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  • 1995-1999  (666,058)
  • 1820-1829  (1,232)
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  • 301
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 6373-6380 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A numerical analysis of the influence of air entrainment into the plasma jet on the thermal plasma characteristics is performed to provide a design basis for nontransferred plasma torches operated in an ambient air of atmospheric pressure along with shroud gas injection. The assumption of steady-state, axisymmetric, local thermodynamic equilibrium, and optically thin plasma is adopted in a two-dimensional modeling of thermal plasma flow with an annular shroud gas shell. A control volume method and a modified semi-implicit pressure linked equations revised algorithm (known as SIMPLER) are used for solving the governing equations, i.e., the conservation equations of mass, momentum, and energy along with the equations describing the so-called K–ε model for flow turbulent kinetic energy (K) and its dissipation rate (ε), and the mass fraction equations for gas mixing. The two-dimensional distributions of temperature and flow velocity of the thermal plasma jet as well as the air mole fraction mixed with the plasma are found in an exterior jet expanding region outside the torch, and they are compared for the two cases with and without shroud gas injection. As a result of calculations, the flow rate of the injected shroud gas and the location of its injector turn out to be major parameters for controlling ambient air entrainment. The calculations also reveal that the annular injection of shroud gas surrounding the plasma jet reduces air entrainment into the plasma jet remarkably while it does not significantly affect the plasma temperature and velocity. The present numerical modeling suggests the optimum design and operating values of an argon shroud gas injector for minimizing air entrainment into the thermal plasma flame ejected from the nontransferred plasma torch operated at normal pressure in the ambient atmosphere. © 1999 American Institute of Physics.
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  • 302
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 6415-6420 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A three-dimensional quasi-steady-state mathematical model is presented for laser heating with a multimode beam. The effects of laser beam scanning direction on the melt pool shape are investigated through the conduction analysis without phase change. The maximum temperature is found to be behind the center of the focal spot due to advection. The isotherms ahead of the focal spot bunch together and spread apart behind the focal spot on the surface of the workpiece due to the same effect. The temperature profile shows four distinct peaks as a result of four intensity peaks. Scanning direction affects the melt pool shape which needs to be considered for high precision cutting applications such as integrated circuit cutting. The melt pool shape is found to be symmetric about the x axis in the x-y plane and z axis in the y-z plane for the scanning angles φs=0° and −90°, however it is asymmetric for other scanning angles. © 1999 American Institute of Physics.
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  • 303
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 6434-6439 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The complex dielectric constants of Zr0.98Hf0.02TiO4 ceramics are reported in the frequency range 10−3–1010 Hz for the temperature range 830 °C≤T≤860 °C, just above the commensurate-incommensurate phase transition temperature, Tc. The disappearance of x-ray satellite reflections at 825 °C was used to determine Tc experimentally. The dielectric measurements show that a relatively narrow distribution of relaxation times is present in the ceramics, which broadens as the temperature approaches Tc from above. By analyzing the temperature at which the dielectric constant is a maximum as a function of frequency using the Vogel-Fulcher relationship, an activation energy of 550±15 kb,where kb is the Boltzmann constant, and an effective freezing temperature, Tf, of 825 °C have been determined, confirming that, to within experimental error, Tf coincided with Tc. The experimental results for Zr0.98Hf0.02TiO4 are interpreted in terms of a possible dipole-glass-like phase that has been proposed for relaxor systems. © 1999 American Institute of Physics.
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  • 304
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 6462-6469 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The microstructure and properties of Cu films containing insoluble Mo in as-deposited and annealed conditions have been studied. Using magnetron sputtering, Cu films with Mo concentrations up to 25 at. % have been deposited. The Cu-Mo films consist of nonequilibrium supersaturated solid solutions of Mo in Cu and have nanocrystalline microstructures. Upon heating, most of the films studied undergo three major transition events: recovery, crystallite growth and coalescence, and grain growth. Recovery occurs at ∼220–250 °C due to the release of strain energies stored during deposition, while the growth and coalescence of crystallites at ∼490 °C are likely driven by the crystallite-boundary reduction. Upon further annealing at above ∼670 °C, the microstructure alters considerably in most of the films, resulting in extensive growth of crystallites and grains. Rather high strain energies are thought to cause the precipitation of Cu particles in the molybdenum-rich Cu-Mo films (e.g., Cu-25 at. % Mo) during annealing at a temperature as low as 200 °C. The fine structure observed in the 800 °C-annealed Cu-25 at. % Mo film suggests that the extensive crystallite/grain growth is effectively impeded by the presence of molybdenum, signifying a good property of thermal stability. The film's resistivity and hardness properties correlate well with the microstructure and are governed by the impurity effect of molybdenum. Low-molybdenum Cu-Mo films yield relatively low resistivity, and this is attributable to the improved film microstructure. Hardness results indicate that the strengthening of the films is mainly due to the fine structure and presence of molybdenum. © 1999 American Institute of Physics.
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  • 305
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    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 6492-6496 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: This article describes an approach to the heteroepitaxy of lattice mismatched semiconductors, that we call nanoheteroepitaxy. The theory developed here shows that the 3D stress relief mechanisms that are active when an epilayer is nucleated as an array of nanoscale islands on a compliant patterned substrate, will significantly reduce the strain energy in the epilayer and extend the critical thickness dramatically. Calculations show that with the scale of patterning that is achievable with advanced lithography (10–100 nm) we can eliminate mismatch dislocations from heterojunctions that are mismatched by as much as 4.2%. © 1999 American Institute of Physics.
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  • 306
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    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 6506-6514 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The grating formation speed in photorefractive polymers is greatly reduced by highly polar molecules incorporated by necessity in large concentrations to produce large diffraction efficiency and two-beam energy coupling gain. The random electric fields generated by these dipoles interfere with charge transport by increasing the width of the hopping site energy distribution and thus greatly reducing the carrier mobility and the photorefractive speed. We conducted transport studies of several model systems consisting of combinations of two polymer binders, six charge transport agents (four for holes and two for electrons), and varying concentrations of two highly polar electro-optic chromophores. The results confirm that carrier mobility is greatly reduced in the presence of polar molecules in accordance with the predictions of models of hopping transport in the presence of dipolar disorder. The randomly positioned and oriented dipoles increase the width of the hopping site energy distribution by an amount proportional to the square root of the dipole concentration and to the strength of the dipole moment. The results also show that transport agents with smaller dipole moments reduce the sensitivity to the dipolar effect. The photorefractive speed may therefore be increased by using transport agents with small dipole moments. © 1999 American Institute of Physics.
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  • 307
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 6530-6538 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We present an improved method to analyze simultaneously the current–voltage and capacitance–voltage characteristics of metal–insulator–semiconductor (MIS) diodes. We use the method to study the effect of Zn doping concentration on the current transport in Au MIS contacts fabricated on In0.21Ga0.79As layers grown by metalorganic vapor phase epitaxy on highly doped GaAs substrates. At room temperature and for low reverse bias voltage, the generation/recombination process via mid-gap traps is the only dominant mechanism in these MIS diodes. For high reverse bias, both this mechanism and thermionic-field emission control current transport. The generation/recombination current observed is due to donor type mid-gap traps whose density shows an almost linear dependence with Zn concentration. The value of the barrier height at zero bias and at room temperature (φb0=0.73 V±12%) is independent of the Zn concentration. For the procedure used to prepare the In0.21Ga0.79As:Zn surfaces, the thickness of the oxide layer and the transmission coefficient of holes across this layer depend on the Zn doping concentration in the range 7×1014≤NA≤5×1018 cm−3. Zn doping seems to inhibit the formation of the unintentional native oxide on the surface of In0.21Ga0.79As epilayers. © 1999 American Institute of Physics.
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  • 308
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    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 6563-6566 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We have grown thin films of (100)-oriented La0.67(CaxSr1−x)0.33MnO3 on (100) NdGaO3 substrates by off-axis sputtering. We have looked at the changes in the resistivity and magnetoresistance of the samples as the Ca/Sr ratio was varied. We find that as the calcium fraction is decreased, the lattice match to the substrate decreases, and the films become more disordered, as observed in transport measurements and the variation in Curie and peak resistance temperatures. We find a correlation between the temperature independent and T2 terms to the low temperature resistivity. The room temperature magnetoresistance exhibits a maximum as the peak temperature is increased by the substitution of Sr for Ca, and a change in the field dependence to the resistivity at room temperature is observed.© 1999 American Institute of Physics.
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  • 309
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    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 6858-6865 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The highest efficiencies of Cu(In, Ga)Se2 (CIGS) thin film solar cells have been achieved when incorporating a thin CdS buffer layer grown by chemical bath deposition (CBD). The reason for this success has recently been discussed in terms of a pure Cd-doping effect in the CIGS layer. Such a model suggests that the bulk properties of the CBD-CdS buffer layer would be of minor importance. In this work, CBD-CdS layers having different bulk properties (i.e., concentrations of incorporated impurities) were employed in a number of CIGS solar cells. To further explore the bulk versus interface properties, half of these CIGS devices were subjected to a pre-deposition of an additional intermediate ultrathin layer. Moreover, CIGS devices made with CBD-CdS layers of different thickness were fabricated. Both standard and temperature dependent current–voltage (I–V) measurements were performed. The results indicate that the bulk properties of the CBD-CdS buffer layer indeed play an important role in the formation of the CdS/CIGS heterojunction. By increasing the impurity concentration or the thickness of the CBD-CdS layer, the open-circuit voltage Voc was observed to substantially increase. This favorable effect was counteracted by the appearance of a crossover effect in the I–V characteristics for devices with the highest impurity concentration or thickness of the CBD-CdS layer. The pre-deposition of an ultrathin layer did not affect these results. The presence of the crossover effect was strongly correlated to the appearance of trap-assisted tunneling in addition to the thermally assisted tunneling. The observed crossover effect was suggested to originate from too high a number of impurities (defect states) in the bulk of the CdS layer. © 1999 American Institute of Physics.
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  • 310
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 6904-6906 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We have numerically investigated the behavior of stacks of long Josephson junctions considering a nonuniform bias profile. In the presence of a microwave field the nonuniform bias, which favors the formation of fluxons, can give rise to a change of the sequence of radio-frequency induced steps. The amplitude of the steps is enhanced when the external frequency matches the fluxon shuttling regime. © 1999 American Institute of Physics.
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  • 311
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    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 6898-6903 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: In order to increase the failure temperature of Ta diffusion barrier for Cu, we investigated the effect of a thin V insertion layer (100 Å) into Ta film with/without ion bombardment on Ta diffusion barrier performance in Cu metallization. When the Ta/V/Ta diffusion barrier was deposited without concurrent ion bombardment, the insertion of the thin V layer into Ta film was not effective to improve the barrier performance of Ta film, because of the thermal instability of the Ta/V/Ta multilayer caused by the reaction between the Ta/V/Ta films and Si substrate. Meanwhile, when the Ta/V/Ta diffusion barrier was deposited with ion bombardment, the insertion of the thin V layer into Ta film improved barrier properties significantly. This was attributed not only to the densification of grain boundaries in Ta/V/Ta films, but also to the formation of two thermally stable sharp interfaces between Ta and V by ion bombardment, resulting in the reduction of the fast diffusion of Cu through Ta/V/Ta films. © 1999 American Institute of Physics.
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  • 312
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    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 6920-6922 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A phenomenological model is proposed to explain quantitatively the interesting compositional dependence on the Ge incorporation rate during low-temperature growth of Si1−xGex by disilane and solid-Ge molecular beam epitaxy, based on enhanced hydrogen desorption from Si sites due to the presence of Ge atoms. The hydrogen desorption rate constant for disilane on Si sites is fitted to an exponential function of Ge incorporation rate and a possible physical explanation is discussed. Simulated results are in excellent agreement with experimental data. © 1999 American Institute of Physics.
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  • 313
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 6932-6934 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We report on a strong piezoresistive effect in AlN–GaN short-range superlattices. The measured static gauge factor varies from 30 to approximately 90 depending on the superlattice composition. These values are substantially larger than the values of the gauge factor reported for GaN–AlN–GaN semiconductor–insulator–semiconductor structures. The measured data are in good agreement with the results of the calculation accounting for the piezoelectric effect. Our results demonstrate a high potential of AlN–GaN-based materials for the development of piezoelectric and piezoresistive sensors. © 1999 American Institute of Physics.
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  • 314
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    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 3960-3965 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The speed of conversion of infrared (IR) images by a planar semiconductor gas discharge system into the visible range has been investigated. Argon or nitrogen are used in the discharge gap having an electrode distance of 100 μm. Using pulse radiation from an IR laser to excite the system, we have shown that the characteristic response time of the device with the cryogenic discharge in the gap can lie in the submicrosecond range. This characteristic of the system can be applied for a fast IR imaging at a rate higher than 106 frame/s. © 1999 American Institute of Physics.
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  • 315
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 6567-6570 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Beryllium-doped InP layers have been grown by solid source atomic layer molecular beam epitaxy at low substrate temperature. The residual n-type doping was reduced by controlling both the amplitude and the length of the phosphorus pulse. We have shown a well controlled p-type doping and obtained a hole concentration in the range 4×1017–3×1019 cm−3 at room temperature. The electrical and optical properties of InP layers grown at low temperatures were investigated by Hall effect and photoluminescence (PL) measurements. PL spectra for lightly doped samples have a near band emission at 1.41 eV and Be-related emissions around 1.38 eV. © 1999 American Institute of Physics.
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  • 316
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4003-4009 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The growth of GaS films on GaAs(001) surfaces by using thermal evaporation of layered-compound GaS has been investigated by Auger electron spectroscopy, low-energy electron-loss spectroscopy (LEELS), x-ray photoemission spectroscopy (XPS), and atomic force microscopy (AFM) as a function of deposition temperature. The LEELS spectrum of the films grown at lower temperatures (≤400 °C) resembles that of a GaS single crystal, whereas that of the films grown at 450 °C reveals that GaAs surface was terminated by Ga2S3 layer. XPS spectra suggest that after annealing at 500 °C, S atoms moved from As atoms to Ga atoms to form stable Ga–S bonds at the interface and As–S bonds are observed to be less stable. The band discontinuity at the GaS/GaAs(001) interface estimated by XPS showed the straddling-type I band alignment. Surface morphology of the films studied by AFM reveals the layer-by-layer initial growth of GaS. © 1999 American Institute of Physics.
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  • 317
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4032-4039 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A spectroscopic ellipsometry technique is used to attempt a quantitative analysis of thin Si/SiO2 nanocomposite films obtained by magnetron co-sputtering. The layers are first fabricated with varying values of deposition temperature and sputtered silicon area, before being annealed at different temperatures. Using an effective medium model, the ellipsometry tool allowed the estimate of the thickness and the volume fraction of silicon agglomerates or grains, in addition to the optical parameters of the layer through a tentative determination of the dielectric function of the Si nanostructures. The Si content obtained by the ellipsometry approach agrees with those previously determined by direct measurements. Besides the obvious increase of incorporated Si with the sputtered area of this material, we noticed a maximum excess of Si for a deposition temperature in the 400–500 °C range. In this respect, the peak position of the photoluminescence (PL) detected only in the annealed samples is found to be closely connected with the amount of excess Si, and in consequence, with the mean size of the thermally grown nanocrystallites. The systematic red shift of maximum PL with the rise of Si content, and implicitly with the increase of the particle size, regardless of the deposition conditions used for the fabrication of the original layer, is liable to allow conclusive argument as for the attribution of the PL in the 1.30–1.65 eV range to the quantum confinement effect. Besides the main contribution of the nanoparticle density, the quality of the Si/SiO2 interface, as examined by infrared absorption spectroscopy, appears determining for the PL efficiency, and is increasingly improved towards stoichiometric SiO2 when the annealing temperature is increased up to 1100 °C. © 1999 American Institute of Physics.
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  • 318
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4071-4075 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Nanoscale In0.53Ga0.47As/In0.52Al0.48As multiquantum wells structures were studied by photocurrent spectroscopy. Photocurrent spectra showed clear steplike structures accentuated by exciton peaks. Many interband transitions were assigned from the spectral structure. As peaks of forbidden transitions, which appeared in large reverse bias voltages, were extrapolated to zero bias voltage on the photocurrent spectra, transition energies were estimated in a square potential well. New estimation methods of valence band parameters, heavy hole effective mass and valence band offset, were derived from a saturation of the heavy hole subband in the valence potential well, using the envelope function model in the effective mass approximation. The heavy hole effective mass in a direction normal to the quantum well plane and the valence band offset were 0.38m0 and 0.22 eV. © 1999 American Institute of Physics.
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  • 319
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4091-4095 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Low-frequency noise measurements have been carried out at room temperature in polycrystalline semiconducting iron disilicide (β-FeSi2) thin film with the current I as a parameter. The power spectral density of the current fluctuations exhibits a 1/f behavior at low frequencies (f〈100 Hz) and is proportional to Iβ (β〈2). The temperature dependence of the conductivity shows that, at room temperature, the measured noise is related to a thermally activated transport mechanism, which satisfies the Meyer–Neldel rule. A noise theory has been developed on the basis of trapping-detrapping of holes of the valence band and the gap states taking into account mobility inhomogeneity across the thickness of the film. Using the experimental data of Hall, conductivity, and noise measurements, the noise model provides an assessment of the distribution of traps within the energy gap of the β-FeSi2 material. © 1999 American Institute of Physics.
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  • 320
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4127-4130 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The giant magnetoimpedance (GMI) effect in films with a sandwiched structure has been studied. FeNiCrSiB/Cu/FeNiCrSiB sandwiched films with a magnetic closed-loop structure were deposited onto a glass substrate by rf sputtering and then annealed at an optimum temperature. GMI ratios as large as 63% and 77% were obtained at 13 MHz in longitudinal and transverse fields, respectively. The ratios are almost twice as large as those obtained in FeNiCrSiB single films. © 1999 American Institute of Physics.
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  • 321
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4160-4164 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Energy transfer processes from Yb3+ to Tm3+ ions have been investigated in various fluoride microcrystals to examine the application limit of a simple rate equation model and to obtain methods for characterizing the host materials as to energy transfer. It has been shown that the energy transfer coefficients from donor Yb3+ to acceptor Tm3+ ions differ by nearly one order of magnitude even for fluoride lattices that have similar luminescence characteristics. The energy transfer coefficients increase monotonically with Yb3+ concentration at low Yb3+ concentrations, while they take nearly constant values at high Yb3+ concentrations. The present experimental results were compared with computer simulation results as well as related analyses. It is shown that the apparently complicated behaviors are consistently explained by a microscopic model. As an example of the application of the present results, the optimization of the infrared emission of Tm3+ ions is shown. © 1999 American Institute of Physics.
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  • 322
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4171-4175 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Effect of surface nonradiative recombination on kinetics and total yield of the interband photoluminescence (PL) of c-Si wafers excited at room temperature by short laser pulses is studied. Numerical simulations show that a correlation of the PL quenching with the surface defect density takes place even at the high excitation level in spite of Auger recombination in the bulk. The quantum yield of PL reaches some percent for Si wafers with low bulk and surface defect concentrations. The calculations are confirmed by the experimental correlation between the PL quenching with the density of interface states (Dit) at the Si/SiO2 interface which has been obtained by conventional capacitance–voltage measurements. The express characterization of the Dit of Si surfaces by the pulsed PL can be carried out for the defect density in the range from 108 to 1014 cm−2 at room temperature. © 1999 American Institute of Physics.
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  • 323
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: In order to analyze the particle generation and its effect on the SiO2 thin film in an atmospheric pressure chemical vapor deposition (APCVD) process using four organic silicon vapors and ozone gas, gas-phase particle generation, growth, transportation and vapor-cluster/particle codeposition processes were studied experimentally and theoretically using a flow-type vertical tube reactor. Decomposition reaction rates of four organic silicon vapors (tetraethylorthosilicate, triethoxysilane, tetramethylorthosilicate, and octamethylcyclotetrasiloxane) due to the O⋅oxidation were determined by arranging the number concentrations of the generated particles in Arrhenius plots. The obtained activation energies and frequency factors of reaction rate constants were used to simulate the vapor-cluster/particle codeposition in the CVD process. In the numerical simulation, computational fluid dynamics equations (continuity, momentum, and energy conservation equations) were solved to evaluate the gas velocity, vapor concentration, and temperature profile inside the reactor. Particle population balance equations based on discrete-sectional presentation for the particle size spectrum were solved coupling with diffusion equations of vapors and clusters/particles. This numerical simulation code could explain the vapor-cluster/particle codeposition in the thin film preparation by the APCVD process. The film growth rate and the surface morphology of the film could be reasonably explained by the deposition flux and the size of deposited clusters/particles obtained as numerical simulation results, respectively.© 1999 American Institute of Physics.
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  • 324
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4238-4242 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The effects of the substrate bias voltage and the deposition temperature on the electrical characteristics and the 1/f noise of TiNx/n-Si Schottky diodes fabricated by reactive magnetron sputtering are investigated. As the substrate bias voltage varies from −40 to −100 V, the ideality factor of the diodes remain almost unchanged whereas the noise intensity as a function of the current shows a shift parallel by about one order of magnitude. At low current levels, the noise intensity is proportional to the current and is attributed to the mobility and diffusivity fluctuation. At higher current levels, the noise intensity is proportional to the square of the current and is attributed to bulk traps mainly near the interface. Analysis of the noise measurements shows that both the Hooge parameter and the bulk trap density near the interface first are increased and then decreased as the negative substrate bias voltage increases from −40 to −100 V. This is in contrast with the effects of the deposition temperature where we found that the Hooge parameter remains almost constant, while both the ideality factor and the interface states density are decreased as the deposition temperature increases from room temperature to 400 °C. The trap properties of the TiNx/n-Si Schottky diodes are correlated with the stoichiometry of the TiNx films investigated by spectroscopic ellipsometry measurements. © 1999 American Institute of Physics.
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  • 325
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4262-4264 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Amorphous GeO2 has been grown by plasma assisted anodic oxidation at temperatures ≤100 °C. The growth kinetics can be explained in terms of a constant current anodization model. Infrared absorption spectroscopy has been used to characterize the transverse and longitudinal optic vibrational modes of the oxide network. Values are displaced with respect to bulk oxide due to geometrical optic effects and plasma induced network structure variation. In relaxed GeO2 we estimate the mean Ge-O-Ge bridging bond angle to be 〉123° and the full width at half peak height of the bond angle distribution is ∼14°. Electrical measurements on thin oxide capacitors suggest that in 25 nm oxides there are ≤2×1011 negative charges cm−2 and negligible interface state densities. © 1999 American Institute of Physics.
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4292-4294 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Topographically induced in-plane magnetic anisotropy has been observed in CoCrTa and CoCrPt films deposited onto oxidized silicon substrates which are lithographically patterned with fine grooves of period 200–320 nm and amplitude 20–50 nm. The coercivity and remanence are higher parallel to the grooves. Anisotropy has been observed in both rf- and dc-magnetron sputtered films with a (112¯0) preferred orientation, which is achieved by growth at elevated temperature on a (200)-oriented Cr underlayer at low base pressures. Anisotropy increases with the amplitude of the grooves in the silica substrate. © 1999 American Institute of Physics.
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  • 327
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4301-4303 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Magnetization reversal processes in Fe–Pt(001) thin films prepared by a high-pressure sputter deposition method were studied. Samples were classified in four types of domain patterns. Type I, with maze-like domain patterns, has a mixing mode of nucleation and wall motion for magnetization reversal. While, type II, with large island domain patterns, shows wall motion in its magnetization reversal. Type III has small island domain patterns, and type IV has fine discrete domain patterns showing rotational modes with inclined M–H loops. Type IV is expected to be one of the candidates for future ultrahigh-density magnetic recording media with high resolution and low noise. © 1999 American Institute of Physics.
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  • 328
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4316-4318 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Nanocomposite films were made consisting of Co nanoparticles, with coatings of amorphous Al2O3. Nanoparticles were deposited on room-temperature substrates by sputtering in 0.10–0.20 Torr Ar. Transmission electron microscope images showed average Co particle sizes between 70 and 223 Å, for different sputtering rates and pressures. Selected-area electron diffraction and x-ray diffraction showed that the particles had a fcc structure for sizes ≤122 Å and a mixture of fcc and hcp phases for larger sizes. Magnetization measurements on a sample with 122 Å mean-particle size showed significant hysteresis at room temperature, with a coercivity of 390 Oe. At 10 K, the coercivity increased to 3145 Oe, and a loop shift of 2020 Oe was measured when the sample was field cooled. This indicates a fraction of the Co was oxidized by reaction with the Al2O3 coating, resulting in a surface layer of antiferromagnetic Co oxide. © 1999 American Institute of Physics.
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  • 329
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4313-4315 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Thin film media with and without a NiAl seedlayer were sputter deposited over a range of substrate temperatures. Two distinctly different crystallographic and recording performance behaviors were observed. For the samples deposited with the NiAl seedlayer, which promotes the Co(10.0)/Cr(112) crystallographic orientation, the media noise was relatively low and constant throughout the temperature range investigated, whereas there was a significant reduction in noise with increasing temperature of deposition for the conventional media which have the Co(11.0)/Cr(200) structure. As a result an increase of more than 7 dB in signal-to-noise ratio was observed over the temperature range of 120–260 °C. The results suggest that the degree of Cr segregation with temperatures strongly depends on grain structures, such as grain size, grain size distribution, and grain crystallographic orientation. Magnetic characterization of both media is correlated to their recording performance as a function of substrate temperatures. © 1999 American Institute of Physics.
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  • 330
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4010-4023 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Laser interference crystallization of amorphous silicon (a-Si) thin films, a technique that combines pulsed laser crystallization with holography, enables the fabrication of periodic arrays of polycrystalline silicon (poly-Si) lines with lateral dimensions between 0.5 and 20 μm. The lines consist of grains with well-defined grain boundary locations and lateral dimensions that are appreciably larger than the thickness of the initial a-Si:H film (up to 2 μm for a 300 nm thick film). We investigated the dynamics of the crystallization process by two-dimensional finite element computer simulations of the heat transport and phase transitions during laser crystallization. The theoretical results were compared to: (i) measurements of the crystallization kinetics, determined by recording the transient changes of the reflectance during laser exposure, and to (ii) the structural properties of the crystallized films, determined by scanning force and transmission electron microscopy. The simulations indicate that the crystallization front responsible for the large grains propagates laterally from the edges of the molten silicon lines to their centers with a velocity of ∼14 m/s. A substantial lateral growth only occurs for laser intensities large enough to melt the a-Si film around the center of the lines down to the substrate. Vertical crystallization, which is substantially slower (0.5 m/s), also participates in the solidification process. Using a transfer matrix approach, we converted the time-dependent phase and temperature distributions generated by the simulation program into values for the reflection and transmission of the film as a function of time during and after the laser exposure. A good agreement between the simulated and measured transient reflection was obtained both in the case of homogeneous crystallization as well as that of laser interference crystallization. © 1999 American Institute of Physics.
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  • 331
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4024-4031 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The local structure of erbium-doped silicon produced by the laser ablation technique is investigated by Er LIII-edge x-ray absorption fine structure analysis. The combined analysis of extended x-ray absorption fine structure analysis and an x-ray absorption near-edge structure simulation based on multiple-scattering theory reveals the most probable atomic coordination of the optically active center; Er bonded with six oxygen atoms has a C4v symmetry. The optical activation process of this system is also discussed. The Si target with 10 wt% Er2O3 has two kinds of local structures, C-rare-earth Er2O3 grain and another Er phase incorporated in Si. The laser ablation homogenizes these phases, and deposits a new single-phase structure of the octahedron (Oh point group) on the substrates. In this phase, the optical transition probability is low due to the forbidden 4f transition of Er in the crystal field originating from the higher-order symmetry of O. After annealing, degradation of the symmetry from Oh to C4v results in a crystal field suitable for inducing sufficient radiation transition. © 1999 American Institute of Physics.
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  • 332
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    Journal of Applied Physics 86 (1999), S. 6586-6589 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A model is proposed that is useful for extraction of transport parameters from the random telegraph signal in a multiple quantum well infrared photodetector, at low current bias and low temperature. Data were obtained using a three well, multiperiod device. Electron mobility was found to be from 2×105 to 4×105 cm2/V s. The number of carriers contributed for transport by each well-barrier-well region was found to be less than five. Two distinct activation energies were obtained that corresponded with the two distinct pulse heights in the random telegraph signal. © 1999 American Institute of Physics.
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  • 333
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 86 (1999), S. 6599-6601 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Minority carrier lifetime in ZnTe has been determined from steady-state and time-resolved photoconductivity (PC) measurements. Three types of single crystal p-ZnTe (EG=2.26 eV) grown by the Bridgman technique were studied: (i) as-grown, before and after hydrogen passivation, (ii) Zn annealed, and (iii) In-doped semi-insulating. Steady-state photoconductivity was studied between 80 and 300 K and showed that for as-grown samples, the lifetime went through a sharp maximum of 4.5×10−7 s at 220 K, decreasing to 2.5×10−8 s at 300 K. For hydrogen passivated samples, the low temperature behavior was similar but the lifetime remained high at 4.5×10−7 s at 300 K, due to passivation of deep acceptors OTe. Time-resolved photoconductivity measurements gave a value of 4.6×10−8 s for as-grown ZnTe in reasonably good agreement and 3.2×10−7 s for Zn annealed and 3.1×10−7 s for SI-ZnTe. The radiative recombination constant B was thus found to be 1.4×10−9 and 4×10−10 cm3 s−1, respectively, at 300 K for as-grown and Zn-annealed samples. PC spectral response studies showed a maximum at 2.41 eV at 300 K corresponding to the main valence–conduction band transition as well as a feature near 3.2 eV corresponding to the splitoff band. Slight shift in peak energy to 2.43 eV occurred on H surface passivation due to reduction of surface recombination velocity. © 1999 American Institute of Physics.
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    Journal of Applied Physics 86 (1999), S. 6611-6612 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The electron swarm growth processes in SF6/Ne gas mixtures have been studied by a pulsed Townsend method over the range 8≤E/P≤140 V mm−1 kPa−1, where E is the electric field and P is the gas pressure. The variation patterns as a function of the pressure reduced electric field of the effective ionization coefficient α¯, electron drift velocity, Ve, and longitudinal diffusion coefficient DL in SF6/Ne gas mixtures have been given. The dielectric strength of SF6/Ne gas mixtures has also been determined, which varies linearly with SF6 concentration in the gas mixtures. © 1999 American Institute of Physics.
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    Journal of Applied Physics 86 (1999), S. 5348-5355 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A new wave-vector-space method capable of finding electromagnetic wave propagation in bounded nonlocal media without using boundary conditions is used to find the modes of an optically active planar dielectric waveguide. Optical activity involves first-order wave-vector dispersion (nonlocality). The method finds how the altered nonlocal interaction close to the surfaces affects the waveguide modes. It is found that first-order effects of the surface layer nonlocality enter both the dispersion relation and the field profiles. The waveguide geometry is also used as an impetus to generalize several aspects of the wave-vector-space method. © 1999 American Institute of Physics.
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  • 336
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    Journal of Applied Physics 86 (1999), S. 5376-5384 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Expressions of the thermal equilibrium concentrations of Si in GaAs have been obtained in terms of fundamental constants of the involved materials. Silicon is an amphoteric dopant in GaAs, with four species: a neutral and an ionized shallow donor species occupying Ga sublattice sites, and a neutral and an ionized shallow acceptor species occupying As sublattice sites. The concentration of an ionized Si species is expressed by the concentration of the appropriate neutral species and the GaAs crystal Fermi level or the carrier concentration and the band gap energy level positions. The thermal equilibrium concentrations of the two neutral species are expressed by the relevant Gibbs free energies of formation and the As4 vapor phase pressure in the ambient. Using these equations, the long observed relations between the carrier and Si concentrations in different experiments involving both n- and p-type Si doping produced GaAs are quantitatively explained. A difference of ∼1.55 eV in the effective formation enthalpy between the neutral Si atoms occupying the As and Ga sublattice sites has been identified. Moreover, at high temperatures, the GaAs intrinsic Fermi level energy Ei appears to be higher than the midgap energy Eg/2 by ∼20–80 meV. © 1999 American Institute of Physics.
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    Journal of Applied Physics 86 (1999), S. 5407-5412 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The self-encapsulation kinetics of Ag/Al bilayers were studied both experimentally and theoretically as part of the effort to introduce Ag as an alternative metallization scheme for future ultra-large-scale-integrated technologies. Theoretical modeling was based on an analytical solution of a modified diffusion equation, which incorporated the diffusion of Al atoms through the Ag layers during the Ag/Al bilayer encapsulation progress. The amount of segregated Al atoms was monitored by both Rutherford backscattering spectrometry and film resistivity measurements, and correlated well with the theoretical predictions. These findings showed that the kinetics of the self-encapsulation could be significantly affected by both (i) the chemical affinity between Al and Ag atoms, and (ii) the interfacial energy between the metal layer (Ag) and the newly formed AlxOyNz diffusion barriers. Higher anneal temperatures were shown to accelerate the encapsulation process, and hence, achieved a lower resistivity in the underneath Ag layer. This model, in addition, confirmed the self-passivating characteristics of AlxOyNz diffusion barriers formed by Ag/Al bilayers annealed between 500 and 725 °C. © 1999 American Institute of Physics.
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  • 338
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    Journal of Applied Physics 85 (1999), S. 4460-4462 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The thermal stability of sputtered NiMn pinned spin valves (NiFe/Co/Cu/Co/NiFe/NiMn) was studied for different Co and Cu thicknesses. The coupling between NiFe and antiferromagnetic NiMn was established by an annealing process which also led to a change of magnetoresistance due to diffusion through the Cu layer. Annealing was performed under vacuum in a magnetic field to prevent degradation of the magnetic anisotropy in the antiferromagnet. High angle x-ray diffraction showed a typical shift of the (111) NiMn peak during annealing and a structural change with different Co thicknesses. © 1999 American Institute of Physics.
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  • 339
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    Journal of Applied Physics 85 (1999), S. 4471-4473 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: This work investigates the magnetic and transport properties of Cu–Co thin films with a special reference to their dependence on the film thickness. Such dependencies of the giant magnetoresistance (GMR) effect in silver-based magnetic alloys, such as Ag–Fe, Ag–Co, and Ag–FeNi films, have recently been found, and they were interpreted within the framework of surface spin-flipping scattering. This article reports on similar thickness dependence in the Cu-based alloy, although the spin-orbit interaction in Cu films is much weaker than in Ag films. A reduction of the GMR in the thinnest samples by a factor of 6, compared to the value of as-deposited bulk samples (8.6% in 50 kOe and at 5 K), was accompanied by an increase in resistivity by no more than 50%. A novel vapor-mixing technique of simultaneous sputtering from two sources was used to deposit Cu80Co20 granular thin films of the 20% nominal Co volume fraction. The thickness of the films, ranging from 8 to 400 nm, was measured by the small-angle x-ray reflectivity method. The average size of the Co particles ranging from 2.5 to 3 nm was determined from the superparamagnetic behavior of the Cu–Co granular films. © 1999 American Institute of Physics.
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    Journal of Applied Physics 85 (1999), S. 4480-4481 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The magnetic properties of orthorhombic PrPtAl with TiNiSi-type crystal structure and a nonmagnetic crystalline-electric field (CEF) ground-state singlet were investigated by measurements of specific heat, magnetic susceptibility, magnetization, and electrical resistivity. The results illustrate that in PrPtAl magnetic exchange interactions are strong enough to overcome the singlet–singlet CEF splitting of 21 K and to induce long-range magnetic order at TC=5.8 K. © 1999 American Institute of Physics.
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    Journal of Applied Physics 85 (1999), S. 4497-4499 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A full identification method is outlined for the ten parameters of a bimodal model for highly magnetostrictive material. In the model, magnetization and strain hysteresis loops are modeled as the superposition of twin hysteresis loops, shifted in critical field activation value by equal amounts in opposite directions. Identification of the parameters for Terfenol-D and Terzinol-D show that the model predicts the behavior of the Terfenol-D better than that of the Terzinol-D, where more low field reversible behavior is evident. © 1999 American Institute of Physics.
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    Journal of Applied Physics 85 (1999), S. 4515-4517 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: In this article we study the magnetic behavior of a series of copper-deficient spin-glass compounds La1.85Sr0.15Cu1−εO4−δ. High-quality ceramic samples were prepared by a sol–gel technique. Stoichiometry and structural characterization of the specimens were verified by x-ray diffraction, inductively coupled plasma spectrometry, atomic absorption spectrophotometry, and thermogravimetric analysis. Low-field ac and dc magnetic measurements, carried out in a superconducting quantum interference device magnetometer for samples with ε=0.05, 0.15, and 0.25, revealed all major characteristics of a spin-glass system: thermal irreversibility, magnetic remanence, time-relaxation and frequency-dependent ac susceptibility. © 1999 American Institute of Physics.
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    Journal of Applied Physics 85 (1999), S. 4524-4526 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We present the results of an inelastic neutron scattering experiment with polarization analysis performed on a single crystal of UO2. A magnetic inelastic response is observed above TN in the energy region between 3 and 10 meV, at least up to 6.5TN. This result provides evidence of the fact that in the time scale of our experiment the uranium triplet ground state is split into three singlets because of a dynamical Jahn–Teller distortion of the oxygen cage, reducing the point symmetry at the uranium site. The position of the peaks and their dispersion are compatible with monoclinic 1-k distortions along the three directions of the 〈100〉 star. This suggests a picture in which as TN is approached, a correlation builds up between the phases of the corresponding vibrations until, eventually, a static 3-k distortion is obtained below TN. © 1999 American Institute of Physics.
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  • 344
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    Journal of Applied Physics 85 (1999), S. 4325-4330 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: High temperature, solution phase reduction of cobalt chloride in the presence of stabilizing agents was employed to produce magnetic colloids (ferrofluids) of cobalt nanocrystals. We systematically synthesized and isolated nearly monodisperse nanocrystal samples ranging in size from 2 to 11 nm while maintaining better than a 7% std. dev. in diameter. As synthesized cobalt particles are each a single crystal with a complex cubic structure related to the beta phase of elemental manganese (ε-Co). Annealing the nanocrystals at 300 °C converts them quantitatively to the more common hexagonal-close-packed crystal form. Deposition of these uniform cobalt particles on solid substrates by evaporation of the carrier solvent results in the spontaneous assembly of two-dimensional and three-dimensional magnetic superlattices (colloidal crystals). A combination of x-ray powder diffraction, transmission electron microscopy, and superconducting quantum interference device magnetometry were used to characterize both the dispersed nanocrystals and the assembled superlattices. © 1999 American Institute of Physics.
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    Journal of Applied Physics 85 (1999), S. 4343-4345 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Room-temperature hysteresis loops of granular Cu100−xCox alloys (5≤x≤15) obtained by planar flow casting in air and submitted to proper annealing treatments have been measured up to a field of 10 kOe by means of a vibrating sample magnetometer. In major loops (|Hvert|=10 kOe), the reduced remanence-to-saturation ratio mr=Mr/Ms and the coercivity Hc measured on all studied materials appear to be related by an almost linear law of the type mr(approximate)1/3 (μHc/kT), μ being the average magnetic moment on Co particles. A similar relation is also observed on minor symmetrical loops (100 Oe≤|Hvert|≤9 kOe). The observed results are accounted for by a model which considers the hysteresis as originating by magnetic interactions among nearly superparamagnetic Co particles. © 1999 American Institute of Physics.
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    Journal of Applied Physics 85 (1999), S. 4340-4342 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We have applied a Monte–Carlo model of the properties of an interacting fine particle system to calculations of the field-cooled (FC) and zero-field cooled (ZFC) magnetization. The variation of Tg, the temperature peak, in the ZFC is also calculated. For an interacting system the effective energy barrier distribution is dependent on the packing density, and this is reflected in the Tg vs H curve. An important result is the demonstration that magnetostatic interactions between the particles can give rise to a peak in the FC magnetization. This is in agreement with experiments and is a result of the magnetic order introduced by the magnetostatic interactions. © 1999 American Institute of Physics.
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    Journal of Applied Physics 85 (1999), S. 4364-4366 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Mechanisms for the switching of the magnetization in ultrathin small structure are summarized. The temperature dependence of the switching field for different sizes and anisotropies is studied and found to be significant. Much of the current interpretations of finite temperature experimental results on giant magnetoresistance and tunnel structures in terms of zero temperature micromagnetics calculations have not considered this problem. © 1999 American Institute of Physics.
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    Journal of Applied Physics 85 (1999), S. 4373-4375 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: This article describes the advances in unification of model descriptions of hysteresis in magnetic materials and demonstrates the equivalence of two widely accepted models, the Preisach (PM) and Jiles–Atherton (JA) models. Recently it was shown that starting from general energy relations, the JA equation for a loop branch can be derived from PM. The unified approach is here applied to the interpretation of magnetization measured in nonoriented Si–Fe steels with variable grain size 〈s〉, and also in as-cast and annealed Fe amorphous alloys. In the case of NO Fe–Si, the modeling parameter k defined by the volume density of pinning centers is such that k(approximate)A+B/〈s〉, where the parameters A and B are related to magnetocrystalline anisotropy and grain texture. The value of k in the amorphous alloys can be used to estimate the microstructural correlation length playing the role of effective grain size in these materials. © 1999 American Institute of Physics.
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    Journal of Applied Physics 85 (1999), S. 4385-4387 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The moment and remanence of a thermally demagnetized sample of sintered, aligned Nd2Fe14B have been measured along the initial magnetizing curve and along the descending branch of the major loop, over an applied field range −12 kOe≤ha≤+12 kOe, and over a wide range of temperatures 25 °C≤T≤220 °C. Changes in temperature have only a weak influence on the magnetizing process, but have a profound effect on the demagnetizing branch and on the curvature of the Henkel plots, which varies from strongly magnetizing-like at room temperature to strongly demagnetizing-like above 140 °C. We present numerical calculations based on a modified version of the scalar Preisach model, which assumes that moment reversal along the demagnetizing branch is characterized by two distinct sets of energy barriers which must be activated sequentially, so that the availability of one set is conditional upon the activation of the other. The model is able to replicate all of the experimental systematics, and shows that long range, mean field interactions, positive or negative, are absent from this system. © 1999 American Institute of Physics.
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    Journal of Applied Physics 85 (1999), S. 4403-4405 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Soft magnetic composite materials produced by powder metallurgy techniques can be very useful for construction of low cost small motors. However, the rotational core losses and the corresponding B–H relationships of soft magnetic composite materials with two-dimensional rotating fluxes have neither been supplied by the manufacturers nor reported in the literature. This article reports the core loss measurement of a soft magnetic composite material, SOMALOY™ 500, Höganäs AB, Sweden, under two-dimensional excitations. The principle of measurement, testing system, and power loss calculation are presented. The results are analyzed and discussed. © 1999 American Institute of Physics.
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    Journal of Applied Physics 85 (1999), S. 4412-4414 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Hysteresis, power losses, and the Barkhausen effect are investigated in an Fe-based highly magnetostrictive amorphous material, as a function of applied stress. By means of the static and dynamic Preisach model, and of existing theories of the Barkhausen effect, the results are shown to be compatible with the existence of a characteristic structural length δc, playing a role similar to that of grain size in crystalline materials. At low applied stresses, where the magnetization process is dominated by quenched-in stresses σi, δc is identified with the typical wavelength of σi fluctuations. The theoretical analysis leads to the estimate δc∼70–100 μm and 〈σi〉∼3.5 MPa. © 1999 American Institute of Physics.
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    Journal of Applied Physics 85 (1999), S. 4436-4438 
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    Source: AIP Digital Archive
    Topics: Physics
    Notes: [Co(20 Å)/Re(6 Å)]20 superlattices were grown on a (112¯0) surface of a Al2O3 single crystal, with the [0001] direction of their hcp structure in the plane of the film. The Co layers were found to be antiferromagnetically coupled (AF), with a saturating field of 6 kOe. Polarized neutron reflectivity was used to determine the direction of the sublattice magnetization. In zero applied field, the AF moments are aligned along the Co[0001] axis. In a magnetic field H perpendicular to the Co[0001] axis, the sublattices moments evolve to a canted arrangement, with the AF component always perpendicular to the field. With H along the Co[0001] axis, the AF moments flop in a direction perpendicular to Co[0001] axis. The spin flop transition is not abrupt, but can be described as a gradual rotation that is completed at 2 kOe. The anisotropy of the sublattice magnetization is related to the anisotropy of the magnetoresistance. This has the conventional dumbbell behavior with the field applied perpendicular to the Co[0001] axis, but exhibits an extended plateau near H=0, and a slight increase up to H∼2 kOe, when H is parallel to Co[0001] axis. © 1999 American Institute of Physics.
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  • 353
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 86 (1999), S. 5817-5828 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The retarded solution to the inhomogeneous wave equation in electrodynamics is studied with a purpose to understand Wu's missile and subsequently the radial dependence of energy transmitted by transient sources. The finite rate of change of the source current is shown to imply the inverse-square law at a sufficiently large distance, the region of which is determined by the minimum scale time tm of the current and may be called the (generalized) Fraunhofer region. With a uniform disk source, the electric field on the symmetry axis for a wide range is shown equal to the difference of the current at two times. Hence, examples with analytic results are given to demonstrate clearly how the pulse energy decreases with distance at a much slower rate in the (generalized) Fresnel region and how the inverse-square dependence is recovered in the farther region. Moreover, Wu's current profile, though with infinite slopes, is a Lighthill's generalized function and missiles refer to the transmitted pulses in the limit of zero tm which gives an infinite Fresnel region. A square temporal profile and other profiles with a sudden rise (or fall), including Samaddar's single-cycled cosine, which also generate missiles with an inverse-linear dependence, are studied. © 1999 American Institute of Physics.
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  • 354
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 86 (1999), S. 5850-5857 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: In this article, we discuss parameters influencing (a) the properties of thin AlxGa1−xN layers grown by metalorganic chemical vapor deposition and (b) the electrical properties of the two-dimensional electron gas (2DEG) forming at the AlxGa1−xN/GaN heterojunction. For xAl〉0.3, the AlxGa1−xN layers showed a strong tendency towards defect formation and transition into an island growth mode. Atomically smooth, coherently strained AlxGa1−xN layers were obtained under conditions that ensured a high surface mobility of adsorbed metal species during growth. The electron mobility of the 2DEG formed at the AlxGa1−xN/GaN interface strongly decreased with increasing aluminum mole fraction in the AlxGa1−xN layer and increasing interface roughness, as evaluated by atomic force microscopy of the surfaces prior to AlxGa1−xN deposition. In the case of modulation doped structures (GaN/AlxGa1−xN/AlxGa1−xN:Si/AlxGa1−xN), the electron mobility decreased with decreasing thickness of the undoped spacer layer and increasing silicon doping. The electron mobility was only moderately affected by the dislocation density in the films and independent of the growth temperature of the AlxGa1−xN layers at xAl=0.3. For Al0.3Ga0.7N/GaN heterojunctions, electron mobility values up to 1650 and 4400 cm2/V s were measured at 300 and 15 K, respectively. © 1999 American Institute of Physics.
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  • 355
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 86 (1999), S. 5879-5887 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Micron- and submicron-size changes induced by local laser heating in thin films of Ge2Sb2Te5 are studied by atomic force microscopy (AFM). This material is presently used for rewritable data storage that employs phase change recording. Reversible switching between the amorphous and crystalline states, which is accompanied by a considerable change in optical properties and film density, is exploited to store bits of information. The density change can be detected by AFM, which we use here to study the amorphization (writing) and recrystallization (erasure) of single bits. Both processes have been measured as a function of modification pulse power and duration. Morphology changes can be detected even if the phase change film is covered by a thin protective layer. AFM allows a precise determination of the bit size and bit depth, which characterizes the progress of the phase change in the direction of the surface normal. The present setup allows the correlation of the change in optical reflectance ΔR caused by a specific laser pulse to the bit topography. This enables a detailed study of the mechanisms of bit writing and erasure. © 1999 American Institute of Physics.
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  • 356
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 86 (1999), S. 5906-5908 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A closed hydrodynamic approach for a full nonparabolic band model is developed from the maximum entropy principle. Generalized kinetic fields are introduced within a total average-energy scheme. Numerical calculations for bulk and submicron Si structures are found to compare well with those obtained by ensemble Monte Carlo simulators thus validating the proposed approach. © 1999 American Institute of Physics.
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  • 357
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 86 (1999), S. 100-106 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The distance between sample and probe in a scanning near-field optical microscope is regulated via tracing the shear-force on the tip which is glued to a tuning fork piezo. A lock-in technique is used. We demonstrate that the bandwidth of the control loop is increased if not only amplitude or phase, but a favorable combination of both is used as feedback signal. The enhancement of bandwidth is connected with a reduction of signal-to-noise ratio. The optimum combination of both, bandwidth and signal-to-noise ratio, can be adjusted purely electronically to the specific needs of an experiment. A theoretical model is developed that discloses the relation between the mechanical and electrical properties of the combination of tuning fork and fiber tip. The frequency response of the shear-force detection system is calculated with a numerical simulation based on this model. Experimental frequency response curves are well fitted by these simulations. Our results are especially important for low-temperature scanning microscopy, where the bandwidth enhancement is essential for obtaining a reasonable scanning speed. © 1999 American Institute of Physics.
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  • 358
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 86 (1999), S. 124-133 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: In a coplanar plasma display panel the discharges in each pixel are sustained between two parallel electrodes on the same substrate. A third electrode perpendicular to the sustaining electrodes and placed on a facing substrate is used to address the pixel. A self-consistent two-dimensional model of the microdischarge has been used to simulate and study the addressing and sustaining phases in an alternating current coplanar cell. The formation and decay of the transient plasma during the address and sustain discharge pulses are described. The time evolution of the charges on the dielectric surfaces above each electrode is also discussed and the model is used to derive the voltage margins of the address and sustain regimes. © 1999 American Institute of Physics.
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  • 359
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4477-4479 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A series of Fe/Si sandwiches have been prepared by ion beam sputtering at room temperature onto glass substrate with the following nomenclature: Glass/Si20 nm/Fe5/6 nm/Fe5 nm/Ru2 nm. Magnetization measurements have been performed at 300 K and show no evidence of antiferromagnetic exchange coupling. However, the magnetoresistance curves recorded at 300 K are very interesting and show an inverse magnetoresistance for sandwiches with Si spacer layer thicknesses between 1.2 and 1.5 nm. The resistance is smaller at zero field than at saturation. This inverse magnetoresistance is due to the superparamagnetic interfaces and finds its origin in the difference of the electronic nature of the Fe/Si interfaces and Fe/Ru interfaces. Fe1−xSix iron silicide at Fe/Si interfaces has a scattering spin asymmetry ratio (α=ρ↓/ρ↑) larger than one, whereas, Fe with Ru impurities at the Fe/Ru interfaces presents a scattering spin asymmetry ratio smaller than one. © 1999 American Institute of Physics.
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  • 360
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4539-4541 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The iron(III) S=5/2 dimer [Fe(OMe)(dbm)2]2 (in short Fe2) has a nonmagnetic S=0 ground state. The separation between the singlet ground state and the first excited (triplet) state is determined from susceptibility measurements to be about 22 K; for a dimer this value is equal to the antiferromagnetic exchange constant J. Proton nuclear magnetic resonance measurements were performed on Fe2. The nuclear spin-lattice relaxation rate (NSLR) was studied as a function of temperature at 31 and 67 MHz and as a function of the resonance frequency (10–67 MHz) at T=295 K. At room temperature the 1H NSLR is independent of frequency contrary to the strong dependence found in planar ring compounds like Fe6 and ferric wheel (Fe10). The temperature dependence of the proton NSLR shows an exponential decrease on lowering the temperature from which we estimate a gap value about double the value obtained from the uniform susceptibility, a result which is unexpected if the NSLR were simply proportional to the concentration of dimers in the triplet excited state. © 1999 American Institute of Physics.
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  • 361
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    Journal of Applied Physics 85 (1999), S. 4556-4558 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The ferromagnetic resonance spectra of thin alloy films, which are often used as components of giant magnetoresistance structures, were observed. Face-centered-cubic films with Cu underlayers and single magnetic layers of permalloy, permalloy containing Co; or Co rich CoFe alloys were deposited by magnetron sputtering. The magnetic field position of the resonance provides information about the magnetic moment and the growth induced anisotropies of the films, and was affected by magnetostriction when stresses were induced. Linewidths and coercivity increased rapidly as a function of the total (Cu+magnet) layer thickness above about 20 nm. The linewidth is sensitive to the damping parameter for the thinner films and to magnetocrystalline anisotropy and crystallographic texture for the thicker Co containing films in which the grains become large. Based on observations of the resonances in stressed films, several nonmagnetostrictive compositions were determined. © 1999 American Institute of Physics.
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  • 362
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    Journal of Applied Physics 85 (1999), S. 4571-4573 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The effect of oxygen and heat treatment on magnetic properties and corrosion resistance of Fe–N thin films sputter-deposited under various N2+O2 partial pressure were investigated. All the as sputtered films have a single phase of α-Fe only, except where a high N2+O2 partial pressure was used. After annealing at 200–500 °C, the structure and magnetic properties of Fe–N–O films were changed. Under suitable conditions the magnetic properties of Fe–N–O films were found to have Hc of 0.5 Oe and 4πMs around 20 kG. It is also demonstrated that the oxygen has improved the corrosion resistance and thermal stability of Fe–N thin film. © 1999 American Institute of Physics.
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  • 363
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    Journal of Applied Physics 85 (1999), S. 4583-4585 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We recently developed the method of generalized magneto-optical ellipsometry (GME), which enabled us to achieve a complete magneto-optical characterization of a magnetic material, including the magnetization orientation. For the present study, we have modified our original setup to allow for measurements at arbitrary external fields including entire field scans. Consequently, GME can be used as a tool to perform vector magnetometry measurements. In this article, we present our first experimental results on polycrystalline Co films which demonstrate the feasibility of GME as a magneto-optical vector magnetometer. © 1999 American Institute of Physics.
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  • 364
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4592-4594 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: In this study, magnetization reversal of a Co–Cr very thin film with rectangular area of 1.0×1.0 cm2 was observed by means of the anomalous Hall effect. The amplitude of the Hall voltage VH took the maximum and minimum values when magnetic field was applied perpendicular and parallel to the film plane, respectively. The hysteresis loop observed in perpendicular direction exhibited the largest lean for the film deposited at substrate temperature Ts of 100 °C. It was found that for the film with a large perpendicular magnetic anisotropy constant, VH is independent to the angle of applied field. The Hall loop of the Co–Cr film 150 Å thick revealed its shape more similar to a Kerr loop than a vibrating sample magnetometer loop. The VH–H measurement is useful to evaluate the magnetization process of very thin films without the perturbation of the magnetization component from the substrates and the specimen folder in the measurement system especially for the case of obliquely applied magnetic field condition. © 1999 American Institute of Physics.
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  • 365
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4759-4761 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Magnetization, electrical resistivity, and thermal expansion measurements have been performed on polycrystalline RTSb3 (R=La, Ce, Pr, Nd, Gd, Tb, and Dy; T=Cr, V) samples in order to study their magnetic properties. Depending on the rare-earth element, RTSb3 has been found to have either a purely ferromagnetic (or antiferromagnetic) phase or combination of antiferromagnetic (lower-temperature) and ferromagnetic (higher-temperature) phases. The antiferromagnetic order evolves from the ferromagnetic order as a result of the competition between R3+ and Cr3+ ions. As R is changed from La to Dy, the antiferromagnetic ordering of the R3+ ions becomes more prominent and predominate over the ferromagnetic ordering of Cr3+ for R=Gd, Tb, and Dy. Thermal expansion measurements show that the antiferromagnetic transition accompanies a drop in the sample dimension. The order of the ferromagnetic transition is found to be of the second order. © 1999 American Institute of Physics.
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  • 366
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    Journal of Applied Physics 85 (1999), S. 4562-4564 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: FeTaN films with moderate Bs of 14 kG and high resistivity of 100–150 μΩ cm have been investigated. Even with a low Ta incorporation of only 3 at. %, films with the above characteristics were obtained by using rf diode and dc magnetron sputtering. When the soft magnetic properties were optimized, only a body-centered-cubic α-Fe phase was found, and it had a significantly expanded crystal lattice. The films exhibited a nearly amorphous grain structure. It was found that low atomic mobility of the sputtered atoms was needed in order to promote formation of this phase. © 1999 American Institute of Physics.
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  • 367
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    Journal of Applied Physics 85 (1999), S. 4574-4576 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We have investigated the magnetic properties of (Co1−xFex)–Al–O granular thin films prepared by a reactive sputtering method in an atmosphere of O2+Ar. The coercivity and electrical resistivity of the films are almost independent of x, but with increasing x the anisotropy field decreases linearly and the saturation induction has a broad maximum of 20 kG around x=0.7. The granular films show the same general tendency as bulk Co–Fe alloys in the compositional dependence of magnetostriction (λ). The magnitude of λ varies with increasing annealing temperature. Using a film with x=0.08 as the core of a spiral-wound inductor gave a quality factor Q=25 at a frequency of 300 MHz. © 1999 American Institute of Physics.
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  • 368
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    Journal of Applied Physics 85 (1999), S. 4586-4588 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: This article examines the characterization of buried magnetic interfaces using a relatively new technique, the second-harmonic magneto-optic Kerr effect (SHMOKE), and a more established technique, x-ray reflectivity (XRR). Results are presented on the interdiffusion and interfacial roughness of Ta/NiFe and TaN/NiFe interfaces. The samples were characterized as deposited and after a 270 °C, 2 h anneal. SHMOKE analysis indicates that the Ta/NiFe interfaces are more susceptible to interdiffusion than the TaN/NiFe interfaces, during deposition as well as anneal. These results are consistent with XRR analysis of the samples and suggest that further development of SHMOKE may be of enormous benefit to interfacial magnetic metrology. © 1999 American Institute of Physics.
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  • 369
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    Journal of Applied Physics 85 (1999), S. 4598-4600 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The magnetization reversal process in an array micron sized NiFe patterns was studied using magnetic force microscopy in the presence of external fields. The behavior of the magnetization distribution was correlated with the aspect ratio and the direction of the applied fields. Magnetizing along the hard axis was found to produce solenoidal magnetization at remanence while applying the field along the easy axis tend to form nonsolenoidal configurations. The micromagnetic evolution, which involved domain wall, crosstie, and vortex displacements, was studied and the correlations were consistent with previously reported M–H loop observations and theoretical predictions. © 1999 American Institute of Physics.
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  • 370
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    Journal of Applied Physics 85 (1999), S. 4619-4621 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We present expressions for the resonant magnetic x-ray scattering from rough surfaces; using our formulas we analyze the structural and magnetic roughnesses, as well as the correlation between them. We demonstrate that the leading contribution to the difference in the diffuse scattering between left- and right-circularly polarized light for a rough surface with in-plane magnetization vanishes unless the structural and magnetic roughnesses are correlated. The effects of magnetic domain structure and magnetic dead layers on the surface scattering are also discussed. © 1999 American Institute of Physics.
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  • 371
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    Topics: Physics
    Notes: GaAs at the ZnSe/GaAs and GaAs/GaAs interfaces of ZnSe/GaAs/GaAs heterostructures is studied by phase selective photoreflectance (PR) spectroscopy. Four samples with ZnSe layers of various thickness were examined. We unambiguously determined the origin of two different features observed in the PR spectra by combining in phase and out of phase measurements, with PR measurements employing excitation lasers with different wavelengths. These two features are found to originate at different regions of the heterostructure. One contributing transition is a bulk-like signal, resembling that of bare GaAs, which originates in a region that encompasses the buffer layer/substrate GaAs homointerface. A second contributing signal is attributed to a strained region adjacent to the ZnSe/GaAs heterointerface. Both this second signal and the bulk-like signal show Franz–Keldysh oscillations that allow us to determine the electric field strength at the ZnSe/GaAs and GaAs/GaAs interfaces. It is found that the electric field strength at the heterointerface is larger than that of the homointerface. Reflectance difference measurements further support the existence of two spatially separated GaAs regions, which produce two independent overlapping optical modulated signals in the ZnSe/GaAs/GaAs heterostructures. © 1999 American Institute of Physics.
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  • 372
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    Journal of Applied Physics 86 (1999), S. 459-463 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Interface roughness scattering-limited electron mobility is calculated for AlAs/GaAs and Ga0.5In0.5P/GaAs wells taking into account the effects of finite barrier potential, extension of the wave function into the barrier layer, energy band nonparabolicity, and screening of the scattering potential. The mobility in AlAs/GaAs wells varies with the well width L as Ln(n=4.7–4.8), but the variation cannot be fitted to a similar relation for Ga0.5In0.5P/GaAs wells. Experimental results for both the systems may be explained with an asperity height between 2.83 and 5.67 Å, and a correlation length smaller than 170 Å. It is concluded that the larger experimental mobility in Ga0.5In0.5P/GaAs wells is due to the smaller barrier potential in this system. © 1999 American Institute of Physics.
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  • 373
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    Journal of Applied Physics 86 (1999), S. 476-479 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We have made thickness dependent in situ resistivity measurements on sputtered metal films in real time during film deposition. These measurements allow the separation of the bulk and finite-size contributions to the resistance. The metals studied were Co, Cu, Ni80Fe20, and Ta, deposited in differing orders to isolate the scattering at interfaces relevant to common spin-valve structures. We see sources of excess diffuse scattering in bilayers of Ta with the 3d metals, regardless of the deposition order. We see a similar effect for Co on Cu, but not for Cu on Co. In some cases, we see significant changes in film resistance from overlayers as thin as 2 Å. These results show that the two Cu interfaces in a spin valve are not equivalent, and that other interfaces in the structure may be important. We discuss the origin of the diffuse scattering in terms of interdiffusion or a roughening transition during the initial deposition and island coalescence. © 1999 American Institute of Physics.
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  • 374
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    Journal of Applied Physics 86 (1999), S. 524-531 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The thin field-effect transistor based on amorphous semiconductors, both inorganic or organic, is modeled using an iterative scheme. The results of modeling gave insight into the temperature dependencies of this device. Further, we present the differential procedure, based on the first and higher derivatives of the data, to derive from the field-effect characteristics the basic parameters of the active semiconductor film, i.e., the density of states and field-effect mobility. © 1999 American Institute of Physics.
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  • 375
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    Journal of Applied Physics 85 (1999), S. 4871-4873 
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    Source: AIP Digital Archive
    Topics: Physics
    Notes: The liquid coating (LC) has been employed to apply epoxy and lubricant over the surface of rapidly solidified Nd–Fe–B powder particles. The LC led to an improvement of physical and magnetic properties for the powders and magnets compared to the dry blending and the encapsulation methods. The LC powders have excellent flowability and can be used for bonded magnets requiring very close tolerances; further bonded magnets made using this powder posses higher strength.© 1999 American Institute of Physics.
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  • 376
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    Journal of Applied Physics 85 (1999), S. 4738-4740 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The ferromagnetic to antiferromagnetic transition in Fe3Ga4 is studied by means of ac-susceptibility measurements under chemical and external hydrostatic pressure. Substitution of Al for Ga results in an increase of the ferromagnetic to antiferromagnetic transition temperature (T0) of 4.1(4) K/at. % Al. Application of hydrostatic pressures up to 7 kbar also yields a positive effect: dT0/dp=3.4(4) K/kbar. The external-pressure-induced increase of T0 in Fe3(Ga0.9Al0.1)4 is considerably weaker: dT0/dp=0.93(10) K/kbar. Thermal-expansion measurements reveal that the volume change at the ferromagnetic to antiferromagnetic transition ΔV/V amounts to only 0.02%. We believe that the volume effect in conjunction with a shift in the Fermi level drives the ferromagnetic to antiferromagnetic transition. The details of the band structure at the Fermi surface determine the magnetic properties and may give rise to the strong pressure dependence of T0. © 1999 American Institute of Physics.
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  • 377
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    Journal of Applied Physics 85 (1999), S. 4750-4752 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The ferromagnetic compound Nd3Co has Curie temperature TC=25 K and the spin reoriented temperatures TR1=8.5 K and TR2=14 K. Neutron powder-diffraction measurements of Nd3Co were carried out at 50 K above TC and at 2.1 K below TR1. The magnetic structure at 2.1 K was determined, whose unit cell has the volume of 2a×b×2c. The values of magnetic moment on Nd atoms in 4c and 8d sites were 2.47 and 3.08 μB, respectively. This magnetic model is consistent with the results of magnetization curves of a single crystalline Nd3Co. © 1999 American Institute of Physics.
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  • 378
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    Journal of Applied Physics 85 (1999), S. 4762-4764 
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    Source: AIP Digital Archive
    Topics: Physics
    Notes: Hexagonal manganites RMnO3 (R=Sc, Y, Ho, Er, Tm, Yb) are compounds in which a ferroelectric and an antiferromagnetic order may coexist. The ferroelectric crystal structure is well known but theoretical studies show that there are different possibilities for the spin structure. By means of polarization- and temperature-dependent second-harmonic spectroscopy it is possible to determine the magnetic structure of RMnO3 compounds. © 1999 American Institute of Physics.
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    Journal of Applied Physics 85 (1999), S. 4773-4775 
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    Source: AIP Digital Archive
    Topics: Physics
    Notes: A microwave test structure has been designed to measure the high-speed response of giant magnetoresistive (GMR) devices. The test structure uses microwave transmission lines for both writing and sensing the devices. Pseudo-spin-valve devices, with line widths between 0.4 and 0.8 μm, were successfully switched with pulses whose full width at half-maximum was 0.5 ns. For small pulse widths τpw the switching fields are observed to increase linearly with 1/τpw. The increase in switching fields at short pulse widths is characterized by a slope which, for the current devices, varies between 4 and 16 μA s/m (50–200 Oe ns). The magnetoresistive response during rotation and switching was observed. For small rotations (∼45° between layer magnetizations) the GMR response pulses had widths of 0.46 ns, which is at the bandwidth limit of our electronics. For larger rotations (∼90°) the response pulses broadened considerably as the magnetic layers were rotated near the unstable equilibrium point perpendicular to the device axis. Full 180° switches of both soft and hard layers were observed with switching times of approximately 0.5 ns. © 1999 American Institute of Physics.
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  • 380
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4785-4787 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Many things will have to go right for quantum computation to become a reality in the lab. For any of the presently proposed approaches involving spin states in solids, an essential requirement is that these spins should be measured at the single-Bohr-magneton level. Fortunately, quantum computing provides a suggestion for a new approach to this seemingly almost impossible task: convert the magnetization into a charge, and measure the charge. I show how this might be done by exploiting the spin-filter effect provided by ferromagnetic tunnel barriers, used in conjunction with one-electron quantum dots. © 1999 American Institute of Physics.
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  • 381
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4788-4790 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A typical magnetic random access memory stack consists of NiFe/Cu/NiFeCo multilayers, sandwiched by contact and antioxidation layers. For patterning of submicron features without redeposition on the sidewalls, it is desirable to develop plasma etch processes with a significant chlorinated etch component in addition to simple physical sputtering. Under conventional reactive ion etch conditions with Cl2-based plasmas, the magnetic layers do not etch because of the relatively involatile nature of the chlorinated reaction products. However, in high ion density plasmas, such as inductively coupled plasma, etch rates for NiFe and NiFeCo up to ∼700 Å min−1 are achievable. The main disadvantage of the process is residual chlorine on the feature sidewalls, which can lead to corrosion. We have explored several options for avoiding this problem, including use of in situ and ex situ cleaning processes after the Cl2-etching, or by use of a noncorrosive plasma chemistry, namely CO/NH3. In the former case, removal of the chlorine residues with in situ H2 plasma cleaning (to form volatile HCl that is pumped away), followed by ex situ solvent rinsing, appears effective in preventing corrosion. In the latter case, the CO/NH3 plasma chemistry produces metal carbonyl etch products, that are desorbed in the simultaneous presence of an ion flux. The etch rates with CO/NH3 are much lower than with Cl2 over a broad range of source powers (0–1500 W), radio frequency chuck powers (50–450 W), pressures (1–30 mTorr) and plasma compositions. We have tried substitution of CO2 for CO, and addition of Ar to produce faster etch rates, without success. Maximum rates of ∼300 Å min−1 for NiFe and NiFeCo were obtained with CO/NH3 under optimum conditions. The etched sidewalls tend to be sloped because of mask erosion during plasma exposure, in contrast to the case of Cl2-based chemistries where the sidewalls are vertical. © 1999 American Institute of Physics.
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  • 382
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4803-4805 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The resistivity tensors of La0.67Ca0.33MnO3 films were investigated at temperatures from the Curie temperature up to 600 K in magnetic fields up to 20 T. The diagonal transport is described by hopping of a small spin polaron cluster of 4 ions to nearest-neighbor spins. A spin-dependent activation energy and a mean field approximation for the magnetization of clustered polaron spins and unclustered Mn ion spins allowed the description of ρ(B,T) with a minimum of free parameters. The electron-like low field Hall coefficient showed a thermally activated behavior with an activation energy higher than that extracted from diagonal data. © 1999 American Institute of Physics.
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  • 383
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4815-4817 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: High-resolution electron microscopy, Lorentz microscopy, and off-axis electron holography have been used to characterize magnetic tunnel junctions. Observations in cross section show that the tunnel barriers are slightly narrower and smoother after annealing at temperatures up to 350 °C. The demagnetization of a magnetically hard CoPtCr reference layer through repeated magnetization reversal of a soft layer of either Co or Ni40Fe60 is likely to originate from magnetic fringing fields at Néel walls, which form in the soft layers close to the coercive field. © 1999 American Institute of Physics.
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  • 384
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4827-4829 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Using a multiple-scattering approach and the local-density and rigid-spin approximations, the exchange interactions are calculated for Fe, Ni, and Co, and the spin-wave spectrum obtained. The interactions contributing to the spin-wave spectrum are found to be rather long-ranged. The exchange parameters are calculated as a function of band filling, and predict transition to antiferromagnetic behavior for electron-deficient alloys of bcc Fe and fcc Co. © 1999 American Institute of Physics.
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  • 385
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4839-4841 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The occurrence of magnetic phases in FeCr and FeCo in the CsCl structure has been studied by first-principles total-energy calculations with a sensitive and accurate method, using a four-atom unit cell. When both atoms in such binary compounds can be strongly magnetic, unusual structures are found. These materials have ferromagnetic (FM) and antiferromagnetic (AF) phases, but the equilibrium state for both is FM. However at 3% expansion of the lattice constant the ground state of FeCr becomes AF, whereas in FeCo the AF phase is never the ground state. The AF phase in both FeCr and FeCo has an unusual structure in that both the Fe and the Cr or Co sublattices are separately AF. In both the FM and AF phases at the equilibrium volume, the Fe moment is reduced in FeCr, but enhanced in FeCo from that in pure body-centered-cubic (bcc) Fe; also the Cr moment is increased from that in pure bcc Cr, while the Co moment is similar to the moment in hexagonal-dose-packed Co. In the FM phase of FeCr, but not in FeCo, the two Fe atoms in the four-atom unit cell have different moments, which have opposite signs at large volume. © 1999 American Institute of Physics.
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  • 386
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4850-4852 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Single crystals of YVO3 were grown using the floating-zone technique. YVO3 crystallizes in the orthorhombic Pbnm structure, and the structural parameters were determined by means of neutron diffraction. Using a superconducting quantum interference device magnetometer, we have studied the magnetic properties of YVO3 along the three principal directions. Our single crystal exhibits two magnetic transitions at about 115 and 75 K. For temperatures above the magnetic ordering, almost isotropic Curie–Weiss behavior is found for the magnetic susceptibility. Below the ordering, however, we find a highly anisotropic response with the c axis as the easy-magnetization direction. Both magnetic phases exhibit a weak ferromagnetic component along the c axis. A complex low-field magnetization behavior indicates that YVO3 orders ferrimagnetically for temperatures between 75 and 115 K. © 1999 American Institute of Physics.
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  • 387
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    Source: AIP Digital Archive
    Topics: Physics
    Notes: CoSiB and FeB single layers and CoSiB/FeB bilayers with thicknesses ranging from 250 to 1500 Å were grown on bowed glass substrates using rf sputtering. A magnetoelastic anisotropy was induced in the magnetic layers after removing the films from the sputtering chamber. The positive (FeB) and the negative (CoSiB) magnetostrictive single layers showed an easy magnetization axis transverse and parallel to the compression axis, respectively. The magnetic behavior of the CoSiB/FeB bilayers is shown to be extremely sensitive to the thickness of each layer, to their thickness ratios, and also to the deposition sequence of the layers on the substrate. These results are discussed in terms of the interactions between two magnetic phases with easy magnetization axes transverse to each other. © 1999 American Institute of Physics.
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  • 388
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4821-4823 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We have developed a new approach for the calculation of electronic structure and magnetic properties in the framework of spin density functional theory for arbitrary magnetic systems. This approach is based on the wavelets technique. We present test calculations and compare with previously published results. As an application of the general formalism to the noncollinear case we consider the two limiting cases of itinerant and localized magnetic moments. The development of this method is a first step to perform ab initio spin dynamics for finite atomic systems. © 1999 American Institute of Physics.
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  • 389
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4842-4844 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We use first principles electronic structure techniques to study the magnetic structure of γ-FeMn using the Korringa–Kohn–Rostocker multiple-scattering approach in conjunction with an extension of the single site coherent potential approximation to noncollinear magnetic structures. Our results show that the noncollinear 3Q and 2Q structures are both stable solutions with the former being slightly lower in energy. The collinear solutions could only be converged in a traditional spin-polarized calculation and are unstable in a noncollinear treatment. © 1999 American Institute of Physics.
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  • 390
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4862-4864 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The present article reports a theoretical study of nondispersive magnetostatic forward volume wave (MSFVW) propagation in a double-layered yttrium–iron–garnet (YIG)-film structure consisting of two YIG films separated by a dielectric layer. Numerical computations are presented that show that a significant improvement in bandwidth for nondispersive MSFVW propagation can be obtained in the present separated double-layered YIG-film structure over the previously reported double-layered YIG-film geometry wherein the two YIG films were in direct contact. © 1999 American Institute of Physics.
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  • 391
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4877-4879 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We have investigated the texture and magnetic properties of Nd12Fe88−xBx sputtered films with various boron contents, x. The c-axis orientation of Nd2Fe14B phase in the films was higher and the perpendicular coercive force became greater with increment of x. With more increment of x than 15, however, the coercive force decreased owing to formation of a large amount of amorphous soft magnetic phase. The transmission electron microscope observations revealed that highly c-axis oriented Nd12Fe71B17 film has a unique microstructure; oriented Nd2Fe14B phase and amorphous phase with widths of about 200 and 50 Å, respectively, are alternately developed. This two-phase structure has realized an exchange coupled nanostructured magnet composed of aligned hard magnetic phase and soft magnetic phase. The maximum energy product of Nd12Fe71B17 film was estimated at 270 kJ/m3 with micromagnetic analysis assuming that the film was composed of complete regular structure. © 1999 American Institute of Physics.
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  • 392
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4874-4876 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The measurements of magnetization and magnetic anisotropy of R2Fe17 (R=Y, Er, Ho, and Gd) single crystals were performed under hydrostatic pressure up to 1 GPa, in temperature range 5–300 K and at magnetic fields up to 5 T, using the SQUID magnetometer with a miniature pressure CuBe cell. A pronounced decrease of spontaneous magnetization M of the R2Fe17 intermetallics has been observed under pressure. The values of dM/dp vary in an interval from −0.32μB/f.u. per kbar (Y2Fe17) up to −0.1μB/f.u. per kbar (Ho2Fe17). The R elements in the R2Fe17 intermetallics have a strong influence on the d(ln mFe)/dp values at 5 K. A remarkable decrease of the anisotropy constant with pressure, d ln K1/dp=−1.7×10−2 kbar−1 at 5 K, was observed on the Y2Fe17 compound. In the Gd2Fe17 compound, |K1(T)| increases with increasing pressure below 150 K and decreases with increasing pressure above this temperature value. The critical field HC(T) of the FOMP in the Er2Fe17 compound exhibits a similar behavior, it increases under pressure at temperatures below 60 K and decreases at higher temperatures. © 1999 American Institute of Physics.
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  • 393
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4898-4900 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Planar-type thin film inductors were fabricated using FeTaN soft magnetic films. It was found that excellent soft magnetic properties (coercivity of 0.1–0.2 Oe, effective permeability of 4000, and saturation magnetization of 15 kG) could be obtained in the Fe78.8Ta8.5N12.7 films after anneals at 400–500 °C. The initial permeability of the films was constant up to 20 MHz. Internal-coil inductors, in which Cu coils were sandwiched by SiO2 insulator/FeTaN magnetic layers, were fabricated and their characteristics were compared with air-core inductors. The inductance was increased by a factor of 4 compared to air-core inductors. However, the high frequency characteristic was degraded due to a frequency-limited permeability of FeTaN magnetic layers. © 1999 American Institute of Physics.
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  • 394
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4901-4903 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: This article is concerned with the design and construction of a bidirectional linear actuator capable of operating in ambient temperatures of up to 800 °C with a rated force of 300 N and a stroke of ±0.5 mm. The electromagnetic design synthesis strategy employed is described with particular emphasis on those aspects most markedly affected by the high operating temperature, viz. the selection of an appropriate actuator topology and the relative merits of candidate soft magnetic alloys. The key role of detailed thermal modeling, particularly the importance of radiation as a heat transfer mechanism in such high temperature applications, is illustrated during the design synthesis. The construction of a prototype actuator is discussed, including the use of tape would conductors with ceramic insulation and Inconel 600 disk springs as bearing elements. © 1999 American Institute of Physics.
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  • 395
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4919-4921 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: In order to clarify the influence of the impurities in the sputtering atmosphere on the exchange anisotropy of ferromagnet/antiferromagnet bilayers, Ni–Fe/Mn–Ni films were prepared under different purities of the sputtering atmosphere by changing the base pressure from 10−11 Torr [extremely clean (XC) process] to 10−7 Torr [lower grade (LG) process]. The correlation between the exchange anisotropy and the microstructure of the films is discussed. As a result, we found that: (1) The exchange anisotropy was enhanced in the XC processed films comparing to the LG processed ones, especially when the thicknesses of both the ferromagnetic and antiferromagnetic layers were very thin. (2) The critical thicknesses of the antiferromagnetic layers were 110 and 150 Å for the XC and the LG processed films, respectively. (3) In the XC processed films, the fcc-[111] direction of the Ni–Fe grains were highly oriented perpendicularly to the film plane and an enlargement of antiferromagnetic grains was observed. We conclude that the enhancement of exchange anisotropy is caused by the enlargement of antiferromagnetic grains in the XC processed films. © 1999 American Institute of Physics.
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  • 396
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4934-4936 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Ni–Fe/FeMn bilayers were deposited by using dual ion beam sputtering apparatus. In order to promote (111) orientation in γ-FeMn layers and to exhibit exchange bias field Hex, Si and/or silicon nitride (Si3N4) layers were deposited as buffer layers. Although silicon nitride (Si3N4) buffer layers did not improve (111) orientation in FeMn layers, as well as in Ni–Fe layers, an amorphous Si buffer layer only 1 nm thick improved (111) orientation in FeMn layers and increased Hex to above 100 Oe. FeMn/Ni–Fe bilayers deposited on Si(0.5 nm)/Si3N4(1 nm) bilayered buffer layer also exhibited high Hex of about 130 Oe. This result implies that the ultrathin a-Si buffer layer was effective in improving (111) orientation in Ni–Fe layers. Very thin Si/Si3N4 bilayers may be applicable as dielectric layers in tunneling magnetoresistive spin valve devices. © 1999 American Institute of Physics.
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  • 397
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4949-4951 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A spin wave theory is developed for ultrathin antiferromagnetic films in the regime where the effects of the dipole–dipole and exchange interactions may be comparable. A microscopic model with a Hamiltonian representation of the above terms is employed, giving a description of linear spin waves in lowest order and the dominant spin wave interactions as higher-order effects. Applications are made to rutile-structure antiferromagnets (such as MnF2), perovskite-structure antiferromagnets (such as RbMnF3), and layered antiferromagnets (such as K2NiF4), which exhibit quite different behavior. © 1999 American Institute of Physics.
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  • 398
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4943-4945 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The purpose of this work is to investigate the magnetic properties of Ti(tTi)/Fe(104 Å) bilayers deposited by dc magnetron sputtering onto MgO(100) substrates. In-plane ferromagnetic resonance (FMR) has been used to measure the resonance field HR and linewidth ΔH as a function of the azimuthal angle and Ti layer thickness. The FMR spectra were obtained at room temperature and at a microwave frequency of 12.3 GHz. The dependence of ΔH with respect to the azimuthal angle is explained by taking into account the combined effects of intrinsic damping and angular dispersion of the cubic axes. The dependence of the magnetic relaxation on Ti thickness exhibits two different regimes. It decreases for the first Ti layers (tTi〈30 Å) and increases up to a saturation value for Ti thickness around 90 Å. Other magnetic parameters such as effective magnetization, magnetocrystalline, and perpendicular anisotropies are also discussed. © 1999 American Institute of Physics.
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  • 399
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The degree of compensation of a normally uncompensated Cr(001) surface is controlled by using a curved substrate with steps parallel to the [100] direction. In this way, the degree of frustration caused by steps at the interface between an Fe overlayer and the Cr substrate can be systematically varied. Previous work on flat Cr(001) at temperatures below the Cr ordering temperature (311 K) has identified a critical Fe thickness of ∼35–38 Å, below which the Fe films display a reduced remanence. For our curved Cr substrate, below this critical Fe thickness three phases are observed for low (〈∼2.5°), intermediate and high (〉∼5°) miscut angle respectively: (i) multidomain; (ii) single domain with magnetization perpendicular to the step edges; and (iii) single domain with magnetization parallel to the step edges. At the same temperature, for Fe films above the critical thickness, region (i) disappears and only regions (ii) and (iii) remain. In a second experiment, the adsorption of submonolayer Au on the Fe is observed to increase the strength of the step-induced anisotropy and accordingly vary the position of the transition from regions (ii) to (iii). © 1999 American Institute of Physics.
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  • 400
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 5030-5032 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The giant magnetoresistance (GMR) effects in sandwiched Co/Cu/Co and Co/CuMn/Co structures have been investigated. The GMR oscillates with the spacer thickness for both cases, but is nearly antiphased. With diluted Mn atoms in the Cu spacer, the GMR curve as a function of the magnetic field changes a lot, and the saturation/switching field for GMR can be reduced greatly compared with that in Co/Cu/Co systems. This may indicate one way to obtain a highly sensitive GMR. © 1999 American Institute of Physics.
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