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  • 1
    Digitale Medien
    Digitale Medien
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 110 (1999), S. 9230-9234 
    ISSN: 1089-7690
    Quelle: AIP Digital Archive
    Thema: Physik , Chemie und Pharmazie
    Notizen: The paper is based on mid-frequency Raman scattering data of neat diamino poly(propylene imine) dendrimer molecule DAB(CN)64; time correlation functions were obtained from a band profile analysis of its fundamental CN mode near 2246 cm−1 at four temperatures between 300 and 123 K; lattice relaxation processes were found to be governed by a stretched exponential modulation function with dispersion parameter α=0.90±0.05 (300 K) and 0.85 (123 K) and corresponding time constant τ0=0.78 and 1.15 ps, respectively. The results suggest that the fast fluctuations of the molecular environment of the CN end groups of the dendrimer system regain equilibrium by independent, parallel pathways with Poisson relaxation times τ that show a broader distribution at lower system temperatures. The results imply that the shape and width of the CN band contour are generated by a vibrational dephasing process in the intermediate modulation regime, under inseparable contributions of intra- and intermolecular oscillator–lattice coupling. © 1999 American Institute of Physics.
    Materialart: Digitale Medien
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  • 2
    Digitale Medien
    Digitale Medien
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 100 (1994), S. 3869-3871 
    ISSN: 1089-7690
    Quelle: AIP Digital Archive
    Thema: Physik , Chemie und Pharmazie
    Notizen: We have extended the Raman spectral accumulations of the ν3 mode (A1, 367 cm−1) of liquid CHCl3–Cl-35 and its simulation in terms of an orientational equilibrium renewal process [W. G. Rothschild, R. M. Cavagnat, and P. Maraval, J. Chem. Phys. 99, 8922 (1993)] to a temperature of 338 K, about the normal boiling point of the system (335 K). The values of the best-fit parameters predict that the orientational motion of liquid chloroform, even at such a relatively high kinetic energy, is described predominantly by libratory states; their lifetime (∼1 ps) is four times longer than that of the free-rotational steps. The character of the orientational motion of the system, when traversing the range of 213 to 338 K from just above its melting to near its boiling point at about atmospheric pressure, reflects the softening of the liquid-cage structure in terms of an increasing dispersion and/or a decreasing value of the mean libration frequency, a lowering of the depth of its potential well, but near-invariance of its lifetime. Simultaneously, there is an approximately twofold increase in the lifetime of the much shorter stages of free-rotational motion. In essence, the system dynamics remain that of an assembly of librators.
    Materialart: Digitale Medien
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  • 3
    Digitale Medien
    Digitale Medien
    s.l. : American Chemical Society
    Macromolecules 1 (1968), S. 43-47 
    ISSN: 1520-5835
    Quelle: ACS Legacy Archives
    Thema: Chemie und Pharmazie , Physik
    Materialart: Digitale Medien
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  • 4
    Digitale Medien
    Digitale Medien
    s.l. : American Chemical Society
    Macromolecules 5 (1972), S. 37-41 
    ISSN: 1520-5835
    Quelle: ACS Legacy Archives
    Thema: Chemie und Pharmazie , Physik
    Materialart: Digitale Medien
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  • 5
    Digitale Medien
    Digitale Medien
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 87 (1987), S. 7293-7299 
    ISSN: 1089-7690
    Quelle: AIP Digital Archive
    Thema: Physik , Chemie und Pharmazie
    Notizen: The stretched ("extended'' or "fractional'') exponential, exp{−(t/T)α}, where 0〈α≤1 and T (ps) a time constant, is introduced as a modulation function for a vibrational T2 process in order to describe the non-Markovian dynamics of the bath of amorphous systems in the picosecond domain. The theory simulates well published dephasing data of probe oscillators in concentrated aqueous solutions of KSCN, molten mixtures of Li and Rb nitrates, and of polycrystalline and smectic phases of the liquid crystal 4-n-octyloxy-4'-cyanobiphenyl. The temperature and phase dependence of dispersion parameter α follows an accepted model of constrained-sequential relaxation with a scale-invariant ("fractal'') distribution of relaxation times.
    Materialart: Digitale Medien
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  • 6
    Digitale Medien
    Digitale Medien
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 83 (1985), S. 4338-4343 
    ISSN: 1089-7690
    Quelle: AIP Digital Archive
    Thema: Physik , Chemie und Pharmazie
    Notizen: We have analyzed the VV- and VH-Raman band profiles of the N–O symmetric stretching fundamental of the nitrate anion of 1 mol/l NaNO3 (or LiNO3) in Li+Cl−-enriched aqueous solutions for the liquid phase between 263 and 353 K and for the vitreous state at 77 K. From the observed isothermal correlation time of the orientational mobility of the C3 axis of NO−3 in Li+-rich solution and from the band asymmetry of the corresponding isotropic profile at increasing temperature, we propose an endothermic local-structure-reforming process that favors incorporation of a few Li+ ions into the solvation sphere of the anions. The vitreous state of 1 mol/l LiNO3 or NaNO3 in the LiCl-rich systems, which shows considerable local order about the nitrate anion, is conceptualized as a percolation cluster of solvated cation–anion interaction that breaks up into cluster distributions for the liquid phase.
    Materialart: Digitale Medien
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  • 7
    Digitale Medien
    Digitale Medien
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 99 (1993), S. 8922-8928 
    ISSN: 1089-7690
    Quelle: AIP Digital Archive
    Thema: Physik , Chemie und Pharmazie
    Notizen: Our paper presents a fit of an orientational equilibrium renewal process in terms of a sequence of random events of free rotational motion and libratory oscillations [Lindenberg and Cukier, J. Chem. Phys. 62, 3271 (1975)] to new pure-rotational spectra and correlation data of the ν3 mode (367 cm−1) of liquid chloroform–Cl-35 at 300 and 213 K. The model fits are good; they account fully for the frequently observed (but rarely well-simulated) partial regain of the memory of the orientational coherence at intermediate time domains. Further, the physical-statistical picture of the nature of the orientational motion turns out to be that of a librator in a potential-well of a strongly temperature-dependent depth; stages of free rotation are significant but one order of magnitude shorter than the oscillatory regimes, even at room temperature and at ambient pressure. This contrasts notions of rotational motion hitherto held for such systems. Second, we explored the rotational correlation data of the C–H stretching mode ν1, which exhibits much faster vibrational relaxation than mode ν3, to ascertain empirically effects of significant vibration-rotation coupling in ν1. We find that this effect is significant for the longer time domains only. Finally, we report low-frequency depolarized Raman spectra (5–200 cm−1) at 212, 243, 273, and 295 K. They yield a temperature dependence of the peak-frequencies of the reduced Raman intensity (density-of-vibrational-states) which can only be reconciled with a predominance of librational motion within the liquid cage.
    Materialart: Digitale Medien
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  • 8
    Digitale Medien
    Digitale Medien
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 98 (1993), S. 3571-3573 
    ISSN: 1089-7690
    Quelle: AIP Digital Archive
    Thema: Physik , Chemie und Pharmazie
    Notizen: We report low-frequency Raman spectra of the title compounds in their metastable solid state quenched rapidly from the high-temperature liquid. The phonon-like spectra indicate crystal-like order superposed on a vibrational density-of-states background. The results imply "order through fluctuation'' effects via autocatalytic and inhibitory growth.
    Materialart: Digitale Medien
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  • 9
    Digitale Medien
    Digitale Medien
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 95 (1991), S. 2072-2079 
    ISSN: 1089-7690
    Quelle: AIP Digital Archive
    Thema: Physik , Chemie und Pharmazie
    Notizen: We describe the temperature dependence of the inhomogeneously broadened CN Raman profile I(ω) at ωc ∼2230 cm−1 of the title compounds (n=1, 6, 8, 9, 11, 12) in their isotropic liquid phase and solutions (CHCl3, CCl4) by simulating the oscillator amplitude correlation function by a vibrational equilibrium renewal process in terms of random fluctuations of the oscillator transition frequency ω(t)=ωc +ω1(t) about its central value ωc. To this effect, the autocorrelation function of the frequency shift ω1(t) is expressed as a probability density function (PDF) Fˆ(t) of recurrence times of the stochastic motional narrowing events in the local environment of the CN oscillators. System-related physical meaning and satisfactory data fit is obtained if Fˆ(t) is understood as an expansion in terms of parallel, independent exponential relaxation processes with characteristic times τ that are distributed by a PDF ρα(τ)=〈τ〉h(τ)/τ, where α is the dispersion parameter of the extended exponential and 〈τ〉 the expectation of τ. Width and ranges of h(τ) show strong molecule–molecule clustering, possibly indicating a trend with alkyl chain length. At temperatures just above the mesophase–liquid-phase transition, the range of the prevalent relaxation times τ in the local environment of the CN oscillators is of the order of 1–4 ps. Only at temperatures near 570 K or by high dilution in the solvents are the inter- and intracluster forces sufficiently diminished to approximate those of ordinary fluids. We consider our method to give a realistic description of the dynamics of types of macroscopically isotropic fluids where, nevertheless, the shape, size, and polarity of their molecules lead to a degree of aggregation that weakens the identity and the influence of constituent members. The temporary structure of the macroscopically isotropic fluids in the liquid-crystal systems is best understood by admitting a significant presence of randomly distributed local regions of dynamic nematicity, causing temperature-dependent relaxation pathways over 10–50 A(ring) distances.
    Materialart: Digitale Medien
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  • 10
    Digitale Medien
    Digitale Medien
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 89 (1988), S. 6454-6460 
    ISSN: 1089-7690
    Quelle: AIP Digital Archive
    Thema: Physik , Chemie und Pharmazie
    Notizen: In this paper we further explore the applicability of a vibrational T2 process based on the extended-exponential modulation model [Rothschild, Perrot, and Guillaume, J. Chem. Phys. 87, 7293 (1987)] to Raman correlation data of concentrated aqueous solutions of LiSCN and KSCN [Kato¯, Mol. Phys. 48, 1119 (1983); Kato¯ and Takenaka, Mol. Phys. 46, 257 (1982)]. In general, the values of dispersion parameter α in the modulation function exp[−(t/τ)α], obtained from the fit of the theory to the isotropic correlation data of the CN oscillator, predict the prevalence of interrelated, collective dynamic processes in the medium that are the cause of the instantaneous oscillator transition frequency shifts (motional narrowing). In particular we predict, from the observed concentration dependence of α, strong short-time (fraction to several ps) cation–water–anion interactions that, in the more concentrated LiSCN–H2O systems at 303 K, are above a site percolation threshold with a value of α∼0.3 (close to that found in glasses). The expectation value of t, 〈t〉=τΓ(1+1/α), becomes critical near a concentration of 5 mol/l and shows a pronounced Vogel–Fulcher-type temperature dependence (T0=250 K) in the 10 mol/l LiSCN–H2O system over a range 0.45–76 ps. However, since α approaches its limiting value=1 at the highest temperature reported (353 K), the large-cluster cation–water–anion distributions in LiSCN–H2O must be rather tenuous. In contrast, the characteristics of α and of 〈t〉 for the KSCN–H2O systems agree with the relatively weak cation–water forces; the (inverse) concentration dependence of α is linear, its temperature dependence is flat, and the Vogel–Fulcher-type temperature behavior of 〈t〉 for the 10 mol/l solution stretches merely from 0.7 to 1.4 ps.
    Materialart: Digitale Medien
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