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  • 1
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The electron diffraction intensity of cyclobutane was measured and analyzed conjointly with the rotational constant, B0=0.355 82(11) cm−1, determined by an analysis of FTIR spectra of the ν14 (CH2 scissoring, B1g) and ν16 (CH2 rocking, A2u) bands. The rz structure was determined to be rz (C–C)=1.552±0.001 A(ring), rz (C–H)=1.093±0.003 A(ring), αz ((angle)HCH)=106.4±1.3°, and the ring dihedral angle, θz =27.9±1.6°; the rg distances of the C–C and C–H bonds are 1.554±0.001 and 1.109±0.003 A(ring), respectively. The uncertainties represent estimated limits of error. The rocking angle βz between the bisectors of the adjacent H–C–H and C–C–C angles was found to be 6.2±1.2°, the axial C–H bonds in the 1,3 positions being tilted towards each other. The coefficient of coupling of the ring-puckering and CH2-rocking motions was estimated to be βz/θz =0.22±0.05. The combination and difference sideband structures appearing in the ν14 band due to the puckering mode ν6 were analyzed. The puckering energy levels thus obtained were consistent with the existing data. A double-minimum potential function for the puckering mode was determined by taking into account the coupling of the puckering motion with the CH2-rocking motion. The potential gave the zero-point vibrational average value of the ring dihedral angle, 27.5±1.1°, which agreed with that determined in the ED–IR joint analysis mentioned above. The puckering potential for C4D8 was found to be consistent with that for C4H8 when the coupling between the puckering and the rocking motions was considered.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 92 (1990), S. 5963-5974 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: State-to-state elastic and inelastic angular distribution and time-of-flight measurements are reported for the scattering of He*(21S) by Ne in crossed supersonic atom beams at four collision energies in the range 0.6–2.8 kcal/mol. The inelastic collision products He+Ne*(nl), where nl=3d', 4p, 4p', 5s, 5s', and 4d, are scattered predominantly forward with respect to the direction of incidence, except for endothermic states near threshold. The data are analyzed with a numerically exact multichannel curve-crossing model that yields good agreement with experimental cross section branching fractions and total quenching and state-to-state rate constants as well as the angular measurements. The model suggests the importance of intermediate "chaperone'' states, in which the excited electron is temporarily trapped in a d or f Rydberg Ne orbital, in channeling flux into the 4s' and 5s' upper laser states of Ne by energy transfer from He*(2s1,3S).
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  • 3
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 90 (1989), S. 7118-7126 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: He*(23S)+Ne differential elastic scattering measurements in crossed supersonic beams over the energy range 0.6–2.8 kcal/mol are combined with total cross section velocity dependence and quenching rate constant temperature dependence to determine a 3×3 potential matrix characterizing a double curve-crossing model for the collision dynamics and energy transfer. The coupled radial Schrödinger equations are integrated numerically to yield the appropriate cross sections. At low energy (E〈4 kcal/mol) a mixed adiabatic/diabatic two-state model derived from the potential matrix accurately represents the data. Dynamics in the three-state model, which is topologically similar to non-adiabatic coupling involving charge transfer, is discussed, and the bearing of the model on collisional pumping of the HeNe 1.1 μ laser is assessed.
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  • 4
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 89 (2001), S. 4772-4776 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The surface structures of an oxide overlayer on Nb(100) single crystal formed by numerous cycles of Ar-ion sputtering and flash annealing at 1973 K in an ultra-high-vacuum chamber have been investigated by scanning tunneling microscopy. Flat terraces with a monatomic step height of Nb(100) are observed; where two orthogonal domains are alternately evident. A ladder-like (3×10) structure of Nb(100) with no long-range order is identified at atomic resolution in the domain on the terrace. The ladder-like (3×10) structure is interpreted to be a modulated NbO2(010) overlayer on the Nb(100) surface and an atomic structural model of the ladder-like (3×10) structure is proposed. © 2001 American Institute of Physics.
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  • 5
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 72 (1992), S. 2652-2658 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: For the numerical simulation of electron cyclotron resonance plasma production, a two-dimensional model that describes wave propagation and plasma transport is developed. The modeling code calculates profiles of electromagnetic wave fields, power absorption of electrons, and temporal evolution of plasma densities in a bounded, inhomogeneous, cylindrical system. The calculation of the plasma production in a mirror magnetic field shows that the plasma production property is very sensitive to the antenna location.
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  • 6
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Transient spectra following the v=1←0 excitation of the OH stretching mode of Brønsted acidic hydroxyl groups in normal and deuterated mordenite zeolites have been measured by a two-color picosecond pump–probe technique. When the OH and OD stretching bands were excited by resonant IR pulses, transient bleaching of the fundamental band (v=1←0) and the transient hot band (v=2←1) absorption signal were observed. For the OH and OD groups free of adsorbates, the spectral widths of the pump-induced signals were broadened by ∼4 cm−1 due to pure dephasing from the convoluted width of the pump and probe IR pulses. When the OH and OD groups were adsorbed by a Xe atom, the frequencies of the ν(OH) and ν(OD) bands shifted to lower frequency and at the same time the widths of both the transient bleaching and the transient hot band absorption were much broader than those of the isolated hydroxyl groups by the factor of more than three. Actually, the widths of the transient signals were about the same as those of the linear absorption signals. An adiabatic approximation has been employed to interpret the observed broadening/shift of the IR bands by making use of the results of DFT (density functional theory) calculations performed on a model cluster consisting of a Xe atom and an H3Si–(OH)–AlH3 substrate. The result agreed well with the observed spectral features. © 1996 American Institute of Physics.
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  • 7
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 79 (1996), S. 1801-1806 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Current–Voltage (I–V) characteristics of GaAs/AlAs double-barrier resonant tunneling diodes (RTDs) with a Si-planar-doped barrier are studied. At 4.2 K the peak-to-valley current ratio decreased when Si was introduced to the barrier next to the electrode from which electrons are emitted (emitter barrier). On the other hand, the ratio did not decrease considerably when Si was introduced to the other barrier, i.e., next to the electrode into which electrons flow (collector barrier). To investigate the origin of the decrease in the peak-to-valley ratio, we evaluated the transmission coefficient experimentally, and found that the resonance transmission widths for the double-barrier RTDs are almost the same. This means that the reduction in the peak-to-valley current ratio is not caused by the broadening of resonance transmission width. To explain why the peak-to-valley current ratio is degraded, we then introduced a new model in which an excess current flows through donor levels in the emitter barrier. To confirm this model, we investigated the I–V characteristics of GaAs/AlAs single-barrier diodes. We found an excess current, which is probably due to a tunneling current through the donor level created in the barrier, when the barrier is planar-doped. It is, therefore, concluded that the decrease in the peak-to-valley current ratio observed for the RTD with the doped emitter barrier is due to this excess current flowing through the doped emitter barrier. © 1996 American Institute of Physics.
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  • 8
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 71 (1992), S. 2408-2413 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Piezoelectric photoacoustic (PA) measurements on liquid-encapsulated-Czochralski-grown n-GaAs were carried out at room temperature. A continuous broad band below 1.35 eV and a peak at 1.383 eV were observed in the PA amplitude spectra. By comparing with the optical-absorption spectra, it is concluded that the broad band is due to the electron transition involving the EL2 deep-lying defect levels. For the observed peak at 1.383 eV, the origin is considered to be dislocation related. The possibility that this peak is an apparent one expected from the proposed models for the PA signal generation is denied.
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  • 9
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Plasmas 2 (1995), S. 3539-3540 
    ISSN: 1089-7674
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The discrepancy in the expression for quasi-linear ponderomotive force as obtained by Klima and Petrazilka [Czech. J. Phys. B 30, 1002 (1980)] and by Fukuyama et al. [Phys. Fluids B 5, 539 (1993)] are resolved by showing that the extra terms in the expression of Klima and Petrazilka are due to fluid helicity of the fluctuations. © 1995 American Institute of Physics.
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  • 10
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Plasmas 1 (1994), S. 1154-1158 
    ISSN: 1089-7674
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Power partition and energy dissipation rates are examined for a self-sustained stationary turbulence of a high-n ballooning mode in a tokamak plasma. It is found that the power to excite fluctuations is almost equally transferred to perpendicular ion motion and to parallel electron motion. The ratio of the thermalized power, which excites and sustains the turbulence, to the total power lost by energy diffusion is found to be of the order of the broken symmetry parameter, i.e., the inverse aspect ratio, a/R. The dissipation rates of the fluctuations due to the thermal conductivity, the electron viscosity, and the ion viscosity are also calculated separately. The dissipation is dominated by that associated with the thermal conductivity. The relation between the induced global flux and the microscopic dissipation is also derived. It is found that a fractional part of order a/R of the dissipated power is effective in sustaining the turbulent modes.
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