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  • 1
    Online Resource
    Online Resource
    Newark :American Geophysical Union,
    Keywords: SCIENCE / Geophysics. ; Electronic books.
    Type of Medium: Online Resource
    Pages: 1 online resource (307 pages)
    Edition: 1st ed.
    ISBN: 9781118637890
    Series Statement: Wiley Works
    DDC: 551.22015118
    Language: English
    Note: Cover -- Title Page -- Copyright -- Contents -- Preface -- Acknowledgments -- List of Abbreviations -- List of Mathematical Symbols -- Part I Models -- Chapter 1 Motivation: Earthquake science challenges -- Chapter 2 Seismological background -- 2.1 Earthquakes -- 2.2 Earthquake catalogs -- 2.3 Description of modern earthquake catalogs -- 2.4 Earthquake temporal occurrence: quasi-periodic, Poisson, or clustered? -- 2.5 Earthquake faults: one fault, several faults, or an infinite number of faults? -- 2.6 Statistical and physical models of seismicity -- 2.7 Laboratory and theoretical studies of fracture -- Chapter 3 Stochastic processes and earthquake occurrence models -- 3.1 Earthquake clustering and branching processes -- 3.2 Several problems and challenges -- 3.3 Critical continuum-state branching model of earthquake rupture -- 3.3.1 Time-magnitude simulation -- 3.3.2 Space-focal mechanism simulation -- Part II Statistics -- Chapter 4 Statistical distributions of earthquake numbers: Consequence of branching process -- 4.1 Theoretical considerations -- 4.1.1 Generating function for the negative binomial distribution (NBD) -- 4.1.2 NBD distribution expressions -- 4.1.3 Statistical parameter estimation -- 4.2 Observed earthquake numbers distribution -- 4.2.1 Statistical analysis of earthquake catalogs -- 4.2.2 Observed earthquake numbers distributions -- 4.2.3 Likelihood analysis -- 4.2.4 Tables of parameters -- Chapter 5 Earthquake size distribution -- 5.1 Magnitude versus seismic moment -- 5.2 Seismic moment distribution -- 5.3 Is B ≡ 1/2? -- 5.3.1 Preamble -- 5.3.2 Catalog analysis and earthquake size distribution -- 5.3.3 Systematic and random effects in determining earthquake size -- 5.3.3.1 Scalar seismic moment errors -- 5.3.3.2 Earthquake sequences and their influence -- 5.3.3.3 Seismic moment tensor and its complexity. , 5.3.3.4 Centroid depth influence -- 5.3.4 Dislocation avalanche statistics -- 5.3.5 What are B ≡ 1 /2 consequences? -- 5.4 Seismic moment sum distribution -- 5.4.1 Simulation and analytical results -- 5.4.2 Applications to seismicity analysis -- 5.5 Length of aftershock zone (earthquake spatial scaling) -- 5.6 Maximum or corner magnitude: 2004 Sumatra and 2011 Tohoku mega-earthquakes -- 5.6.1 Maximum moment for subduction zones -- 5.6.2 Seismic moment conservation principle -- Chapter 6 Temporal earthquake distribution -- 6.1 Omori's law -- 6.2 Seismic moment release in earthquakes and aftershocks -- 6.2.1 Temporal distribution of aftershocks -- 6.2.2 Southern California earthquakes and their aftershocks -- 6.2.3 Global shallow earthquakes -- 6.2.4 Comparison of source-time functions and aftershock moment release -- 6.3 Random shear stress and Omori's law -- 6.4 Aftershock temporal distribution, theoretical analysis -- 6.4.1 Lévy distribution -- 6.4.2 Inverse Gaussian distribution (IGD) -- 6.5 Temporal distribution of aftershocks: Observations -- 6.5.1 Aftershock sequences -- 6.5.2 Temporal distribution for earthquake pairs -- 6.6 Example: The New Madrid earthquake sequence of 1811-12 -- 6.7 Conclusion -- Chapter 7 Earthquake location distribution -- 7.1 Multipoint spatial statistical moments -- 7.2 Sources of error and bias in estimating the correlation dimension -- 7.2.1 The number of earthquakes in a sample -- 7.2.2 Earthquake location error -- 7.2.2.1 Earthquake location error: the 3-D case -- 7.2.2.2 Earthquake location error: the 2-D case -- 7.2.3 Projection effect for epicentral scaling dimension -- 7.2.4 Boundary effects -- 7.2.4.1 Boundary effects: a 2-D case -- 7.2.4.2 Boundary effects: 3-D case -- 7.2.5 Inhomogeneity of earthquake depth distribution -- 7.2.6 Temporal influence -- 7.2.7 Randomness. , 7.3 Correlation dimension for earthquake catalogs -- 7.3.1 California catalogs -- 7.3.2 Global PDE catalog -- 7.4 Conclusion -- Chapter 8 Focal mechanism orientation and source complexity -- 8.1 Random stress tensor and seismic moment tensor -- 8.1.1 Challenges in stress studies -- 8.1.2 Cauchy stress distribution -- 8.1.3 Random stress tensors -- 8.2 Geometric complexity of earthquake focal zone and fault systems -- 8.2.1 Tensor invariants -- 8.2.2 CLVD sources and complexity -- 8.3 Rotation of double-couple (DC) earthquake moment tensor and quaternions -- 8.3.1 Quaternions -- 8.3.2 DC moment tensor and quaternions -- 8.4 Focal mechanism symmetry -- 8.4.1 Symmetry of DC source -- 8.4.2 DC symmetry and rotation angle -- 8.5 Earthquake focal mechanism and crystallographic texture statistics -- 8.6 Rotation angle distributions -- 8.6.1 Uniform random rotation of DC sources -- 8.6.2 Non-uniform distributions of random rotations -- 8.7 Focal mechanisms statistics -- 8.7.1 Disorientation angle statistics -- 8.7.2 Distributions of rotation axes -- 8.7.3 Rodrigues space statistics and display -- 8.7.4 Summary of results for DC orientation -- 8.8 Models for complex earthquake sources -- 8.8.1 Complex point source solutions -- 8.8.1.1 Point sources of elastic deformation in homogeneous infinite medium -- 8.8.1.2 Point sources of elastic deformation in homogeneous half-space -- 8.8.2 Higher-rank correlation tensors -- Part III Testable Forecasts -- Chapter 9 Global earthquake patterns -- 9.1 Earthquake time-space patterns -- 9.2 Defining global tectonic zones -- 9.3 Corner magnitudes in the tectonic zones -- 9.4 Critical branching model (CBM) of earthquake occurrence -- 9.4.1 Branching models -- 9.4.2 Earthquake clusters-independent events -- 9.4.3 Dependent events -- 9.4.4 Stochastic branching processes and temporal dependence. , 9.5 Likelihood analysis of catalogs -- 9.5.1 Statistical analysis results -- 9.5.2 Comparison of results with the ETAS model -- 9.6 Results of the catalogs' statistical analysis -- Chapter 10 Long- and short-term earthquake forecasting -- 10.1 Phenomenological branching models and earthquake occurrence estimation -- 10.2 Long-term rate density estimates -- 10.2.1 Low-resolution forecasts -- 10.2.2 High-resolution global forecasts -- 10.2.3 Smoothing kernel selection -- 10.2.4 Comparing long-term forecasts -- 10.3 Short-term forecasts -- 10.4 Example: earthquake forecasts during the Tohoku sequence -- 10.4.1 Long- and short-term earthquake forecasts during the Tohoku sequence -- 10.4.2 Long-term earthquake rates for the Tokyo region -- 10.5 Forecast results and their discussion -- 10.6 Earthquake fault propagation modeling and earthquake rate estimation -- 10.6.1 Earthquake extended rupture representation and earthquake rate estimation -- 10.6.2 Earthquake fault propagation modeling -- Chapter 11 Testing long-term earthquake forecasts: Likelihood methods and error diagrams -- 11.1 Preamble -- 11.2 Log-likelihood and information score -- 11.3 Error diagram (ED) -- 11.3.1 Relation between the error diagram and information score -- 11.3.2 Two-segment error diagrams and information score -- 11.3.3 Information score for GCMT and PDE catalogs -- 11.4 Tests and optimization for global high-resolution forecasts -- 11.5 Summary of testing results -- Chapter 12 Future prospects and problems -- 12.1 Community efforts for statistical seismicity analysis and earthquake forecast testing -- 12.1.1 Community Online Resource for Statistical Seismicity Analysis (CORSSA) -- 12.1.2 Collaboratory for the Study of Earthquake Predictability (CSEP): Global and regional forecast testing -- 12.2 Results and challenges -- 12.3 Future developments -- References -- Index.
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  • 2
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 89 (2001), S. 5944-5948 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We report on a high-resolution transmission electron microscopy and energy-dispersive x-ray spectroscopy study of the microstructure of CdTe thin films epitaxially grown on single-crystal hexagonal CdS and cubic CdTe substrates. We find that the different structures of the substrates do not make a great structural difference on the grown CdTe films; i.e., on both substrates, the grown CdTe films have a cubic structure and high density of planar defects near the interface regions. At the CdTe/CdS interface, interdiffusion occurs, forming CdTe1−xSx and CdS1−xTex alloys. These alloys lead to significantly reduced mismatch at the interface.© 2001 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)
    Journal of Applied Physics 85 (1999), S. 5393-5395 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Single crystals of Ln1−x−ySrxPbyMnO3 (Ln: La, Pr, or Nd) with sizes up to 3 cm3 have been obtained using a flux solution of PbF2 and PbO at the temperature range between 917 and 1300 °C. The content of Pb was found to range between 0.26≤y≤0.43, depending upon the growing temperature, i.e., the higher the temperature, the lower the Pb content. Transmission electron microscopy studies provided evidence of a nanostructural behavior for Nd0.67Sr0.01Pb0.32MnO3. The crystals exhibit a sharp transition of ferromagnetic metallic to paramagnetic insulating behavior. Resistance measurement was performed in a magnetic field of 0, 2 and 7 T, respectively. © 1999 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)
    Journal of Applied Physics 89 (2001), S. 4564-4569 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: In this work, we found that the interdiffusion of the CdS and Zn2SnO4 (ZTO) layers can occur either at high temperature (550–650 °C) in Ar or at lower temperature (400–420 °C) in a CdCl2 atmosphere. By integrating a Zn2SnO4 film into a CdS/CdTe solar cell as a buffer layer, this interdiffusion feature can solve several critical issues and improve device performance and reproducibility of both SnO2-based and Cd2SnO4-based CdTe cells. Interdiffusion consumes the CdS film from both the ZTO and CdTe sides during the device fabrication process and improves quantum efficiency at short wavelengths. The ZTO film acts as a Zn source to alloy with the CdS film, which results in increases in the band gap of the window layer and in short-circuit current density Jsc. Interdiffusion can also significantly improve device adhesion after CdCl2 treatment, thus providing much greater process latitude when optimizing the CdCl2 process step. The optimum CdCl2-treated CdTe device has high quantum efficiency at long wavelength, because of its good junction properties and well-passivated CdTe film. We have fabricated a Cd2SnO4/Zn2SnO4/CdS/CdTe cell demonstrating an NREL-confirmed total-area efficiency of 15.8% (Voc=844.3 mV, Jsc=25.00 mA/cm2, and fill factor=74.82%). This high-performance cell is one of the best thin-film CdTe solar cells in the world. © 2001 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 67 (1995), S. 2554-2556 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The structure of high angle boundaries in the (BiPb)2Sr2Ca2Cu3Ox system, which is compositional and structurally modulated along the boundaries, was investigated by high resolution electron microscopy. These compositional variable boundaries tend to facet onto the (001) plane, leaving steps of height equal c/2 for the (BiPb)2Sr2CuOx and (BiPb)2Sr2Ca1Cu2Ox phases with amorphous material at the corners of these steps. These data suggest a weak link is formed at high angle boundaries where there are such lower Tc or insulating phases. © 1995 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)
    Journal of Applied Physics 70 (1991), S. 5940-5940 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The effects of a magnetic underlayer on the magnetic behavior of overlayer/underlayer combinations were investigated. Permalloy underlayers of 100 nm thickness and composition 82% Ni-18% Fe by weight were sputter deposited on 3-in.-diam Si substrates. Magnetic orientations of the underlayers were set at 0°, 45°, and 90° with respect to the orientation of a subsequently plated Permalloy (79%Ni-21%Fe overlayer. Several film combinations were generated on each of the various underlayer configurations with plated thicknesses ranging from 0.1 to 2.0 μm. Spatial maps of magnetic orientation and Hk for underlayers and underlayer/overlayer combinations were collected using a modified Kerr BH imager (Kerr BHI) designed from Gudeman.1 The maps covered a 5 cm×5 cm square region with 5 mm spacing between points. Comparison of the maps before and after plating shows a partial reduction in the measured Hk values for film systems with large underlayer/overlayer orientation differences. A uniform decline in the effect of the underlayer to the overall orientation direction as film thicknesses increase was also observed.
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 75 (1999), S. 1961-1963 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The atomic structure of a planar defect with a (001) habit plane in single crystal layered perovskite SrBi2Ta2O9 is determined by high-resolution Z-contrast imaging. We found that the defect forms a structure, with two Sr–Ta–O perovskite blocks connected by a metallic Sr2 plane, rather than a Bi2O2 layer as in the perfect crystal. This defect is expected to be an efficient hole trap and may have important implications for the electronic properties and the ferroelectric response of the SrBi2Ta2O9 material. © 1999 American Institute of Physics.
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  • 8
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 94 (1991), S. 997-1005 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A microscopic theory for ultrafast coherent Raman spectroscopy of polyatomic molecules in condensed phases is developed. For off resonant excitation, an effective Hamiltonian that controls the molecular dynamics in a Raman process is derived. The limitations of the driven oscillator model are clarified, and generalized equations of motion, which hold for resonant and off resonant excitation, are derived. Spectral selectivity using pulse shaping is discussed.
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 93 (1990), S. 4501-4509 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Dynamic light scattering from highly concentrated colloidal systems with a narrow distribution of particle sizes can be interpreted in terms of the sum of two independent modes due, respectively, to collective diffusion and polydispersity fluctuations; a general formalism has been presented for calculating the relative mode amplitudes for hard spheres in the Percus–Yevick approximation [Pusey, Fijnaut, and Vrij, J. Chem. Phys. 77, 4270(1982)]. This work extends the relative mode amplitude calculation to the general case where optical (i.e., refractive index) and size polydispersity are completely coupled such as in water-in-oil microemulsions. To develop the theory a concentric core-shell hard sphere model is adopted, in which particles possess a continuous variation in the core sizes but have constant shell thickness, thus giving rise to a distribution in the particle refractive indices. A new "measured'' static structure factor SM(0) is derived, and applied to the calculation for the relative amplitude of the slow mode, A2/(A1+A2), as a function of solvent refractive index n0. A strong enhancement of the slow mode is predicted as the optical matching point is approached. The theory also shows that the dependence of A2/(A1+A2) on n0 is very sensitive to the extent of polydispersity, but rather insensitive to the distribution function used. Neglect of the nonuniformity in particle refractive index can cause a substantial overestimate of the size polydispersity. We have used our extended treatment to interpret the dynamic light scattering data from concentrated water-in-oil microemulsions formed from H2O, AOT, and apolar solvents using solvent composition to control the contrast in refractive index. It is found that the AOT-stabilized water microemulsion droplets have a size polydispersity of about 6.5%, which is smaller than previously thought.
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    New York, NY : American Institute of Physics (AIP)
    Physics of Fluids 1 (1989), S. 2495-2501 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A relativistic fluid theory is constructed to analyze the inverse Compton scattering of an unmagnetized counterpropagating plasma wave by a cold relativistic electron beam. A Langmuir wave and electromagnetic plasma wave wigglers are considered, and the properties of the two types of wigglers are comparatively discussed. The growth rates are comparable to those of the ac free-electron laser and the free-electron lasers with magnetostatic wigglers in the Raman regime.
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