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  • 1
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 100 (1994), S. 357-361 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The ion–molecule reaction OH−+H2CO→H3O−+CO has been studied at 300 K with isotopic labeling of reactants. The H3O− product is only observed in small abundance because the ion dissociates into OH−+H2 upon multiple collisions in a helium buffer gas. Without isotopic labeling, the pseudo-first-order kinetics plots for the reactions of OH− with H2CO and OD−+D2CO were found to be curved as a result of the regeneration of OH− or OD− reactant. A scavenger technique was used to remove the H3O− (or D3O−) produced prior to dissociation, to reveal the true first-order attenuation of OH− (or OD−) in reaction with H2CO (or D2CO). The rate constant for the OH−+H2CO reaction is 7.6×10−10 cm3 s−1, and for OD−+D2CO is 5.7×10−10 cm3 s−1. For the isotopically mixed cases OH−+D2CO and OD−+H2CO, the rate constants are equal to 1.3×10−9 cm3 s−1, about twice as large as those for the reactions involving only a single hydrogen isotope, indicating that isotopic exchange is an important process. The rate constants for the thermal dissociation of H3O− and D3O− in helium were found to be 1.6×10−12 and 1.1×10−12 cm3 s−1, respectively, within a factor of 2. The results are discussed in terms of other thermal dissociation reactions of ions.
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  • 2
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 76 (1994), S. 7075-7077 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Polarized neutron reflectometry measurements were carried out on a thin-film Co-Re multilayer sample with Re thickness of 6 A(ring) which is at the peak of the first oscillation of the magnetoresistance. Antiferromagnetic coupling between successive Co layers is observed at in-plane magnetic fields below 0.1 T. Towards the low field end of this regime, the axes of the antiferromagnetic domains are distributed relatively uniformly in the sample plane but at ∼0.1 T the moments flop perpendicular to the applied field. As the field is increased further, the Co moments are pulled into the field direction producing a partial ferromagnetic alignment. At 0.5 T, the highest field where the measurements have been made, the antiferromagnetic to ferromagnetic transition was found to be only ∼50% complete, indicating that the saturation field required for Co-Re system is much higher than that for Co-Cu multilayers of similar layer spacing.
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  • 3
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 75 (1994), S. 6554-6556 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Structural properties of sputtered Si/Re 50 A(ring)/(Co 20 A(ring)/Re x A(ring))40 superlattices have been investigated in detail by low- and high-angle x-ray-diffraction measurements. The low-angle x-ray reflectivity data have been analyzed using an optical model and the high-angle data have been treated on the basis of a trapezoidal model. The fitted results indicate that the films with small xRe=3, 5, and 7 A(ring) are essentially composed of pure Co layers and Re rich alloy (∼80%) interfaces about 3–5 monolayers thick. The magnetoresistance (MR) data of the antiferromagnetically coupled films have been analyzed using a semiclassical MR model of interfacial spin-dependent scattering.
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  • 4
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 73 (1993), S. 5530-5532 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We have studied the effect of annealing on the magnetic and structural properties of sputtered Si/Re50 A(ring) [Co20 A(ring)/RexA(ring)]40 superlattices with xRe=3,5,7,10 A(ring). Annealing the samples for 1 h at 300 °C causes a slight increase in interfacial mixing and a contraction of lattice spacing d(002) owing to interdiffusion and structural relaxation, as indicated by the x-ray diffraction data. In addition, the subsequent room-temperature magnetoresistance (MR) increases for samples with antiferromagnetic (AF) coupling, by up to 20% for xRe=5 A(ring), providing strong experimental evidence for the spin-dependent scattering mechanism which predicts an increasing MR with increasing diffuse interface scattering. A further 1 h anneal at 525 °C provokes dramatic interdiffusion between the Co and Re layers, which is accompanied by a considerable decrease of the MR, indicating a disappearance of the interlayer AF coupling.
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  • 5
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The reaction between N2 and Dy2Fe17 has been studied by thermopiezic analysis on 20–25 μm sized powders in the temperature range 400–500 °C. Partially nitrided powders were analyzed using CuKα x-ray diffraction and thermomagnetic techniques. Both high angle x-ray and thermomagnetic data show only the presence of Dy2Fe17 and Dy2Fe17N3−δ (δ〈0.3) with no evidence of intermediate compositions. The results of the x-ray diffraction experiments at several Bragg peaks were simulated using a two phase model structure: a Dy2Fe17 core with a Dy2Fe17N3 surface layer. The results show that at low temperatures the nitride layer is too thin to account for all of the nitrogen absorbed by the sample, indicating that a significant amount of the nitrogen diffused into the core of the particles, presumably along grain boundaries.
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  • 6
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Structural and magnetoresistance results on annealed sputtered (Ni81Fe19, Ni66Fe16Co18)/Ag granular multilayers are presented. Structural evolution has shown that highly (111) textured, discontinuous layered structures can persist on annealing up to 400 °C. The average magnetic particle size is controlled by the annealing temperature and the initial magnetic layer thickness. No giant magnetoresistance was observed in the as-deposited films, while significant MR was found after annealing between 300 °C and 400 °C. Magnetoresistance over 30%, together with a small saturation field, was found at 4.2 K for a starting magnetic thickness of 4 A(ring). Increasing the magnetic layer thickness to 20 A(ring) greatly improves the magnetic thermal stability, and leads to high magnetoresistive sensitivities of up to 0.35%/Oe in a field of 10 Oe at room temperature. The magnetization hysteresis, anisotropy, and magnetic interaction in such a granular multilayer are also discussed.
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  • 7
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Cumulative interface roughness and its influence on the magnetization process in antiferromagnetically coupled (Ni80Co20/Cu)×N multilayers is studied. In these multilayers, Cu and Ni80Co20 thicknesses are fixed at 20 and 15 A(ring), respectively, in order to obtain the antiferromagnetic coupling at the second oscillation peak of giant magnetoresistance (GMR) versus Cu thickness. Low-angle x-ray reflectivity measurements show that cumulative interface roughness increases with increasing bilayer number N. In-plane magnetization hysteresis measured with both SQUID and surface magneto-optic Kerr effect (SMOKE) magnetometers are compared. When the cumulative interface roughness is significant, SMOKE hysteresis loops, which are sensitive to the top 5 or 6 magnetic layers, display a nonlinear plateau region at small fields. Comparison of low-angle x-ray, and SMOKE results show that interfaces of relatively high quality in top layers only exist for sputtered multilayer with N〈10.
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  • 8
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The Krätschmer–Huffman carbon-arc method of preparing fullerenes has been used to generate carbon-coated transition metal (TM) and TM-carbide nanocrystallites. The magnetic nanocrystallites were extracted from the soot with a magnetic gradient field technique. For TM=Co the majority of nanocrystals exist as nominally spherical particles, 0.5–5 nm in radius. Hysteretic and temperature-dependent magnetic response, in randomly and magnetically aligned powder samples frozen in epoxy, correspond to fine particle magnetism associated with monodomain TM particles. The magnetization exhibits a unique functional dependence on H/T, and hysteresis below a blocking temperature TB. Below TB, the temperature dependence of the coercivity can be expressed as Hc=Hc0[1−(T/TB)1/2], where Hc0 is the 0 K coercivity.
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  • 9
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 69 (1991), S. 1183-1191 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The effect of a gas cooling system on the efficiency of an average-power solid-state disk laser amplifier is addressed. Such a configuration has application in solid-state fusion drivers. Analytical models are discussed that identify the important parameters in specifying an optimized laser and optimized cooling system. It is shown that the penalty that the cooling and conditioning system power requirements have on the overall laser system efficiency can be easily maintained below 10%, particularly for large-aperture systems.
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 65 (1989), S. 2195-2198 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The problem of the scattering by air which has been locally heated by aerosols irradiated by a short pulse, for example, by a pulsed laser, is addressed through the use of the heat conduction equation and scattering theory. The resulting air scattering cross section increases as with the square of the absorbed fluence. After a pulse, it increases to a maximum and then decays as the inverse of time. For absorbed fluences greater than 2 J/cm2, the air scattering cross section can exceed that of the aerosol itself. For multiple irradiation pulses, the air scattering cross section reaches a maximum asymptotic limit. For an aerosol cloud, the air scattering cross section decays exponentially after the thermal wave from an aerosol reaches one-third of the interparticle spacing.
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