuterated
and several tritiated (CH<sub>4</sub>T<sup>+</sup> and CH<sub>3</sub>T<sub>2</sub><sup>+</sup>) analogues
of this reaction are investigated. As anticipated, the replacement
of one or more of the hydrogen atoms with deuterium or tritium atoms
lowers the zero-point energy of the system. Further, in the partially
deuterated or tritiated isotopologues, the lowest energy configuration
generally has the heavy atoms in the CH<sub>3</sub><sup>+</sup> fragment. Analysis of the wave functions
allows us to study how zero-point energy influences the approach geometries
sampled during low-energy collisions between CH<sub>3</sub><sup>+</sup> and H<sub>2</sub>, and to gain
insights into how the dynamics is affected by the substitution of
heavier isotopes for one or more of the hydrogen atoms. Differences
between quantum and classical descriptions of the title reaction are
also discussed
Minimum Energy Path Diffusion Monte Carlo Approach for Investigating Anharmonic Quantum Effects: Applications to the CH<sub>3</sub><sup>+</sup> + H<sub>2</sub> Reaction
A method for evaluating anharmonic corrections to energies along a minimum energy path is developed and described. The approach is based upon the Diffusion Monte Carlo theory as initially developed by Anderson. Diffusion Monte Carlo has been shown to be effective for evaluating the ground-state properties of highly anharmonic systems. By using Jacobi coordinates, the evaluation of anharmonic corrections to the energies along a minimum energy path are straightforward to implement using Diffusion Monte Carlo. In this work, the CH<sub>3</sub><sup>+</sup> + H<sub>2</sub> → CH<sub>5</sub><sup>+</sup> reaction and its singly deuterated analogues are investigated. In addition to exploring how the energetics of this reaction change upon partial deuteration, projections of the probability amplitude onto various internal coordinates are evaluated and used to provide a quantum mechanical description of how deuteration affects the orientation of the two fragments as they combine to form the CH<sub>4</sub>D<sup>+</sup> molecular ion
Virtual Issue Highlighting Articles That Describe New Methodologies Soon To Be Considered for Publication in <i>JPC</i>
Virtual Issue Highlighting Articles That Describe
New Methodologies Soon To Be Considered for Publication in <i>JPC</i
Diffusion Monte Carlo in Internal Coordinates
An internal coordinate extension
of diffusion Monte Carlo (DMC)
is described as a first step toward a generalized reduced-dimensional
DMC approach. The method places no constraints on the choice of internal
coordinates other than the requirement that they all be independent.
Using H<sub>3</sub><sup>+</sup> and
its isotopologues as model systems, the methodology is shown to be
capable of successfully describing the ground state properties of
molecules that undergo large amplitude, zero-point vibrational motions.
Combining the approach developed here with the fixed-node approximation
allows vibrationally excited states to be treated. Analysis of the
ground state probability distribution is shown to provide important
insights into the set of internal coordinates that are less strongly
coupled and therefore more suitable for use as the nodal coordinates
for the fixed-node DMC calculations. In particular, the curvilinear
normal mode coordinates are found to provide reasonable nodal surfaces
for the fundamentals of H<sub>2</sub>D<sup>+</sup> and D<sub>2</sub>H<sup>+</sup> despite both molecules being highly fluxional
Rotation/Torsion Coupling in H<sub>5</sub><sup>+</sup>, D<sub>5</sub><sup>+</sup>, H<sub>4</sub>D<sup>+</sup>, and HD<sub>4</sub><sup>+</sup> Using Diffusion Monte Carlo
Two methods for studying the rotation/torsion
coupling in H<sub>5</sub><sup>+</sup> are described. The first involves
a fixed-node treatment in which the nodal surfaces are obtained from
a reduced dimensional calculation in which only the rotations of the
outer H<sub>2</sub> groups are considered. In the second, the torsion
and rotation dependence of the wave function is described in state
space, and the other internal coordinates are described in configuration
space. Such treatments are necessary for molecules, like H<sub>5</sub><sup>+</sup>, where there is a very low-energy barrier to internal
rotation. The results of the two approaches are found to be in good
agreement with previously reported energies for <i>J</i> = 0. The diffusion Monte Carlo treatment allows us to extend the
calculations to low <i>J</i>, and results are reported for
the three lowest energy torsion excited states with <i>J</i> ≤ 3. For the level of rotational and vibrational excitation
investigated, only modest changes in the vibrational wave functions
are found. The effects of deuteration are also investigated, focusing
on D<sub>5</sub><sup>+</sup> and the symmetric variants of H<sub>4</sub>D<sup>+</sup> and HD<sub>4</sub><sup>+</sup>
Dynamics of Small, Ultraviolet-Excited ICN<sup>–</sup> Cluster Anions
The ultraviolet (UV) photodissociation
of mass-selected ICN<sup>–</sup>Ar<sub><i>n</i></sub> and ICN<sup>–</sup>(CO<sub>2</sub>)<sub><i>n</i></sub> clusters (<i>n</i> = 0–5) is studied using
a secondary reflectron mass spectrometer.
Relative photodissociation cross sections of bare ICN<sup>–</sup> show the dominance of the I<sup>–</sup> photoproduct from
270 to 355 nm, the entire wavelength range studied. UV excitation
populates both the <sup>2</sup>Σ<sup>+</sup> state that produces
I* + CN<sup>–</sup> and the <sup>2</sup>Πstates that
produce I<sup>–</sup> + CN*. While the excited <sup>2</sup>Πstates directly produce I<sup>–</sup>, excitation
to the <sup>2</sup>Σ<sup>+</sup> state also produces some I<sup>–</sup> product via nonadiabatic transitions to the <sup>2</sup>Π<sub>1/2</sub> state, which produces I<sup>–</sup> +
CN. Partial solvation of the anion by Ar atoms or CO<sub>2</sub> molecules
alters the UV-branching percentages between the various dissociation
channels: I* + CN<sup>–</sup> and I<sup>–</sup> + CN
or I<sup>–</sup> + CN*. In addition, solvation by two or more
Ar atoms or three or more CO<sub>2</sub> molecules results in recombination,
reforming ICN<sup>–</sup>. Examination of the potential surfaces
and transition moments in combination with the results of quantum
dynamics calculations performed on the relevant excited states assist
in the analysis of the experimental results
Simultaneous Evaluation of Multiple Rotationally Excited States of H<sub>3</sub><sup>+</sup>, H<sub>3</sub>O<sup>+</sup>, and CH<sub>5</sub><sup>+</sup> Using Diffusion Monte Carlo
An
extension to diffusion Monte Carlo (DMC) is proposed for simultaneous
evaluation of multiple rotationally excited states of fluxional molecules.
The method employs an expansion of the rotational dependence of the
wave function in terms of the eigenstates of the symmetric top Hamiltonian.
Within this DMC approach, each walker has a separate rotational state
vector for each rotational state of interest. The values of the coefficients
in the expansion of the rotational state vector associated with each
walker, as well as the locations of the walkers, evolve in imaginary
time under the action of a propagator based on the imaginary-time
time-dependent Schrödinger equation. The approach is first
applied to H<sub>3</sub><sup>+</sup>, H<sub>2</sub>D<sup>+</sup>, and H<sub>3</sub>O<sup>+</sup> for
which the calculated energies can be compared to benchmark values.
For low to moderate values of <i>J</i> the DMC results are
found to be accurate to within the evaluated statistical uncertainty.
The rotational dependence of the vibrational part of the wave function
is also investigated, and significant rotation–vibration interaction
is observed. Based on the successful application of this approach
to H<sub>3</sub><sup>+</sup>,
H<sub>2</sub>D<sup>+</sup>, and H<sub>3</sub>O<sup>+</sup>, the method
was applied to calculations of the rotational energies and wave functions
for CH<sub>5</sub><sup>+</sup> with <i>v</i> = 0 and <i>J</i> ≤ 10.
Based on these calculations, the rotational energy progression is
shown to be consistent with that for a nearly spherical top molecule,
and little evidence of rotation–vibration interaction is found
in the vibrational wave function