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  • 1
    ISSN: 1520-4995
    Source: ACS Legacy Archives
    Topics: Biology , Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    Journal of the American Chemical Society 113 (1991), S. 7823-7825 
    ISSN: 1520-5126
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    Journal of the American Chemical Society 111 (1989), S. 1248-1255 
    ISSN: 1520-5126
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 92 (1990), S. 3798-3812 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A model and detailed calculations are presented to describe the flow of energy in a shocked solid consisting of large organic molecules. The shock excites the bulk phonons, which rapidly achieve a state of phonon equilibrium characterized by a phonon quasitemperature. The excess energy subsequently flows into the molecular vibrations, which are characterized by a vibrational quasitemperature. The multiphonon up pumping process occurs because of anharmonic coupling terms in the solid state potential surface. Of central importance are the lowest energy molecular vibrations, or "doorway'' modes, through which mechanical energy enters and leaves the molecules. Using realistic experimental parameters, it is found that the quasitemperature increase of the internal molecular vibrations and equilibration between the phonons and vibrations is achieved on the time scale of a few tens of picoseconds. A new mechanism is presented for the generation of "hot spots'' at defects. Defects are postulated to have somewhat greater anharmonic coupling, causing the vibrational temperature in defects to briefly overshoot the bulk. The influence of the higher defect vibrational temperature on chemical reactivity is calculated. It is shown that even small increases in defect anharmonic coupling have profound effects on the probability of shock induced chemistry. The anharmonic defect model predicts a size effect. The defect enhanced chemical reaction probability is reduced as the particle size is reduced.
    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 89 (1988), S. 830-841 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A model is presented to describe vibrational cooling (VC) in crystals of large molecules. Vibrational cooling is the process by which a vibrationally excited crystal returns to the ground state. This process may consist of many sequential and parallel vibrational relaxation (VR) steps. The model describes a highly excited, vibrationally dense molecular crystal at zero and finite temperatures. An initially excited vibration relaxes via anharmonic coupling by sequential emission of many lattice phonons until all vibrational energy is destroyed. The time evolution of vibrational excitation probability is described with a Master equation. Various models for the phonon density of states, which exerts primary control over the VR process, are considered. It is found that VC occurs on a much slower time scale than VR, and that the rate of VC is only weakly dependent on temperature, even in systems where VR is highly temperature dependent. An important conclusion of this work is that vibrational cooling is described by an ensemble averaged vibrational population distribution function which moves to lower energy states and broadens as time increases. The motion to lower energy is described by a "vibrational velocity'' (emitted energy per unit time) which is independent of temperature, while the width of the distribution increases with increasing temperature. The model is then used to calculate experimental observables including time resolved absorbance, emission, and Raman scattering following excitation of a high frequency vibration.
    Type of Medium: Electronic Resource
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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. 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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  • 7
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 93 (1990), S. 8771-8776 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The recombination after flash photolysis of carbon monoxide (CO) to protoheme (PH) in glycerol: water is studied over ten decades in time (1 ps to 10 ms). The rebinding consists of an initial nonexponential geminate phase followed by a slower exponential bimolecular phase. The entire time course of this reaction between 260 and 300 K can be explained in a unified way using a simple, analytically tractable diffusion model involving just three parameters: the relative diffusion constant, the contact radius, and the intrinsic rate of reaction at contact.
    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 90 (1989), S. 3590-3602 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Ultrafast laser experiments are conducted on low temperature crystals of pentacene in naphthalene (PTC/N) to study the process of vibrational cooling. A vibration of the excited singlet state, denoted Sν1, is excited, and the decay out of this state, as well as the subsequent arrival at the vibrationless ground state S01, are monitored by photon echoes, absorption recovery, and a new technique, pump-induced coherent Stokes Raman scattering [T.-C. Chang and D. D. Dlott, Chem. Phys. Lett. 147, 18 (1988)]. Eight vibrational modes of PTC, ranging from 260 to 1350 cm−1 are studied. The experimental results are interpreted using a previously developed model of vibrational cooling [J. R. Hill and D. D. Dlott, J. Chem. Phys. 89, 830 (1988)]. This model predicts the dependence of the vibrational cooling rate on the amount of excess vibrational energy and the temperature. The motion of the vibrational probability distribution toward the ground state is predicted to occur with a temperature independent "vibrational velocity'' which describes the rate of vibrational energy dissipation. Using the model, we fit all eight data sets with a single adjustable parameter, the vibrational velocity, and we obtain the value V0=10±2 cm−1/ps. The prediction of a nearly temperature independent V0 is confirmed over the temperature range 1.5 to 35 K. Finally, we discuss the application of these measurements to the problem of heme cooling in optically excited heme proteins.
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  • 9
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 94 (1991), S. 1825-1836 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Ultrafast spectroscopy is used to investigate the temperature dependence of a bimolecular chemical reaction occurring at reaction centers embedded in a glycerol:water glass. The reaction centers consist of carbon monoxide bound to protoheme (PH–CO), or to myoglobin at pH=3 (Mb3–CO), a protein containing PH–CO with a broken proximal histidine–Fe bond. These systems have in common a small energetic barrier for rebinding of the photodissociated ligand. In the glass, the ligand is caged, so that only geminate rebinding is possible. Rebinding is not exponential in time. For t(approximately-greater-than)20 ps, the survival fraction of deligated heme N(t)∝t−n(n≥0). Below 100 K, rebinding is dominated by an inhomogeneous distribution of activation enthalpy P(ΔH
    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 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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