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21 Nov 2009

Volume 131, Issue 19, Articles (19xxxx)

Issue Cover Spotlight Figure

J. Chem. Phys. 131, 194701 (2009); http://dx.doi.org/10.1063/1.3257621 (10 pages)

Peter L. Cook, Xiaosong Liu, Wanli Yang, and F. J. Himpsel
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back to top Theoretical Methods and Algorithms

An optimized full-configuration-interaction nuclear orbital approach to a “hard-core” interaction problem: Application to (3He)N–Cl2(B) clusters (N ≤ 4)

M. P. de Lara-Castells, P. Villarreal, G. Delgado-Barrio, and A. O. Mitrushchenkov

J. Chem. Phys. 131, 194101 (2009); http://dx.doi.org/10.1063/1.3263016 (13 pages) | Cited 7 times

Online Publication Date: 16 November 2009

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An efficient full-configuration-interaction nuclear orbital treatment has been recently developed as a benchmark quantum-chemistry-like method to calculate ground and excited “solvent” energies and wave functions in small doped ΔEest clusters (N ≤ 4) [ M. P. de Lara-Castells, G. Delgado-Barrio, P. Villarreal, and A. O. Mitrushchenkov, J. Chem. Phys. 125, 221101 (2006) ]. Additional methodological and computational details of the implementation, which uses an iterative Jacobi–Davidson diagonalization algorithm to properly address the inherent “hard-core” He–He interaction problem, are described here. The convergence of total energies, average pair He–He interaction energies, and relevant one- and two-body properties upon increasing the angular part of the one-particle basis set (expanded in spherical harmonics) has been analyzed, considering Cl2 as the dopant and a semiempirical model (T-shaped) He–Cl2(B) potential. Converged results are used to analyze global energetic and structural aspects as well as the configuration makeup of the wave functions, associated with the ground and low-lying “solvent” excited states. Our study reveals that besides the fermionic nature of 3He atoms, key roles in determining total binding energies and wave-function structures are played by the strong repulsive core of the He–He potential as well as its very weak attractive region, the most stable arrangement somehow departing from the one of N He atoms equally spaced on equatorial “ring” around the dopant. The present results for N = 4 fermions indicates the structural “pairing” of two 3He atoms at opposite sides on a broad “belt” around the dopant, executing a sort of asymmetric umbrella motion. This pairing is a compromise between maximizing the 3He–3He and the He-dopant attractions, and suppressing at the same time the “hard-core” repulsion. Although the He–He attractive interaction is rather weak, its contribution to the total energy is found to scale as a power of three and it thus increasingly affects the pair density distributions as the cluster grows in size.
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36.40.Mr Spectroscopy and geometrical structure of clusters
31.15.V- Electron correlation calculations for atoms, ions and molecules
33.15.Mt Rotation, vibration, and vibration-rotation constants
34.20.Gj Intermolecular and atom-molecule potentials and forces

Stability of binary mixtures in electric field gradients

Sela Samin and Yoav Tsori

J. Chem. Phys. 131, 194102 (2009); http://dx.doi.org/10.1063/1.3257688 (9 pages) | Cited 1 time

Online Publication Date: 17 November 2009

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We consider the influence of electric field gradients on the phase behavior of nonpolar binary mixtures. Small fields give rise to smooth composition profiles, whereas large enough fields lead to a phase-separation transition. The critical field for demixing as well as the equilibrium phase-separation interface are given as a function of the various system parameters. We show how the phase diagram in the temperature-composition plane is affected by electric fields, assuming a linear or nonlinear constitutive relations for the dielectric constant. Finally, we discuss the unusual case where the interface appears far from any bounding surface.
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64.75.Ef Mixing
61.20.-p Structure of liquids
77.22.Ch Permittivity (dielectric function)
64.75.Cd Phase equilibria of fluid mixtures, including gases, hydrates, etc.

Efficient calculation of the polarization induced by N coherent laser pulses

Maxim F. Gelin, Dassia Egorova, and Wolfgang Domcke

J. Chem. Phys. 131, 194103 (2009); http://dx.doi.org/10.1063/1.3265213 (6 pages) | Cited 2 times

Online Publication Date: 18 November 2009

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We have developed a novel method, the equation-of-motion phase-matching approach (EOM-PMA), for the calculation of the response of a quantum system to N coherent laser fields. The N-pulse EOM-PMA is limited to weak fields (its domain of validity is equivalent to the traditional nonlinear response functions approach), but allows for arbitrary pulse durations and automatically accounts for pulse-overlap effects. The N-pulse EOM-PMA allows the evaluation of the time evolution of the N-pulse-induced polarization in any phase-matching direction by performing 2N−1 independent propagations of certain auxiliary density matrices. The N-pulse EOM-PMA can straightforwardly be incorporated into codes which provide the time evolution of the density matrix of material systems of interest and can efficiently be implemented on parallel computers.
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33.80.-b Photon interactions with molecules
42.65.Jx Beam trapping, self-focusing and defocusing; self-phase modulation
33.15.Kr Electric and magnetic moments (and derivatives), polarizability, and magnetic susceptibility

Excited and ionized states of the ozone molecule with full triples coupled cluster methods

Monika Musiał, Stanisław A. Kucharski, Piotr Zerzucha, Tomasz Kuś, and Rodney J. Bartlett

J. Chem. Phys. 131, 194104 (2009); http://dx.doi.org/10.1063/1.3265770 (10 pages) | Cited 3 times

Online Publication Date: 20 November 2009

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The role of connected triple excitations in coupled cluster (CC) calculations of vertical excitation energies, ionization potentials, and the electron affinity of the ozone molecule is evaluated. The equation of motion (EOM) and Fock space (FS) multireference CC approaches with full triples have been used in the calculations. The effect of the T3 and R3 operators significantly improve the EOM CCSD results for all considered quantities. A similar behavior is observed in the case of the FS-CC calculations. The FS-CC calculations with full triples have been obtained only for the intermediate Hamiltonian realization of the FS approach as the standard formulation diverges. The latter results are rigorously linked, and less expensive since smaller matrices are diagonalized.
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31.15.bw Coupled-cluster theory
33.15.Ry Ionization potentials, electron affinities, molecular core binding energy

Extrapolating MP2 and CCSD explicitly correlated correlation energies to the complete basis set limit with first and second row correlation consistent basis sets

J. Grant Hill, Kirk A. Peterson, Gerald Knizia, and Hans-Joachim Werner

J. Chem. Phys. 131, 194105 (2009); http://dx.doi.org/10.1063/1.3265857 (13 pages) | Cited 26 times

Online Publication Date: 20 November 2009

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Accurate extrapolation to the complete basis set (CBS) limit of valence correlation energies calculated with explicitly correlated MP2-F12 and CCSD(T)-F12b methods have been investigated using a Schwenke-style approach for molecules containing both first and second row atoms. Extrapolation coefficients that are optimal for molecular systems containing first row elements differ from those optimized for second row analogs, hence values optimized for a combined set of first and second row systems are also presented. The new coefficients are shown to produce excellent results in both Schwenke-style and equivalent power-law-based two-point CBS extrapolations, with the MP2-F12/cc-pV(D,T)Z-F12 extrapolations producing an average error of just 0.17 mEh with a maximum error of 0.49 for a collection of 23 small molecules. The use of larger basis sets, i.e., cc-pV(T,Q)Z-F12 and aug-cc-pV(Q,5)Z, in extrapolations of the MP2-F12 correlation energy leads to average errors that are smaller than the degree of confidence in the reference data ( ∼ 0.1 mEh). The latter were obtained through use of very large basis sets in MP2-F12 calculations on small molecules containing both first and second row elements. CBS limits obtained from optimized coefficients for conventional MP2 are only comparable to the accuracy of the MP2-F12/cc-pV(D,T)Z-F12 extrapolation when the aug-cc-pV(5+d)Z and aug-cc-pV(6+d)Z basis sets are used. The CCSD(T)-F12b correlation energy is extrapolated as two distinct parts: CCSD-F12b and (T). While the CCSD-F12b extrapolations with smaller basis sets are statistically less accurate than those of the MP2-F12 correlation energies, this is presumably due to the slower basis set convergence of the CCSD-F12b method compared to MP2-F12. The use of larger basis sets in the CCSD-F12b extrapolations produces correlation energies with accuracies exceeding the confidence in the reference data (also obtained in large basis set F12 calculations). It is demonstrated that the use of the 3C(D) Ansatz is preferred for MP2-F12 CBS extrapolations. Optimal values of the geminal Slater exponent are presented for the diagonal, fixed amplitude Ansatz in MP2-F12 calculations, and these are also recommended for CCSD-F12b calculations.
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31.15.bw Coupled-cluster theory
31.15.vn Electron correlation calculations for diatomic molecules
31.15.xp Perturbation theory
back to top Gas Phase Dynamics and Structure: Spectroscopy, Molecular Interactions, Scattering, and Photochemistry

Laser spectroscopy of NiI: New electronic states and hyperfine structure

A. S.-C. Cheung, H. F. Pang, W. S. Tam, and J. W.-H. Leung

J. Chem. Phys. 131, 194301 (2009); http://dx.doi.org/10.1063/1.3262715 (7 pages)

Online Publication Date: 16 November 2009

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Two new electronic transition systems, namely, the [14.0]2Φ7/2-Χ 2Δ5/2 and the [15.7]2Φ5/2-Χ 2Δ5/2 transitions were observed and analyzed using laser vaporization/reaction supersonic free jet expansion and high resolution laser induced fluorescence spectroscopy. In addition, the (v, 0) bands with v = 6–10 of the [14.6]2Δ5/2-Χ 2Δ5/2 transition were found to be perturbed by the [15.7]2Φ5/2 state. The interaction between the [14.6]2Δ5/2 and the [15.7]2Φ5/2 states is evident in the progressive increase in hyperfine width of rotational lines of the [14.6]2Δ5/2-X 2Δ5/2 transition as the vibrational quantum number increases. Deperturbation procedures were successfully applied to analyze the interaction between these two states. All observed spectra show partially resolved hyperfine structure, and the hyperfine width decreases rapidly as J increases suggested that the hyperfine structure conforms to the Hund’s case aβ coupling scheme. Accurate molecular and hyperfine constants for the [14.0]2Φ7/2, the [14.6]2Δ5/2 and the [15.7]2Φ5/2 states were obtained and analyzed.
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33.15.Pw Fine and hyperfine structure
33.50.Dq Fluorescence and phosphorescence spectra
33.15.Mt Rotation, vibration, and vibration-rotation constants
33.20.Tp Vibrational analysis
33.80.-b Photon interactions with molecules
31.50.Df Potential energy surfaces for excited electronic states

Electronic relaxation dynamics in large anionic water clusters: (H2O)n− and (D2O)n− (n = 25–200)

Graham B. Griffin, Ryan M. Young, Oli T. Ehrler, and Daniel M. Neumark

J. Chem. Phys. 131, 194302 (2009); http://dx.doi.org/10.1063/1.3263419 (9 pages) | Cited 10 times

Online Publication Date: 16 November 2009

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Electronic relaxation dynamics subsequent to s→p excitation of the excess electron in large anionic water clusters, (H2O)n− and (D2O)n− with 25 ≤ n ≤ 200, were investigated using time-resolved photoelectron imaging. Experimental improvements have enabled considerably larger clusters to be probed than in previous work, and the temporal resolution of the instrument has been improved. New trends are seen in the size-dependent p-state lifetimes for clusters with n ≥ 70, suggesting a significant change in the electron-water interaction for clusters in this size range. Extrapolating the results for these larger clusters to the infinite-size limit yields internal conversion lifetimes τIC of 60 and 160 fs for electrons dissolved in H2O and D2O, respectively. In addition, the time-evolving spectra show evidence for solvent relaxation in the excited electronic state prior to internal conversion and in the ground state subsequent to internal conversion. Relaxation in the excited state appears to occur on a time scale similar to that of internal conversion, while ground state solvent dynamics occur on a ∼ 1 ps time scale, in reasonable agreement with previous measurements on water cluster anions and electrons solvated in liquid water.
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36.40.Mr Spectroscopy and geometrical structure of clusters
36.40.Sx Diffusion and dynamics of clusters
33.60.+q Photoelectron spectra
33.50.Hv Radiationless transitions, quenching
33.70.Ca Oscillator and band strengths, lifetimes, transition moments, and Franck-Condon factors
31.70.Dk Environmental and solvent effects

Multiconfiguration time-dependent Hartree and classical dynamics studies of the photodissociation of HF and HCl molecules adsorbed on ice: Extension to three dimensions

S. Woittequand, C. Toubin, M. Monnerville, S. Briquez, B. Pouilly, and H.-D. Meyer

J. Chem. Phys. 131, 194303 (2009); http://dx.doi.org/10.1063/1.3263605 (8 pages) | Cited 1 time

Online Publication Date: 17 November 2009

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The 3D photodissociation dynamics of HCl and HF molecules adsorbed on ice is studied by quantum and classical simulations. The quantum calculations are carried out with the multiconfiguration time-dependent Hartree (MCTDH) approach. Dynamical observables like angular distributions in the momentum space of the H fragments, absorption cross sections are computed. The results are compared with our previous 2D studies. As expected, less encapsulation of the H atom between the ice surface and the halogen atom is obtained in the 3D study, resulting in less pronounced interference structures in the photoabsorption cross sections and in a decrease of the classical rainbow peaks observed in the 2D scheme. Although the amplitudes of the oscillations corresponding to quantum interferences in the asymptotic angular distribution of the H fragment are different between the 2D and 3D results, the qualitative pattern of the oscillations is similar in the 2D and 3D approaches. In addition, a good agreement is observed for the angular distribution between the classical and the quantum calculations.
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33.80.Gj Diffuse spectra; predissociation, photodissociation
31.15.xr Self-consistent-field methods

Unimolecular decomposition of tetrazine-N-oxide based high nitrogen content energetic materials from excited electronic states

A. Bhattacharya, Y. Q. Guo, and E. R. Bernstein

J. Chem. Phys. 131, 194304 (2009); http://dx.doi.org/10.1063/1.3262688 (8 pages) | Cited 3 times

Online Publication Date: 18 November 2009

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Unimolecular excited electronic state decomposition of novel high nitrogen content energetic molecules, such as 3,3′-azobis(6-amino-1,2,4,5-tetrazine)-mixed N-oxides (DAATO3.5), 3-amino-6-chloro-1,2,4,5-tetrazine-2,4-dioxide (ACTO), and 3,6-diamino-1,2,4,5-tetrazine-1,4-dioxde (DATO), is investigated. Although these molecules are based on N-oxides of a tetrazine aromatic heterocyclic ring, their decomposition behavior distinctly differs from that of bare tetrazine, in which N2 and HCN are produced as decomposition products through a concerted dissociation mechanism. NO is observed to be an initial decomposition product from all tetrazine-N-oxide based molecules from their low lying excited electronic states. The NO product from DAATO3.5 and ACTO is rotationally cold (20 K) and vibrationally hot (1200 K), while the NO product from DATO is rotationally hot (50 K) and vibrationally cold [only the (0–0) vibronic transition of NO is observed]. DAATO3.5 and ACTO primarily differ from DATO with regard to molecular structure, by the relative position of oxygen atom attachment to the tetrazine ring. Therefore, the relative position of oxygen in tetrazine-N-oxides is proposed to play an important role in their energetic behavior. N2O is ruled out as an intermediate precursor of the NO product observed from all three molecules. Theoretical calculations at CASMP2/CASSCF level of theory predict a ring contraction mechanism for generation of the initial NO product from these molecules. The ring contraction occurs through an (S1/S0)CI conical intersection.
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82.30.Lp Decomposition reactions (pyrolysis, dissociation, and fragmentation)
82.20.Hf Product distribution

Reactions of simple aromatic heterocycles with niobium cluster ions (n ≤ 30)

Britta Pfeffer, Stephanie Jaberg, and Gereon Niedner-Schatteburg

J. Chem. Phys. 131, 194305 (2009); http://dx.doi.org/10.1063/1.3264575 (12 pages) | Cited 2 times

Online Publication Date: 19 November 2009

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Prior work on benzene activation by size selected niobium cluster cations and anions of up to 30 atoms is extended systematically through studying aromatic poly- and heterocyclic molecules such as naphthalene, pyridine, thiophene, pyrrole, furan, and benzofuran. Naphthalene is found to act much like benzene when reacting under single collision conditions with individual clusters. The most likely process is carbidization through complete dehydrogenation. Some clusters of particular sizes (most notably n = 19) fail to activate both homocyclic molecules. Instead seemingly intact adsorption is observed which proves that activation is kinetically hindered at some point. All of the five studied heterocyclic aromatic molecules react unconditionally and by complete dehydrogenation with cationic niobium clusters, while they only attach to or react with anionic clusters larger than a minimum size of n = 19–21. These findings are taken as strong evidence for initial coordination to the metal clusters of the heterocycles through their lone pair orbitals. The paper comprehends the observations in terms of cluster surface structure and reactivity.
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82.30.Cf Atom and radical reactions; chain reactions; molecule-molecule reactions
82.65.+r Surface and interface chemistry; heterogeneous catalysis at surfaces
68.35.B- Structure of clean surfaces (and surface reconstruction)

Ab initio molecular dynamics simulation of photoisomerization in azobenzene in the nπ∗ state

Yusuke Ootani, Kiminori Satoh, Akira Nakayama, Takeshi Noro, and Tetsuya Taketsugu

J. Chem. Phys. 131, 194306 (2009); http://dx.doi.org/10.1063/1.3263918 (10 pages) | Cited 14 times

Online Publication Date: 19 November 2009

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Photoisomerization mechanism of azobenzene in the lowest excited state S1(nπ∗) is investigated by ab initio molecular dynamics (AIMD) simulation with the RATTLE algorithm, based on the state-averaged complete active space self-consistent field method. AIMD simulations show that cis to trans isomerization occurs via two-step rotation mechanism, accompanying rotations of the central NN part and two phenyl rings, and this process can be classified into two types, namely, clockwise and counterclockwise rotation pathways. On the other hand, trans to cis isomerization occurs via conventional rotation pathway where two phenyl rings rotate around the NN bond. The quantum yields are calculated to be 0.45 and 0.28±0.14 for cis to trans and trans to cis photoisomerizations, respectively, which are in very good agreement with the corresponding experimental results.
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31.15.A- Ab initio calculations
31.15.xv Molecular dynamics and other numerical methods
31.15.xr Self-consistent-field methods
82.50.-m Photochemistry
82.30.Qt Isomerization and rearrangement

Photochemistry of 3-hydroxyflavone inside superfluid helium nanodroplets

R. Lehnig, D. Pentlehner, A. Vdovin, B. Dick, and A. Slenczka

J. Chem. Phys. 131, 194307 (2009); http://dx.doi.org/10.1063/1.3262707 (8 pages) | Cited 4 times

Online Publication Date: 20 November 2009

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3-hydroxyflavone is a prototype system for excited state intramolecular proton transfer which is one step of a closed loop photocycle. It was intensively studied for the bare molecule and for the influence of solvents. In the present paper this photocycle is investigated for 3-hydroxyflavone and some hydrated complexes when doped into superfluid helium droplets by the combined measurement of fluorescence excitation spectra and dispersed emission spectra. Significant discrepancies in the proton transfer behavior to gas phase experiments provide evidence for the presence of different complex configurations of the hydrated complexes in helium droplets. Moreover, for bare 3-hydroxyflavone and its hydrated complexes the proton transfer appears to be promoted by the helium environment.
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82.50.-m Photochemistry
33.80.Rv Multiphoton ionization and excitation to highly excited states (e.g., Rydberg states)
33.80.Gj Diffuse spectra; predissociation, photodissociation
82.80.-d Chemical analysis and related physical methods of analysis
82.30.Hk Chemical exchanges (substitution, atom transfer, abstraction, disproportionation, and group exchange)
33.50.Dq Fluorescence and phosphorescence spectra

Oscillator strengths and line widths of dipole-allowed transitions in 14N2 between 86.0 and 89.7 nm

A. N. Heays, B. R. Lewis, G. Stark, K. Yoshino, Peter L. Smith, K. P. Huber, and K. Ito

J. Chem. Phys. 131, 194308 (2009); http://dx.doi.org/10.1063/1.3257690 (9 pages) | Cited 1 time

Online Publication Date: 20 November 2009

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Oscillator strengths of 23 electric-dipole-allowed bands of 14N2 in the 86.0–89.7 nm (111 480–116 280 cm−1) region are reported from synchrotron-based photoabsorption measurements at an instrumental resolution of 6.5×10−4 nm (0.7 cm−1) full width at half maximum. The absorption spectrum comprises transitions to vibrational levels of the cn 1Πu (n = 3,4), o3 1Πu, and cn+1′ 1Σu+(n = 3,4) Rydberg states as well as the b 1Πu and b′ 1Σu+ valence states. The J dependences of band f-values derived from the experimental line f-values are reported as polynomials in J(J+1) and are extrapolated to zero nuclear rotation in order to facilitate comparisons with the results of coupled Schrödinger equation calculations. Many bands in this study are characterized by a strong J dependence of the band f-values and display anomalous P-, Q-, and R-branch intensity patterns. Predissociation line widths are reported for six bands. The experimental f-value and line-width patterns inform current efforts to develop comprehensive spectroscopic models for N2 that incorporate rotational effects and predissociation mechanisms, and are critical for the construction of realistic atmospheric radiative-transfer models.
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33.70.Ca Oscillator and band strengths, lifetimes, transition moments, and Franck-Condon factors
33.70.Jg Line and band widths, shapes, and shifts
33.80.Gj Diffuse spectra; predissociation, photodissociation
33.80.Rv Multiphoton ionization and excitation to highly excited states (e.g., Rydberg states)
33.15.Mt Rotation, vibration, and vibration-rotation constants

Electronic photodissociation spectra and decay pathways of gas-phase IrBr62−

Jesse C. Marcum and J. Mathias Weber

J. Chem. Phys. 131, 194309 (2009); http://dx.doi.org/10.1063/1.3265956 (8 pages) | Cited 5 times

Online Publication Date: 20 November 2009

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We report photodissociation action spectra for the dianion IrBr62− in the range of 1.08–5.6 eV. The photoproducts observed are IrBr6−, IrBr5−, IrBr4− and Br−. Comparison of the action spectra to the aqueous absorption spectrum of K2IrBr6 leads to the determination of solvatochromic shifts of between 0.02 and 0.16 eV in the visible region and approximately 0.3 eV in the ultraviolet. The fragmentation branching ratios vary greatly as a function of photon energy. This behavior can be attributed to differences in the fragmentation mechanisms as well as differences in the excited states that are accessed at different energies. Absorption in the visible region favors fragmentation into IrBr5− and Br−, whereas a number of fragmentation channels and mechanisms are active in the ultraviolet region. These mechanisms include fragmentation as well as electron detachment and dissociative electron detachment.
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33.80.Gj Diffuse spectra; predissociation, photodissociation
82.50.Hp Processes caused by visible and UV light
33.20.Kf Visible spectra
82.80.Dx Analytical methods involving electronic spectroscopy
back to top Condensed Phase Dynamics, Structure, and Thermodynamics: Spectroscopy, Reactions, and Relaxation

Improvement of the ab initio embedded cluster method for luminescence properties of doped materials by taking into account impurity induced distortions: The example of Y2O3:Bi3+

Florent Réal, Belén Ordejón, Valérie Vallet, Jean-Pierre Flament, and Joël Schamps

J. Chem. Phys. 131, 194501 (2009); http://dx.doi.org/10.1063/1.3259048 (17 pages) | Cited 1 time

Online Publication Date: 16 November 2009

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New ab initio embedded-cluster calculations devoted to simulating the electronic spectroscopy of Bi3+ impurities in Y2O3 sesquioxide for substitutions in either S6 or C2 cationic sites have been carried out taking special care of the quality of the environment. A considerable quantitative improvement with respect to previous studies [ F. Réal et al. J. Chem. Phys. 125, 174709 (2006) ; F. Réal et al. J. Chem. Phys. 127, 104705 (2007) ] is brought by using environments of the impurities obtained via supercell techniques that allow the whole (pseudo) crystal to relax (WCR geometries) instead of environments obtained from local relaxation of the first coordination shell only (FSR geometries) within the embedded cluster approach, as was done previously. In particular the uniform 0.4 eV discrepancy of absorption energies found previously with FSR environments disappears completely when the new WCR environments of the impurities are employed. Moreover emission energies and hence Stokes shifts are in much better agreement with experiment. These decisive improvements are mainly due to a lowering of the local point-group symmetry (S6→C3 and C2→C1) when relaxing the geometry of the emitting (lowest) triplet state. This symmetry lowering was not observed in FSR embedded cluster relaxations because the crystal field of the embedding frozen at the genuine pure crystal positions seems to be a more important driving force than the interactions within the cluster, thus constraining the overall symmetry of the system. Variations of the doping rate are found to have negligible influence on the spectra. In conclusion, the use of WCR environments may be crucial to render the structural distortions occurring in a doped crystal and it may help to significantly improve the embedded-cluster methodology to reach the quantitative accuracy necessary to interpret and predict luminescence properties of doped materials of this type.
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78.55.Hx Other solid inorganic materials
61.72.up Other materials
61.72.S- Impurities in crystals
61.50.Ah Theory of crystal structure, crystal symmetry; calculations and modeling
71.70.Ch Crystal and ligand fields
61.66.Fn Inorganic compounds

Pressure dependence of the large-scale structure of water

A. Cunsolo, F. Formisano, C. Ferrero, F. Bencivenga, and S. Finet

J. Chem. Phys. 131, 194502 (2009); http://dx.doi.org/10.1063/1.3259882 (5 pages) | Cited 7 times

Online Publication Date: 16 November 2009

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We report on small-angle x-ray scattering measurements on liquid water aimed at characterizing the pressure evolution of its large-scale structure. Diffraction profiles have been fitted assuming a Lorentzian dependence on the exchanged momentum. As a result, we observe an anomalous behavior of the diffracted intensity that tends to disappear, increasing either the pressure or the temperature. This effect is discussed in detail and imputed to the ability of hydrostatic pressure to weaken hydrogen bonds.
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61.25.Em Molecular liquids

Multiplet splittings and intensities of fine structure components of the Q1(0)H2+S0(0)N2 transition in a solid parahydrogen matrix

Adya P. Mishra and Param Jeet Singh

J. Chem. Phys. 131, 194503 (2009); http://dx.doi.org/10.1063/1.3264689 (6 pages) | Cited 1 time

Online Publication Date: 16 November 2009

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A comprehensive analysis of theoretical multiplet splittings and intensities of the fine structure components of the Q1(0)H2+S0(0)N2 transition in a solid parahydrogen crystal is presented. The consideration of higher order anisotropic term responsible for splittings is essential to explain the observed splitting of the three components. The pair interaction parameters ΔB and ΔC have been determined by comparing the theoretical splittings with the experimental values. The information about the small splittings ( ∼ 0.1 cm−1) due to crystal-field interaction is completely obscured due to fast hopping of v′ = 1, J′ = 0 H2 vibron. Also, the theoretical expressions are derived for the intensities of the fine structure components of the QvH2(0)+SvN2(0) transition and the theoretical results are compared with the experimental findings.
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34.20.Gj Intermolecular and atom-molecule potentials and forces
33.15.Pw Fine and hyperfine structure
71.70.Ch Crystal and ligand fields
FREE

Theory for the three-dimensional Mercedes-Benz model of water

Alan Bizjak, Tomaz Urbic, Vojko Vlachy, and Ken A. Dill

J. Chem. Phys. 131, 194504 (2009); http://dx.doi.org/10.1063/1.3259970 (7 pages) | Cited 6 times

Online Publication Date: 16 November 2009

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The two-dimensional Mercedes-Benz (MB) model of water has been widely studied, both by Monte Carlo simulations and by integral equation methods. Here, we study the three-dimensional (3D) MB model. We treat water as spheres that interact through Lennard-Jones potentials and through a tetrahedral Gaussian hydrogen bonding function. As the “right answer,” we perform isothermal-isobaric Monte Carlo simulations on the 3D MB model for different pressures and temperatures. The purpose of this work is to develop and test Wertheim’s Ornstein–Zernike integral equation and thermodynamic perturbation theories. The two analytical approaches are orders of magnitude more efficient than the Monte Carlo simulations. The ultimate goal is to find statistical mechanical theories that can efficiently predict the properties of orientationally complex molecules, such as water. Also, here, the 3D MB model simply serves as a useful workbench for testing such analytical approaches. For hot water, the analytical theories give accurate agreement with the computer simulations. For cold water, the agreement is not as good. Nevertheless, these approaches are qualitatively consistent with energies, volumes, heat capacities, compressibilities, and thermal expansion coefficients versus temperature and pressure. Such analytical approaches offer a promising route to a better understanding of water and also the aqueous solvation.
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61.20.Ja Computer simulation of liquid structure
65.20.-w Thermal properties of liquids
62.10.+s Mechanical properties of liquids

A theoretical basis for spontaneous polarization transfer in non-hydrogenative parahydrogen-induced polarization

Ralph W. Adams, Simon B. Duckett, Richard A. Green, David C. Williamson, and Gary G. R. Green

J. Chem. Phys. 131, 194505 (2009); http://dx.doi.org/10.1063/1.3254386 (15 pages) | Cited 6 times

Online Publication Date: 16 November 2009

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When parahydrogen adds to a metal template containing a substrate of interest, the substrate and parahydrogen become coupled, and polarization is shared between the two without the incorporation of the parahydrogen into the substrate. A mechanism for this polarization transfer is presented in which the transfer is propagated through the scalar couplings. At zero field, polarization is transferred between two-, three-, and four-spin zero quantum states, but no single spin magnetization is created. The interplay between the chemical shift evolution and the evolution under scalar coupling at non-zero field generates additional longitudinal spin order and now includes single spin longitudinal z-magnetization. The additional chemical shift interaction introduces a field dependency to the nuclear spin states of the polarized substrate. The net effect of the polarization field strength on the resultant nuclear spin states is shown to be predictable but complex.
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33.25.+k Nuclear resonance and relaxation

A new generic model potential for mesogenic systems: Square well line potential of variable range

Szabolcs Varga and Franz J. Vesely

J. Chem. Phys. 131, 194506 (2009); http://dx.doi.org/10.1063/1.3264109 (8 pages) | Cited 1 time

Online Publication Date: 18 November 2009

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A single-site pair potential is derived to approximate the linear n-site square well interaction. The resulting square well line (SWL) potential is analytical, fairly smooth, and reproduces the distance and orientation dependence of the multisite pair energy. It contains only three control parameters n, L, and s2, in addition to the units of length s1 and energy ε. The advantages of the new model over the traditional potentials such as Gay–Berne and Kihara are that n, L, and s2 are physically meaningful quantities and that no additional adjustable parameters are introduced. With the SWL potential even very long square well chain molecules may be treated in Monte Carlo (MC) simulations; moreover the model is well suited for perturbation theory. Using Onsager-like theories we test the effect of molecular elongation, temperature, and the range of the square well potential on the vapor-liquid and nematic-smectic A (NS) phase transitions. We find that the vapor-liquid binodal of the SWL fluid is in good agreement with MC results for square well dumbbells. For repulsive SWL particles, varying the interaction range s2 results in a similar effect on the NS transition as the change in the ionic strength in a real suspension of fd viruses.
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34.20.Gj Intermolecular and atom-molecule potentials and forces
31.15.xp Perturbation theory

A molecular dynamics study of the influence of ionic charge distribution on the dynamics of a molten salt

Hualin Li and Mark N. Kobrak

J. Chem. Phys. 131, 194507 (2009); http://dx.doi.org/10.1063/1.3263129 (7 pages) | Cited 3 times

Online Publication Date: 19 November 2009

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The distribution of charge in an ion of a fused salt is known to be an important determinant of liquid dynamics. However, the details of this relationship remain poorly understood. We present the results of molecular dynamics simulations on a model molten salt system and show that changes in the distribution of ionic charge can have a profound effect on liquid dynamics. In particular, we observe complex relationships between the distribution of charge, the rate of ionic rotation, and the translational diffusion of ions in the liquid.
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61.25.-f Studies of specific liquid structures
66.10.C- Diffusion and thermal diffusion
61.20.Ja Computer simulation of liquid structure

Localized soft modes and the supercooled liquid’s irreversible passage through its configuration space

Asaph Widmer-Cooper, Heidi Perry, Peter Harrowell, and David R. Reichman

J. Chem. Phys. 131, 194508 (2009); http://dx.doi.org/10.1063/1.3265983 (12 pages) | Cited 4 times

Online Publication Date: 19 November 2009

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Using computer simulations, we show that the localized low frequency normal modes of a configuration in a supercooled liquid are strongly correlated with the irreversible structural reorganization of the particles within that configuration. Establishing this correlation constitutes the identification of the aspect of a configuration that determines the heterogeneity of the subsequent motion. We demonstrate that the spatial distribution of the summation over the soft local modes can persist in spite of particle reorganization that produces significant changes in individual modes. Along with spatial localization, the persistent influence of soft modes in particle relaxation results in anisotropy in the displacements of mobile particles over the time scale referred to as β-relaxation.
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61.20.Ja Computer simulation of liquid structure
61.25.-f Studies of specific liquid structures
64.70.pm Liquids

Spin-locking of half-integer quadrupolar nuclei in nuclear magnetic resonance of solids: Second-order quadrupolar and resonance offset effects

Sharon E. Ashbrook and Stephen Wimperis

J. Chem. Phys. 131, 194509 (2009); http://dx.doi.org/10.1063/1.3263904 (15 pages) | Cited 5 times

Online Publication Date: 19 November 2009

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Spin-locking of spin I = 3/2 and I = 5/2 nuclei in the presence of small resonance offset and second-order quadrupolar interactions has been investigated using both exact and approximate theoretical and experimental nuclear magnetic resonance (NMR) approaches. In the presence of second-order quadrupolar interactions, we show that the initial rapid dephasing that arises from the noncommutation of the state prepared by the first pulse and the spin-locking Hamiltonian gives rise to tensor components of the spin density matrix that are antisymmetric with respect to inversion, in addition to those symmetric with respect to inversion that are found when only a first-order quadrupolar interaction is considered. We also find that spin-locking of multiple-quantum coherence in a static solid is much more sensitive to resonance offset than that of single-quantum coherence and show that good spin-locking of multiple-quantum coherence can still be achieved if the resonance offset matches the second-order shift of the multiple-quantum coherence in the appropriate reference frame. Under magic angle spinning (MAS) conditions, and in the "adiabatic" limit, we demonstrate that rotor-driven interconversion of central-transition single- and three-quantum coherences for a spin I = 3/2 nucleus can be best achieved by performing the spin-locking on resonance with the three-quantum coherence in the three-quantum frame. Finally, in the "sudden" MAS limit, we show that spin I = 3/2 spin-locking behavior is generally similar to that found in static solids, except when the central-transition nutation rate matches a multiple of the MAS rate and a variety of rotary resonance phenomena are observed depending on the internal spin interactions present. This investigation should aid in the application of spin-locking techniques to multiple-quantum NMR of quadrupolar nuclei and of cross-polarization and homonuclear dipolar recoupling experiments to quadrupolar nuclei such as 7Li, 11B, 17O, 23Na, and 27Al.
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76.60.-k Nuclear magnetic resonance and relaxation

Manipulating stimulated coherent anti-Stokes Raman spectroscopy signals by broad-band and narrow-band pulses

Saar Rahav, Oleksiy Roslyak, and Shaul Mukamel

J. Chem. Phys. 131, 194510 (2009); http://dx.doi.org/10.1063/1.3259653 (11 pages) | Cited 3 times

Online Publication Date: 20 November 2009

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A transition-amplitude based representation of heterodyne detected coherent anti-Stokes Raman signals is used to separate them into a parametric component that involves no change in the material and dissipative processes associated with various transitions between states. Qualitatively different contributions from the two processes are predicted for the signal generated by an overlapping narrow (picosecond) and broad-band (femtosecond) pulse.
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42.65.Dr Stimulated Raman scattering; CARS
42.65.Es Stimulated Brillouin and Rayleigh scattering
42.70.Nq Other nonlinear optical materials; photorefractive and semiconductor materials
42.65.Jx Beam trapping, self-focusing and defocusing; self-phase modulation
42.65.Re Ultrafast processes; optical pulse generation and pulse compression

Molecular cooperativity in the dynamics of glass-forming systems: A new insight

L. Hong, P. D. Gujrati, V. N. Novikov, and A. P. Sokolov

J. Chem. Phys. 131, 194511 (2009); http://dx.doi.org/10.1063/1.3266508 (7 pages) | Cited 6 times

Online Publication Date: 20 November 2009

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The mechanism behind the steep slowing down of molecular motions upon approaching the glass transition remains a great puzzle. Most of the theories relate this mechanism to the cooperativity in molecular motion. In this work, we estimate the length scale of molecular cooperativity ξ for many glass-forming systems from the collective vibrations (the so-called boson peak). The obtained values agree well with the dynamic heterogeneity length scale estimated using four-dimensional NMR. We demonstrate that ξ directly correlates to the dependence of the structural relaxation on volume. This dependence presents only one part of the mechanism of slowing down the structural relaxation. Our analysis reveals that another part, the purely thermal variation in the structural relaxation (at constant volume), does not have a direct correlation with molecular cooperativity. These results call for a conceptually new approach to the analysis of the mechanism of the glass transition and to the role of molecular cooperativity.
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64.70.qj Dynamics and criticality
76.60.-k Nuclear magnetic resonance and relaxation
61.43.Fs Glasses
63.50.Lm Glasses and amorphous solids
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