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  • 1
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 86 (1999), S. 2078-2082 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The electrical conductivity of semiconducting magnesium vanadate glasses has been reported for a wide composition range in the temperature range of 80–500 K. The experimental results have been analyzed in the framework of different hopping models. It has been observed that the multiphonon assisted hopping model of small polarons in the nonadiabatic regime, proposed by Emin, can interpret the temperature dependence of the conductivity data of these glasses over the entire temperature range of measurement. The parameters obtained from the fits of the experimental data to this model appear reasonable and are consistent with the glass composition. On the other hand, Mott's optical phonon assisted hopping model at high temperatures provides smaller values of the localization length. However, Mott's variable range hopping model is consistent with the low temperature data. Schnakenberg's model yields higher values of the hopping and the disorder energies than the activation energy obtained at the highest and the lowest temperature ranges. © 1999 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 3671-3676 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Metal/polymer Schottky contacts have been fabricated using electrochemically prepared free standing thin films of conducting polyaniline/polycarbonate composite as well as conducting polyaniline pellets with various metals such as Al, In, Pb and Sn. The current–voltage characteristics have been studied from room temperature down to 100 K. The data have been analyzed and interpreted on the basis of the thermionic emission mechanism. The barrier height varies from 0.6 to 0.7 V for pellet and from 0.7 to 0.8 V for composite films. There is little dependence of metal on the work function. The ideality factor is dependent on the amount of polyaniline incorporation in polycarbonate, as indicated by the shift in the carbonyl peak in the Fourier transform infrared spectrum. The abnormal decrease in barrier height and increase of ideality factor with decrease in temperature have been interpreted assuming a Gaussian distribution of barrier heights at the interface. This takes account of the nonuniformity and inhomogeneities at the interface. As in the case of inorganic semiconductor diodes, the analysis indicates an apparent decrease in zero bias height and nonlinearity in activation plots. The bias dependence of barrier height and standard deviation causing an increase in ideality factor at low temperature has also been explored. © 1999 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Plasmas 5 (1998), S. 1000-1003 
    ISSN: 1089-7674
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The well-known instability associated with the drift-ballooning modes is shown to be stabilized in the presence of a radially varying parallel flow profile. This is contrary to the usual belief that the parallel flow shear is destabilizing for the drift-like microinstabilities. The scale length of the flow profile required for this stabilization is rather modest and is usually observed in the toroidal flow profile measured during various improvement modes in the tokamak core. This shows that purely parallel flow can be used to create transport barriers to reduce the loss of particle and energy from the plasma. The improved mode formed by the parallel flow will, unlike the reverse shear mode, be nontransient in nature. © 1998 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)
    Physics of Plasmas 4 (1997), S. 3113-3116 
    ISSN: 1089-7674
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The combined effect of the perpendicular and the parallel flow curvatures on the toroidal branch of the collisionless drift waves is investigated. The full analytical stability analysis shows that the ratio of the stabilising influences of the perpendicular to the parallel flow curvature scales as α2Lv2/Ln2, where α is a numerical factor whose value is usually around 3 and Lv, Ln are respectively the velocity shear and the density variation scale length. Thus at the plasma edge (since Lv∼Ln∼ρiθ, where ρiθ is the ion poloidal gyroradius) the perpendicular flow is expected to play the major role in stabilising microinstabilities and turbulence in the improved regimes of confinement (like the high confinement-modes). However, at the plasma core (since Ln∼a(very-much-greater-than)Lv∼ρiθ, where a is the minor radius of the cross section) it is the parallel component of the flow which plays the dominant role. Furthermore, since the confinement improvement in the core is usually related to the toroidal velocity and V|| coming from the toroidal flow is much more that V⊥ coming from the toroidal flow, our result clearly indicates that it is the parallel component of the toroidal flow and not the perpendicular component, as is usually thought, that is responsible for the core confinement improvement. This conclusion is consistent with our earlier result calculated in a sheared slab configuration [S. Sen and A. Sen, Phys. Plasmas 3, 2224 (1996)]. © 1997 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Plasmas 4 (1997), S. 3731-3733 
    ISSN: 1089-7674
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The question of whether it is the shear [V(r)′] or the curvature [V(r)″] in the flow profile [V(r)] which plays the dominant role in suppressing the low-frequency (ω〈ωi, where ωi is the ion gyrofrequency) instabilities and fluctuations is investigated. Rayleigh–Taylor (RT) instability is considered in this work. The role of flow curvature is found to have a robust effect on the stability and on the radial structure of the mode. For a positive value in the flow curvature RT is suppressed whereas a negative flow curvature excites the mode. Flow shear, on the other hand, plays an insignificant role in this matter. These theoretical findings are in agreement with the recent experimental results. © 1997 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Plasmas 2 (1995), S. 777-780 
    ISSN: 1089-7674
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The effect of a radially varying poloidal velocity field on the recently found radially extended toroidal drift waves [Connor et al., Phys. Rev. Lett. 70, 1803 (1993)] is investigated analytically. The role of velocity curvature (Vθ‘) is found to have robust effects on the radial mode structure of the mode. For a positive value of the curvature [usually found in the high-(H) mode edges] the radial mode envelope, similar to the sheared slab case, becomes fully outgoing. On the other hand, for a negative value of the curvature [usually observed in the low-(L) mode edges] the characteristics of conventional drift waves return back. The radial mode envelope reduces to a localized Gaussian shape and the mode can be unstable again for typical (magnetic) shear values in tokamaks. Velocity shear (Vθ') on the other hand is found to have a rather insignificant role both in determining the radial mode structure and the stability. © 1995 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Plasmas 5 (1998), S. 2637-2641 
    ISSN: 1089-7674
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The crucial question of whether it is the shear [V(r)′] or the curvature [V(r)″] in the flow profile [V(r)], which plays the dominant role in suppressing the low-frequency (ω〈ωi, where ωi is the ion gyrofrequency) fluctuations is investigated. The role of flow curvature is found to have a robust effect on the fluctuations. For a positive value in the flow curvature, fluctuations are suppressed, whereas a negative flow curvature excites fluctuations. Flow shear, on the other hand, plays an insignificant role in this matter. These experimental findings are in complete agreement with the theoretical predictions. © 1998 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)
    Physics of Plasmas 3 (1996), S. 2224-2228 
    ISSN: 1089-7674
    Source: AIP Digital Archive
    Topics: Physics
    Notes: It has recently [S. Sen and M. G. Rusbridge, Phys. Plasmas 2, 2705 (1995)] been shown that, contrary to the usual belief, parallel flow curvature (V(parallel)″) can stabilize drift-like microinstabilities. Here the earlier work is extended to include the effect of the perpendicular flow curvature (V⊥″), which is known to have a stabilizing role on the drift-like microinstabilities. The full analytic stability analysis shows that the ratio of the stabilizing influences of the perpendicular to the parallel flow curvature scales as Ls/2Ln, where Ls and Ln are the magnetic shear and the density variation scale length, respectively. Thus, at the plasma edge (since Ls(very-much-greater-than)Ln) the perpendicular flow may play a crucial role in stabilizing microinstabilities and turbulence in the improved regimes of confinement [like the high (H) modes]. However, in the core confinement improvement [like the very high (VH) mode] both the parallel and the perpendicular flow curvatures are important, since Ls∼2Ln. Furthermore, as the confinement improvement in the core is usually related to the toroidal velocity and since V(parallel) coming from the toroidal flow is much more than V⊥ (V⊥∼εV(parallel), here ε is the inverse aspect ratio), this implies that it is the parallel component of the toroidal flow and not the perpendicular component, as is usually thought, which is responsible for the core confinement improvement. © 1996 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Plasmas 2 (1995), S. 2705-2710 
    ISSN: 1089-7674
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Earlier studies indicate that shear in the parallel flow (V(parallel)'(x)) is destabilizing for drift-like modes. Here, it is shown that taking the flow curvature (V(parallel)‘(x)) effect into account can change the picture altogether. Depending on its sign, parallel flow curvature can be both stabilizing and destabilizing. For a negative value in the curvature [usually found during the neutral beam injection (NBI) heating and the high (H)-mode edges] parallel flow has a stabilizing effect on drift waves and the mode width gets elongated. Velocity shear, on the other hand, plays an insignificant role both in determining the mode stability and its radial width. As a result, parallel flow must be considered as a viable agent in drift-like wave stabilization for achieving high confinement operation of fusion devices. © 1995 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Plasmas 5 (1998), S. 4280-4283 
    ISSN: 1089-7674
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The use of radio frequency waves is shown to stabilize drift-type waves in a tokamak if the radial profile of the radio frequency field energy is properly chosen. The estimate of the radio frequency power required for this stabilization is found to be rather modest. This result might have important implications as regards whether the use of the radio frequency waves can create a transport barrier to reduce the loss of particle and energy from the plasma. © 1998 American Institute of Physics.
    Type of Medium: Electronic Resource
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