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  • 1
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 102 (1995), S. 5480-5485 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Molecular dynamics simulations of clusters containing hundreds of naphthalene molecules were used to investigate vibrational cooling and vibrational heating. The effects of isotopic substitution, modeled by changing the masses of the extended-atom C–H groups, were also studied. In vibrational cooling, a hotter molecule (300 K) is allowed to interact with a cold cluster (10 K). Pure clusters of normal, light, and heavy naphthalene molecules were cooled with roughly the same time constant (∼50 ps). However, in mixed clusters containing a normal molecule in an isotopically substituted heavy or light cluster, the normal molecule cooled much more slowly, indicating the dominant cooling mechanism in pure clusters is resonant intermolecular vibrational energy transfer. In vibrational heating studies, a cold molecule (10 K) is allowed to interact with a cluster which is much hotter (300 K) than in the vibrational cooling studies (10 K). Normal molecules in pure or mixed clusters were heated at about the same rates and those rates were about what was seen in vibrational cooling simulations. At the higher temperatures of the vibrational heating simulation, phonon-assisted intermolecular vibrational energy transfer between unlike molecules in mixed clusters occurs at rates similar to resonant transfer processes between like molecules in pure clusters. © 1995 American Institute of Physics.
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  • 2
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 90 (2001), S. 5139-5146 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Shock-wave induced nanopore collapse (average diameter 100 nm) at 4.2 GPa in a 3-μm-thick poly-methyl methacrylate (PMMA) layer is measured in real time using coherent anti-Stokes Raman spectroscopy (CARS). Pore collapse is monitored via CARS transitions of a dye probe embedded in the porous medium. A pore collapse time constant of 3 ns in PMMA is in poor agreement with hydrodynamic pore collapse models but in excellent agreement with a viscoplastic model that uses the "shock viscosity" determined from the PMMA viscoelastic response to shock. The shock viscosity is more than 12 orders of magnitude smaller than the ordinary viscosity. A downstream gauge of polycrystalline anthracene monitors changes in the steeply rising shock front (〈25 ps rise time) after passing through the porous medium or a scattering medium with 100-nm-diam scatterers. The anthracene is a two-dimensional (2D) shock gauge that provides a time sequence of CARS spectra S(t,λ). The 2D gauge is shown to be capable of discriminating between a shock front that gradually rises with time constant tr or a bunch of steeply rising shocklets with an arrival time spread equal to tr. The transmitted shock front is shown to consist of a bunch of steep shocklets with an arrival time spread of 550 ps. © 2001 American Institute of Physics.
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  • 3
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 64 (1988), S. 2955-2958 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A high-power ultrafast laser spectrometer with image acquisition capability, the "picosecond microscope'' is used to study optical surface damage processes in a transparent polymer, polymethyl methacrylate. Optical damage is a fast, violent, inhomogeneous solid-state chemical reaction. We observe three distinct fast processes: creation and growth of a dark absorbing damage volume, the "damage core,'' creation and propagation of a hypersonic shock wave in the surrounding atmosphere, and creation of large amplitude acoustic waves which propagate outward from the core at the velocity of sound.
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  • 4
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 88 (1988), S. 949-967 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The processes of vibrational relaxation (VR) and vibrational cooling (VC) are investigated in low temperature crystals of complex molecules, specifically benzene, naphthalene, anthracene, and durene. In the VR process, a vibration is deexcited, while VC consists of many sequential and parallel VR steps which return the crystal to thermal equilibrium. A theoretical model is developed which relates the VR rate to the excess vibrational energy, the molecular structure, and the crystal structure. Specific relations are derived for the vibrational lifetime T1 in each of three regimes of excess vibrational energy. The regimes are the following: Low frequency regime I where VR occurs by emission of two phonons, intermediate frequency regime II where VR occurs by emission of one phonon and one vibration, and high frequency regime III where VR occurs by evolution into a dense bath of vibrational combinations. The VR rate in each regime depends on a particular multiphonon density of states and a few averaged anharmonic coefficients. The appropriate densities of states are calculated from spectroscopic data, and together with available VR data and new infrared and ps Raman data, the values of the anharmonic coefficients are determined for each material. The relationship between these parameters and the material properties is discussed. We then describe VC in a master equation formalism. The transition rate matrix for naphthalene is found using the empirically determined parameters of the above model, and the time dependent redistribution in each mode is calculated.
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  • 5
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 93 (1990), S. 1695-1710 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A new method is presented for calculating ultrafast vibrational energy redistribution in anharmonic solids composed of large molecules. It is an improvement over the previous weak coupling model of Hill and Dlott [J. Chem. Phys. 89, 842 (1988)] because the emitted phonons are now allowed to act back on the excited vibrations. The model is used to investigate the dynamics of "ultrahot'' molecular solids, materials with enormous levels of vibrational or phonon excitation. Ultrahot solids are produced in laser ablation and shock-induced detonation. Using model parameters for crystalline naphthalene, we investigate multiphonon up pumping after a 40 kbar shock and vibrational cooling after strong excitation of a high frequency vibrational fundamental. In both processes, the phonons attain a state of internal equilibrium characterized by a time-dependent phonon quasitemperature θp(t) within a few ps. Energy redistribution among the phonons is efficient because phonons are more anharmonic than molecular vibrations. In up pumping, there is a large excess of phonons at t=0, which decreases as vibrations are pumped by phonons. Under these conditions, the rates of anharmonic scattering processes are maximum at t=0 and the lower levels of the ladder of molecular vibrations are pumped before the higher levels. The vibrational population distribution then rapidly attains an approximate state of quasiequilibrium, characterized by a vibrational quasitemperature θv(t). Thermal equilibrium where θp(t) = θv(t) is achieved in ∼100 ps. In vibrational cooling, there is initially a large excess of high frequency vibrations and few phonons. Because phonons accumulate as the vibrations cool, the rates of anharmonic scattering processes are a minimum at t=0. Under these conditions, the vibrations are far from a state of quasiequilibrium until thermal equilibrium is attained at ∼1 ns.
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  • 6
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 88 (1988), S. 2361-2371 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Vibrational relaxation (VR) of dilute impurity molecules (naphthalene, anthracene) in crystalline host matrices (durene, naphthalene) is studied with the ps photon echo technique. The results obtained by echoes on vibrations in the electronically excited state are compared to previous ps time delayed coherent Raman studies of ground state vibrations of the pure host matrix. The relaxation channels for guest and host, and the effects of molecular and crystal structure on VR rates are determined.
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  • 7
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 95 (1991), S. 5775-5784 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Polarization-selective transient grating experiments have been used to study the subnanosecond time scale dynamics of several sodium-seeded, premixed flames. Intensity gratings (in which both excitation beams are of the same polarization) were used to determine excited-state quenching collision rates, while polarization gratings (in which the excitation beams are cross polarized) were used to measure Na diffusion constants and the rates of Na ground state magnetic sublevel population scattering collisions. In addition, the rates of scattering between the 3P1/2 and 3P3/2 excited state levels were measured using an excited state probing scheme.
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  • 8
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 94 (1991), S. 8203-8209 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A molecular dynamics simulation of crystalline naphthalene is used to study nanometer scale thermal transport in solids. One molecule in a cluster of 75 is heated to a large initial temperature and then allowed to cool. Stochastic boundary conditions which preserve the time averaged volume of the cluster are used. The excess translational and librational energy of the hot molecule is lost within 1 ps. The excess vibrational energy is lost on the 100 ps time scale. Translational and librational energy propagates rapidly throughout the cluster at velocities which are comparable to the speed of sound. Despite the far slower rate of vibrational energy loss from the hot molecule, the growth of vibrational energy occurs uniformly on the other molecules in the cluster. Therefore intermolecular vibrational energy transfer occurs primarily via an indirect mechanism. Vibrational excitations are first converted into translational and librational excitations, which propagate throughout the cluster and then excite vibrations on distant molecules via multiphonon up pumping. Examination of the molecular neighbors shows that intermolecular transfer of mechanical energy can be anisotropic, since the hot molecule can only transfer energy where it contacts atoms on adjacent molecules. Energy transfer along the b- and c-crystallographic axes is more efficient than along the a axis. The most efficient energy transfer is in the direction of two of the four nearest neighbors. Transient hot spots are produced on these neighboring molecules. The implications of this anisotropic conduction for the propagation of thermal reactions, e.g., the decomposition of high explosives, are discussed briefly.
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  • 9
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 65 (1989), S. 4548-4563 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: An ultrafast two-color laser spectrometer with image acquisition capability is used to study surface ablation of a transparent polymer, PMMA (polymethyl methacrylate). Surface ablation was produced by 100-ps, 0.532-μm pulses and probed by 2-ps, 0.570-μm pulses. Computer-digitized images were obtained over the time range 10−12 –100 s. The images were analyzed to obtain the time-dependent behavior of the damaged solid, and the blast wave generated at the solid-gas interface. Near the peak of the ablation pulse, self-focusing begins and produces a small-diameter filament lasting for 20 ps. The polymer irradiated by the filament then undergoes explosive thermal decomposition, ejecting particles from a conical volume into the atmosphere above the surface. This ablated matter produces a hemispherical, supersonic blast wave whose kinetic energy is one-fourth of the ablation pulse energy. The evacuated pit produced in the polymer is very hot, and the surrounding solid softens and flows, resolidifying in about 1 s. A mechanism for the ablation process involving nonlinear absorption is proposed. The steeply rising envelope of the ablation pulse simultaneously increases the absorption coefficient and decreases the absorption length, resulting in a runaway heating process with a rate of ≈1013 K/s. The polymer is overheated far beyond the normal decomposition temperature. Thermal decomposition then proceeds with a large, negative free energy.
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  • 10
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 54 (1989), S. 2274-2276 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Laser surface ablation of polymethylmethacrylate by ultrafast 0.532 μm pulses is studied using an imaging apparatus with 2 ps resolution. Coherent two-photon absorption rapidly heats the sample, inducing explosive thermal decomposition. Electron microscopy is used to characterize the damaged surface. Ultrafast imaging shows that surface damage is accompanied by the production of a transient optical filament. The intensity dependence shows that self-focusing results from an accumulative, rather than instantaneous, relaxation of the transient refractive index. At all intensities, there is a 20 ps delay before ablation commences.
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