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  • 1
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 111 (1999), S. 3498-3507 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The rate constant kO(υ=1) for NO(υ=1) vibrational relaxation by O has been measured at room temperature using a laser photolysis-laser probe technique. Vibrationally excited NO and relaxer O atoms were formed using 355 nm laser photolysis of a dilute mixture of NO2 in argon bath gas. The time evolution of both the NO(υ=1) and the O atoms was monitored using laser-induced fluorescence (LIF). The required absolute O-atom densities were obtained through a comparison of O-atom LIF signals from the photolysis source and from a titrated cw microwave source. At early times the O atoms constitute the most important loss mechanism for the nascently produced NO(υ=1). Possible effects from NO(υ=1) vibrational ladder-climbing and from thermal expansion have been shown to be minimal. The rate constant kO(υ=1)=(2.4±0.5)×10−11 cm3 s−1 determined herein is a factor of 2 to 3 lower than the generally accepted value of kO(υ=1) used in thermospheric modeling. The present value for kO(υ=1) is the same, within the error bars, as the kO(υ=2,3) previously measured in this laboratory using an entirely different technique, resonant infrared laser excitation of NO(υ=0). This result suggests that the collisional relaxation rates are independent of υ. A recent quasiclassical trajectory calculation, in which both allowed NO–O surfaces have been explicitly considered, predicts a collisional relaxation rate which is in good agreement with the present result. The kO(υ=1) value, along with previously measured rate constants for NO–O high-pressure recombination (krec∞) and isotope exchange (kiso), can serve as a proxy for the rate coefficient kC describing the formation of a long-lived NO2* intermediate from O+NO collisions. The present value for kO(υ=1) is significantly lower, however, than a recent determination of krec∞ and also the value of kC derived from kiso. In the latter case the comparison is not as straightforward. © 1999 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 101 (1994), S. 6141-6156 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A new molecular dynamics model in which the point charges on atomic sites are allowed to fluctuate in response to the environment is developed and applied to water. The idea for treating charges as variables is based on the concept of electronegativity equalization according to which: (a) the electronegativity of an atomic site is dependent on the atom's type and charge and is perturbed by the electrostatic potential it experiences from its neighbors and (b) charge is transferred between atomic sites in such a way that electronegativities are equalized. The charges are treated as dynamical variables using an extended Lagrangian method in which the charges are given a fictitious mass, velocities, and kinetic energy and then propagated according to Newtonian mechanics along with the atomic degrees of freedom. Models for water with fluctuating charges are developed using the geometries of two common fixed-charge water potentials: the simple point charge (SPC) and the four-point transferable intermolecular potential (TIP4P). Both fluctuating charge models give accurate predictions for gas-phase and liquid state properties, including radial distribution functions, the dielectric constant, and the diffusion constant. The method does not introduce any new intermolecular interactions beyond those already present in the fixed charge models and increases the computer time by only a factor of 1.1, making this method tractable for large systems.
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  • 3
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Review of Scientific Instruments 71 (2000), S. 3567-3569 
    ISSN: 1089-7623
    Source: AIP Digital Archive
    Topics: Physics , Electrical Engineering, Measurement and Control Technology
    Notes: A liquid nitrogen immersion cryostat has been developed for optical measurements. Liquid nitrogen in the sample chamber is kept free of bubbles and schlieren by the use of a cooling jacket of sacrificial liquid nitrogen, which is kept at a lower pressure than the sample chamber. This design has proven especially useful for volatile liquid samples, where direct electrical connections, rapid sample freezing, and efficient heat dissipation are required, but it can also accommodate a wide variety of other samples. The cryostat is compact, easy to use, and relatively inexpensive. © 2000 American Institute of Physics.
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  • 4
    Publication Date: 2014-11-15
    Description: Al x In y Ga (1-x-y) N materials show promise for use in GaN-based heterojunction devices. The growth of these materials has developed to the point where they are beginning to see implementation in high electron mobility transistors (HEMTs) and light emitting diodes. However, the electrical properties of these materials are still poorly understood, especially as related to the net polarization charge at the AlInGaN/GaN interface ( Q π ( net )). All theoretical calculations of Q π ( net ) share the same weakness: dependence upon polarization bowing parameters, which describe the deviation in Q π ( net ) from Vegard's law. In this study, direct analysis of Q π ( net ) for Al 0.54 In 0.12 Ga 0.34 N/GaN HEMTs is reported as extracted from C-V , I-V , and Hall measurements performed on samples grown by metalorganic chemical vapor deposition. An average value for Q π ( net ) is calculated to be 2.015 × 10 −6 C/cm 2 , with just 6.5% variation between measurement techniques.
    Print ISSN: 0021-8979
    Electronic ISSN: 1089-7550
    Topics: Physics
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  • 5
    Publication Date: 2016-10-18
    Description: Cu 2 ZnSn(S,Se) 4 is an interesting, earth abundant photovoltaic material, but has suffered from low open circuit voltage. To better understand the film structure, we have measured resonant x-ray diffraction across the Cu and Zn K -edges for the device quality thin films of Cu 2 ZnSnS 4 (8.6% efficiency) and Cu 2 ZnSn(S,Se) 4 (3.5% efficiency). This approach allows for the confirmation of the underlying kesterite structure and quantification of the concentration of point defects and vacancies on the Cu, Zn, and Sn sublattices. Rietveld refinement of powder diffraction data collected at multiple energies is used to determine that there exists a high level of Cu Zn and Zn Cu defects on the 2c and 2d Wyckoff positions. We observe a significantly lower concentration of Zn Sn defects and Cu or Zn vacancies.
    Print ISSN: 0003-6951
    Electronic ISSN: 1077-3118
    Topics: Physics
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  • 6
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 94 (1991), S. 1698-1704 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The nondegenerate ν2←0 and 2ν2←ν2 bands of the ammonia cation NH+3 have been observed using tunable diode lasers combined with the velocity modulation technique. The ion was produced in a water-cooled 6 kHz ac glow discharge cell with a gas mixture of [He]@B:[N2]@B:[H2]=9@B:0.06@B:0.3 (Torr). From the observed spectra, the band origins were determined to be ν1←0=903.3898 cm−1 and ν2←1=939.771 cm−1. Vibration–rotation interaction constants and potential constants were derived. The missing of K=0 R-branch transitions with N=odd in the ν2←0 band and N=even in the 2ν2←ν2 band clearly shows the characteristics of a D3h planar structure with a 2A‘2 ground electronic state, just like its isoelectronic case CH3 radical. Spin–rotation doublets were well-resolved in R-branch transitions and spin–rotation interaction constants of the ground, ν2, and 2ν2 states were determined. A potential function consisting of a quadratic term and a quartic term was used for modeling the out-of-plane bending vibration of NH+3. In comparison with the methyl radical, the ammonia cation is more rigid and closer to a harmonic oscillator.
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 93 (1990), S. 2640-2657 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The distribution of potentials or fields felt at any given point in a liquid (the local field distribution) ends up being the crucial element in calculating quantities ranging from the inhomogeneous broadening of spectral lines to the rates of irreversible electron transfer. Indeed, the usefulness of this distribution in even its simplest form, the version which assumes a completely uncorrelated environment, has long been appreciated. However, there are a number of difficulties with this version. When the fluid density is low enough to make a neglect of correlations reasonable, the distribution function can still be awkward to calculate numerically. Much more seriously, the omission of correlations among the surrounding atoms is totally unrealistic in a dense liquid. We show here that it is possible to arrive at expressions for the local field distribution that are both accurate under dense liquid conditions and are straightforward to evaluate numerically. The key to this development turns out to be the recognition that the short-ranged and long-ranged contributions to the local field play qualitatively different roles—which can be separated formally using a device we call a closest particle expansion. The qualitative differences between the results for correlated and uncorrelated particles are discussed, as is the appropriateness of the commonly used Gaussian approximation.
    Type of Medium: Electronic Resource
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  • 8
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 92 (1990), S. 1758-1767 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The CO fundamental vibration–rotation spectra resulting from the interaction of discharged nitrogen with carbon monoxide at low pressure (∼3 mTorr) exhibit bimodal rotational distributions. We have identified 14 vibrational levels of a rotationally relaxed (80 K) component and eight vibrational levels from a rotationally excited component. The eight rotationally excited bands are best reproduced by a statistical distribution E=ER+EV=3.7 eV, which provides sufficient population in the region of the Fortrat reversal (J∼90) to account for the observed R-branch bandhead formation. The rotationally relaxed vibrational levels are populated by single- and two-quantum transfer from N2(v), N2(v)+CO→N2(v−1,2)+CO(v=1,2), and radiative cascade from CO(A) produced by quenching of N2(a'), N2(a' 1Σ−u) +CO→N2(X,v)+CO(A 1Π)→CO(v≤9)+hν, and relaxation of the rotationally excited component. Kinetic and energetic arguments indicate that a branch of N2(a') quenching N2(a' 1Σ−u) +CO→N2(X,v)+CO(v≤14,J) is responsible for the rotationally excited component. Surprisal analysis indicates two dynamic mechanisms are responsible for the rotationally excited component. We have modeled the vibrational distribution of the rotationally excited component with equal contributions from a statistical (all v) process and a process favoring excitation of low vibrational levels (v≤4).
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 91 (1989), S. 439-453 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A novel modification to the "slithering snake'' algorithm is used to enable Monte Carlo simulations of partially ionized polyelectrolyte chains where the charged beads interact via screened Coulomb interactions. The use of "stroboscopic'' averaging enables detailed shape characteristics of the chains to be calculated. The moment of inertia tensor, the distribution function of the end-to-end distance and the segment density distribution functions from the center of mass and both ends of the polyion are combined to give an overall characterization of the shape changes of a polyion as added salt concentration, chain length (up to 240 beads) and degree of ionization are varied. Some abrupt behavior seen for high degree of ionization may be smoothed once ionic degrees of freedom are included. The present work—by characterizing the shape of short chains—may also help to formulate models for very long polyions consisting of many segments, each of a few hundred beads.
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  • 10
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 90 (1989), S. 1188-1199 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The density functional theory of freezing is used to study the freezing of binary Lennard-Jones mixtures. The phase diagrams of several different Lennard-Jones systems are presented, including models of real binary mixtures of argon, krypton, and methane. The relative importance of size ratio and interaction energy are examined. Three generic types of phase diagram, found in real materials, are obtained. The phase diagram of the hard sphere binary mixture is also presented.
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