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  • 1
    Online Resource
    Online Resource
    AIP Publishing ; 2006
    In:  Journal of Applied Physics Vol. 100, No. 12 ( 2006-12-15)
    In: Journal of Applied Physics, AIP Publishing, Vol. 100, No. 12 ( 2006-12-15)
    Abstract: A semiclassical double-well model of dielectric relaxation current in glasses is extended to (i) nonzero temperature, (ii) complex bias histories, and (iii) strong electric fields. At finite temperature, thermal excitation yields a contribution linear in temperature, which adds to the temperature-independent contribution from tunneling from the zero-temperature case. Both contributions vary linearly with applied field and have a time dependence of 1∕tn. Experimental measurements in three different glasses are shown to agree with this prediction, and it is shown how to use such measurements to estimate the material parameters t0 and σ0. For complex bias histories, a principle of superposition is found, as observed experimentally, if the applied fields are weak compared to the material parameter E0, estimated to be on the order of 107V∕m. For an electric field pulsed periodically from 0 to E, the current can be decomposed into a fast contribution due to particles tunneling back and forth every cycle of the field, and a slow residual contribution whose time dependence is the same as that for a continuous bias, but whose magnitude is reduced by the duty cycle of the periodic bias. For a sinusoidal electric field, thermal excitation gives a contribution to the dielectric constant that varies linearly with temperature and has a real part that varies logarithmically with frequency and an imaginary part that varies as the inverse tangent of frequency. For tunneling, both parts are independent of temperature and vary approximately as the logarithm of frequency, a dependence observed experimentally and almost indistinguishable from that suggested by the 1∕tn current response to a step voltage. For strong electric fields, the current that flows after the field is removed is found to be dominated by particles that fell forward when the field was on. Since particles fall forward quickly but tunnel back slowly, even strong fields applied for a short period of time can produce a large, long-lasting return current. These analyses lead to a number of testable predictions, and should be useful for understanding the phenomenon of dielectric relaxation and its impact on electronic devices.
    Type of Medium: Online Resource
    ISSN: 0021-8979 , 1089-7550
    Language: English
    Publisher: AIP Publishing
    Publication Date: 2006
    detail.hit.zdb_id: 220641-9
    detail.hit.zdb_id: 3112-4
    detail.hit.zdb_id: 1476463-5
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  • 2
    In: Applied Physics Letters, AIP Publishing, Vol. 119, No. 24 ( 2021-12-13)
    Abstract: Qubits made from superconducting materials are a mature platform for quantum information science application, such as quantum computing. However, material-based losses are now a limiting factor in reaching the coherence times needed for applications. In particular, knowledge of the atomistic structure and properties of the circuit materials is needed to identify, understand, and mitigate material-based decoherence channels. In this work, we characterize the atomic structure of the native oxide film formed on Nb resonators by comparing fluctuation electron microscopy experiments to density functional theory calculations, finding that an amorphous layer is consistent with an Nb2O5 stoichiometry. Comparing x-ray absorption measurements at the Oxygen K edge with first-principles calculations, we find evidence of d-type magnetic impurities in our sample, known to cause impedance in proximal superconductors. This work identifies the structural and chemical composition of the oxide layer grown on Nb superconductors and shows that soft x-ray absorption can fingerprint magnetic impurities in these superconducting systems.
    Type of Medium: Online Resource
    ISSN: 0003-6951 , 1077-3118
    RVK:
    Language: English
    Publisher: AIP Publishing
    Publication Date: 2021
    detail.hit.zdb_id: 211245-0
    detail.hit.zdb_id: 1469436-0
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  • 3
    Online Resource
    Online Resource
    AIP Publishing ; 2004
    In:  Applied Physics Letters Vol. 84, No. 18 ( 2004-05-03), p. 3489-3491
    In: Applied Physics Letters, AIP Publishing, Vol. 84, No. 18 ( 2004-05-03), p. 3489-3491
    Abstract: We show that a straightforward account of dielectric relaxation current in glasses follows from a semiclassical treatment of the double-well model [P. W. Anderson, B. I. Halperin, and C. M. Varma, Philos. Mag. 25, 1 (1972) and W. A. Phillips, J. Low Temp. Phys. 7, 351 (1972)] explaining the linear specific heat of glasses at low temperature. The current is obtained from the field-induced tunneling of the glass between the minima of its potential energy surface, and is found to have the experimentally observed linear dependence on field and inverse dependence on time. The effects of temperature and prior biases are briefly discussed, as well as the relation of the model to the theory of charge trapping. No dielectric relaxation is expected in a perfect insulating crystal, raising the important technological question of how perfect high-k dielectrics like HfO2 and ZrO2 must be in order to serve as gate dielectrics in transistors.
    Type of Medium: Online Resource
    ISSN: 0003-6951 , 1077-3118
    RVK:
    Language: English
    Publisher: AIP Publishing
    Publication Date: 2004
    detail.hit.zdb_id: 211245-0
    detail.hit.zdb_id: 1469436-0
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  • 4
    Online Resource
    Online Resource
    AIP Publishing ; 2015
    In:  The Journal of Chemical Physics Vol. 142, No. 9 ( 2015-03-07)
    In: The Journal of Chemical Physics, AIP Publishing, Vol. 142, No. 9 ( 2015-03-07)
    Abstract: A coarse-grained simulation method to predict nuclear magnetic resonance (NMR) spectra of ions diffusing in porous carbons is proposed. The coarse-grained model uses input from molecular dynamics simulations such as the free-energy profile for ionic adsorption, and density-functional theory calculations are used to predict the NMR chemical shift of the diffusing ions. The approach is used to compute NMR spectra of ions in slit pores with pore widths ranging from 2 to 10 nm. As diffusion inside pores is fast, the NMR spectrum of an ion trapped in a single mesopore will be a sharp peak with a pore size dependent chemical shift. To account for the experimentally observed NMR line shapes, our simulations must model the relatively slow exchange between different pores. We show that the computed NMR line shapes depend on both the pore size distribution and the spatial arrangement of the pores. The technique presented in this work provides a tool to extract information about the spatial distribution of pore sizes from NMR spectra. Such information is difficult to obtain from other characterisation techniques.
    Type of Medium: Online Resource
    ISSN: 0021-9606 , 1089-7690
    Language: English
    Publisher: AIP Publishing
    Publication Date: 2015
    detail.hit.zdb_id: 3113-6
    detail.hit.zdb_id: 1473050-9
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  • 5
    Online Resource
    Online Resource
    AIP Publishing ; 2002
    In:  Journal of Applied Physics Vol. 92, No. 8 ( 2002-10-15), p. 4431-4440
    In: Journal of Applied Physics, AIP Publishing, Vol. 92, No. 8 ( 2002-10-15), p. 4431-4440
    Abstract: We use tight-binding theory to investigate the electronic contribution to dielectric susceptibility in thin films and interfaces of covalent materials. We begin by describing the effects of an electric field on the elemental unit of a covalent material, the bond. Then, we show how the responses of individual bonds can be added up to obtain an estimate of the susceptibility of a bulk material. In doing so, we see that the polarization of a material can be viewed as arising from the transfer of charge from one side of the system to the other, and that this viewpoint leads naturally to a local definition of susceptibility in semiconductors. Using this concept, we examine dielectric susceptibility in thin films and interfaces, with a Si/Ge/Si heterostructure serving as an example. The interesting feature of thin films and interfaces is that they exhibit spatial variations in susceptibility, which we attribute to: (i) elastic distortions; (ii) the creation of bonds at an interface which are of a type not found in either bulk material; and (iii) the coupling of a bond to neighboring antibonds different than those in the bulk material. We then ask what error is introduced by neglecting these local variations when calculating the capacitance of a multilayer dielectric. For the Si/Ge/Si heterostructure, we find that effect (iii) introduces only small errors, even for very thin Ge layers, because the decrease in susceptibility on the Ge side of an interface is offset by the increase in susceptibility on the Si side. Similarly, effect (ii) is small because the polarizability of the Si–Ge bonds at the interface is very nearly the average of that for Si and Ge. On the other hand, effect (i) does lead to noticeable errors, but these errors can be removed almost entirely by choosing the permittivity of the Ge layer to be that of bulk Ge under the same state of strain as the Ge layer in the heterostructure. We conclude by interpreting recent experiments on “high-k” dielectrics in term of what we have learned here. [C. M. Perkins et al., Appl. Phys. Lett. 78, 2357 (2001); M. Koyama et al., Tech. Dig. Int. Electron Devices Meet., 459 (2001); W.-J. Qi et al., ibid., 145 (1999)].
    Type of Medium: Online Resource
    ISSN: 0021-8979 , 1089-7550
    Language: English
    Publisher: AIP Publishing
    Publication Date: 2002
    detail.hit.zdb_id: 220641-9
    detail.hit.zdb_id: 3112-4
    detail.hit.zdb_id: 1476463-5
    Location Call Number Limitation Availability
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  • 6
    Online Resource
    Online Resource
    AIP Publishing ; 2001
    In:  Journal of Applied Physics Vol. 90, No. 9 ( 2001-11-01), p. 4570-4577
    In: Journal of Applied Physics, AIP Publishing, Vol. 90, No. 9 ( 2001-11-01), p. 4570-4577
    Abstract: We present a tight-binding model of Zr silicate in the limit that every Zr and Si atom is bonded to four O atoms. We view the material as being composed of small, relatively uncoupled collections of atoms, called bonding units, with stoichiometries SiSiO4 and ZrSiO4. The SiSiO4 bonding unit constitutes a model for pure SiO2, and the ZrSiO4 bonding unit represents the fundamental element distinguishing tetrahedral Zr silicate from pure SiO2. In the first part of this article we look at the electronic structure of “ideal” bonding units in which the O atoms are arranged in a perfect tetrahedron and the M–O–Si angle is 180° (M=Si or Zr). We find the valence levels of both bonding units to be dominated by O p states, and the lowest conduction levels of the ZrSiO4 bonding unit to derive primarily from Zr d states, whose energy depends sensitively upon the charge transfer to the O atoms. The energy gap of the ideal ZrSiO4 bonding unit is found to be 5.9 eV, compared to 8.0 eV for the SiSiO4 bonding unit. Finally, for the ZrSiO4 bonding unit, we present a simplification which allows the energy levels of the ZrSiO4 bonding unit to be obtained approximately in terms of decoupled Zr–O and Si–O interactions. In the next part of the article we investigate how bond angle and bond length distortions affect the electronic structure of the ZrSiO4 bonding unit. In particular, we note that significant distortions of the Zr–O–Si angle could produce Zr-based localized states that could act as traps for electrons tunneling through the material. In the last part of the article we discuss the basic principles governing band lineups for Si/silicate interfaces constructed by substituting Zr atoms for Si atoms on the SiO2 side of crystalline Si/SiO2 interfaces. We calculate the band lineups as a function of Zr concentration for one particular interface.
    Type of Medium: Online Resource
    ISSN: 0021-8979 , 1089-7550
    Language: English
    Publisher: AIP Publishing
    Publication Date: 2001
    detail.hit.zdb_id: 220641-9
    detail.hit.zdb_id: 3112-4
    detail.hit.zdb_id: 1476463-5
    Location Call Number Limitation Availability
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