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  • 1
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 99 (1995), S. 4525-4530 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 99 (1995), S. 9102-9109 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 77 (1995), S. 5950-5960 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Picosecond time-resolved coherent Raman spectroscopy (ps CARS) is used to study photothermal ablation, induced by 150 ps duration near-infrared optical pulses, of poly-(methyl methacrylate) (PMMA) thin films doped with a small amount of near-infrared absorbing dye. The pressure and temperature shifts of a PMMA transition at ≈808 cm−1 were calibrated in static P and T experiments. Dynamic frequency shifting of the PMMA transition is used to determine temperature and pressure in the ablating thin film, and to investigate the dynamics of fast thin-film volume expansion. When the ablation pulse intensity is varied, ps CARS measurements of T and P are shown to be consistent with the results of conventional measurements below threshold, but near and above threshold picosecond time scale data show noticeable differences. Picosecond time scale ablation involves solid-state shock waves, which are not produced by longer duration ablation pulses. A pressure jump, often several kbar, is produced when the film is heated faster than a characteristic hydrodynamic volume relaxation time τh. Pressure release occurs by shock rarefaction wave propagation. When the rarefaction wave reaches the substrate, a tensile force is exerted on the thin film, causing it to break away from the substrate. The pressure in the thin film at ablation threshold, Pabl≈0.5 GPa, is found to be generated by roughly equal contributions from shock and thermochemical polymer decomposition processes. Therefore the picosecond time scale ablation process is termed shock-assisted photothermal ablation. The value of Pabl is interpreted to be the nanosecond time scale dynamic tensile strength of the thin film under conditions of ultrafast heating. It is found to be about one order of magnitude greater than the static strength of PMMA. © 1995 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 75 (1994), S. 4975-4983 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A large area shock target array was fabricated. By moving the array through a ps pulsed laser beam, shock waves could be reproducibly generated at a high repetition rate of up to ten shocks per second. The dynamics of shock wave propagation through various layers of the array were studied using optical nanogauges. A nanogauge is a sub micron thick layer whose optical properties are affected when the shock front passes through the layer. Since shock velocities are typically a few nm/ps, nanogauges can be used to study picosecond time scale shock dynamics. Using picosecond optical microscopy on targets with different thickness aluminum layers, it was found that the shock required 0.5 ns to form and then it propagated for a few ns with a constant velocity of 8.3 km/s (8.3 nm/ps), indicating a shock pressure of 49 GPa. The arrival time jitter of many hundreds of shocks, at an aluminum/polymer interface was found to be ±50 ps. The shock propagation through a polymer, polyester, was studied by observing the arrival of the front at a 50 nm thick nanogauge embedded in the polymer. When the shock was transmitted from the aluminum to a polymer layer, its velocity was 5.5 km/s, indicating a shock pressure of 14 GPa, in good agreement with shock impedance calculations. The shock target array is a flexible method of studying picosecond time scale dynamics of materials at and just behind the shock front. The use of different optical nanogauges, such as dye-doped polymer films, which can sense the temperature, pressure, and which indicate multiphonon up pumping, is briefly discussed.
    Type of Medium: Electronic Resource
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  • 5
    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.
    Type of Medium: Electronic Resource
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  • 6
    ISSN: 1520-4995
    Source: ACS Legacy Archives
    Topics: Biology , Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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  • 7
    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.
    Type of Medium: Electronic Resource
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  • 8
    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.
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 72 (1992), S. 2440-2448 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Photothermal laser ablation is studied using poly-(methyl methacrylate) films doped with a dye, IR-165, which functions as a molecular heater and thermometer. Direct optical measurements of temperature are performed on samples heated by 100 ns near-IR pulses at 1.064 μm, at rates dT/dt≈5×109 deg/s. Below ablation threshold, the heat capacity measured by optical calorimetry is precisely the value obtained by conventional calorimetry. At ablation threshold, the peak surface temperature is Tabl=600 °C. The increase in heat capacity observed above threshold, together with the results of a conventional thermal analysis, is used to determine the weight fraction of material decomposed at ablation time χth=0.02. With increasing pulse energy, the fraction decomposed increases and a more forceful ablation is observed, but the surface temperature does not continue to increase past Tlim=715 °C, which is determined to be the limiting temperature for thermal decomposition.
    Type of Medium: Electronic Resource
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  • 10
    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.
    Type of Medium: Electronic Resource
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