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  • American Institute of Physics (AIP)  (10,194)
  • Nature Publishing Group  (7,466)
  • 2000-2004  (14,126)
  • 1995-1999
  • 1975-1979  (3,534)
  • 2001  (14,126)
  • 1978  (3,534)
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  • 2000-2004  (14,126)
  • 1995-1999
  • 1975-1979  (3,534)
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  • 1
    Publication Date: 2017-01-04
    Description: Tropical South America is one of the three main centres of the global, zonal overturning circulation of the equatorial atmosphere (generally termed the 'Walker' circulation1). Although this area plays a key role in global climate cycles, little is known about South American climate history. Here we describe sediment cores and down-hole logging results of deep drilling in the Salar de Uyuni, on the Bolivian Altiplano, located in the tropical Andes. We demonstrate that during the past 50,000 years the Altiplano underwent important changes in effective moisture at both orbital (20,000-year) and millennial timescales. Long-duration wet periods, such as the Last Glacial Maximum—marked in the drill core by continuous deposition of lacustrine sediments—appear to have occurred in phase with summer insolation maxima produced by the Earth's precessional cycle. Short-duration, millennial events correlate well with North Atlantic cold events, including Heinrich events 1 and 2, as well as the Younger Dryas episode. At both millennial and orbital timescales, cold sea surface temperatures in the high-latitude North Atlantic were coeval with wet conditions in tropical South America, suggesting a common forcing.
    Type: Article , PeerReviewed
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  • 2
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    Nature Publishing Group
    In:  Nature, 412 . pp. 605-606.
    Publication Date: 2017-02-28
    Description: One way of accounting for lowered atmospheric carbon dioxide concentrations during Pleistocene glacial periods is by invoking the Antarctic stratification hypothesis, which links the reduction in CO2 to greater stratification of ocean surface waters around Antarctica1, 2. As discussed by Sigman and Boyle3, this hypothesis assumes that increased stratification in the Antarctic zone (Fig. 1) was associated with reduced upwelling of deep waters around Antarctica, thereby allowing CO2 outgassing to be suppressed by biological production while also allowing biological production to decline, which is consistent with Antarctic sediment records4. We point out here, however, that the response of ocean eddies to increased Antarctic stratification can be expected to increase, rather than reduce, the upwelling rate of deep waters around Antarctica. The stratification hypothesis may have difficulty in accommodating eddy feedbacks on upwelling within the constraints imposed by reconstructions of winds and Antarctic-zone productivity in glacial periods.
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  • 3
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    Nature Publishing Group
    In:  Nature, 410 (6827). pp. 427-428.
    Publication Date: 2017-02-28
    Description: To what extent was the Arctic Ocean glaciated in the past? Heavily, according to data, gathered by a submarine, which show considerable ice-scouring of topography in parts of the ocean basin
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  • 4
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 90 (2001), S. 4498-4501 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Multiphonon assisted frequency upconversion was observed in a Nd3+-doped fluoroindate glass pumped at 866 nm. A near-infrared upconverted emission at 750 nm with a peculiar linear dependence with the laser intensity was observed and explained. The intensity of the upconverted emission experienced a 40-fold enhancement when the sample's temperature was varied from 298 to 498 K. A rate equation model that includes light pumping and multiphonon absorption via thermally coupled electronic excited states of Nd3+ was used, describing quite well the experimental results. © 2001 American Institute of Physics.
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  • 5
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 90 (2001), S. 4502-4508 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The electromigration damage in flip chip solder bumps of eutectic SnPb and SnAg3.8Cu0.7 was studied after current stressing at 120 °C with 1.5 A. The diameter of the bumps was about 200 μm. The under-bump metallization (UBM) on the chip side was electroless Ni and on the board side was electroplated Cu. Surface marker motion was used to measure the atomic flux driven by electromigration and to calculate the effective charge number, Z*, of the solder. For eutectic SnPb, Z* is about 36–100 after 39.5 h of electromigration, but for SnAg3.8Cu0.7 the marker movement was too small to measure Z* even after 200 h of current stressing. While the effect of electromigration in SnAg3.8Cu0.7 is much smaller than that in eutectic SnPb, hillocks of intermetallic compounds at the anode have been observed in the former. An extensive growth of Ni–Cu–Sn intermetallic compounds in the matrix of both solder bumps was found. A localized dissolution of electroless Ni UBM was observed under current stressing, yet no dissolution of the Cu UBM by electromigration was found. © 2001 American Institute of Physics.
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  • 6
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 90 (2001), S. 4509-4519 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We use atomic-level simulation methods to determine the zero-temperature structure and properties of coherent KNbO3/KTaO3 superlattices. We find that the in-plane behavior is essentially bulk-like with an abrupt jump in the polarization at the interfaces. By contrast, the polarization in the modulation direction is continuous through the interfaces with the interior of the KTaO3 layers remaining polarized for modulation lengths of up to 160 unit cells. The zero-frequency dielectric constant in the modulation direction has a similar magnitude to that of KNbO3. An investigation of the switching behavior shows that for modulation lengths greater than 24 unit cells, each KNbO3 layer behaves essentially independently. For modulation lengths of less than 12 unit cells, the KNbO3 layers interact so strongly with each other that the superlattice essentially behaves as a single artificial structure. © 2001 American Institute of Physics.
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  • 7
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 90 (2001), S. 4520-4525 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Metal-containing carbon (Me-C:H) films were deposited using the electron cyclotron resonance chemical vapor deposition technique in conjunction with a metal screen-grid system. Four sets of Me-C:H films were analyzed using Raman scattering. Two sets were molybdenum-containing carbon (Mo-C:H) films deposited at fixed dc bias (at different CH4/Ar ratios), and at fixed CH4/Ar ratio (at different dc bias). Another two sets of nickel-containing carbon (Ni-C:H) films were deposited at fixed rf power, but at a different CH4/Ar ratio, with and without postgrowth thermal annealing at 200 °C. All films showed the characteristic G and D peaks except for those with high metal content. The D peak is very pronounced in the Ni-C:H films, and both the G and D peaks follow an opposite trend; downshifting and upshifting in wave number, respectively, as the CH4/Ar ratio was increased. In the case of Mo-C:H films deposited at fixed dc bias, both peaks downshifted in wave number, following an increase in the CH4/Ar ratio. The G peak full width at half maximum for both the Ni- and Mo-C:H films increased slightly with an increase in CH4/Ar ratio, consistent with the variation in the relative integrated intensity of the D to G peak (ID/IG). Thermal annealing experiments conducted on the film samples revealed relatively stable characteristics with a minor effect on the film structure. The results showed that the impinging ion energy plays an important role in the structural properties of the Me-C:H films. © 2001 American Institute of Physics.
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  • 8
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    Journal of Applied Physics 90 (2001), S. 4526-4531 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Electrical properties of single crystals of the MnPSe3, CdPSe3, and CdPS3 layered compounds have been investigated by in-layer dc conductivity and photoconductivity measurements as a function of temperature. The observed dc conductivity dependence exhibits a semiconductor behavior for all three compounds in spite of their high resistivity values. At high temperatures the dc conductivity of all three compounds shows an Arrhenius temperature dependence, while photoconductivity is thermally activated only for MnPSe3 and almost temperature independent for CdPSe3 and CdPS3. These results, interpreted in terms of the simplified energy-band schemes existing for CdPX3 and MnPSe3, have allowed us to identify the conduction mechanisms and to deduce more information about the distribution of the electronic states in the gap region. © 2001 American Institute of Physics.
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  • 9
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    Journal of Applied Physics 90 (2001), S. 4532-4542 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Temperature dependent ac dielectric spectroscopy and room-temperature I–V characterization were performed on atomic layer deposited (Ta1−xNbx)2O5 films. The high frequency permittivity, as well as the dc conductivity of the films, were found to increase with increasing Nb content. The conduction mechanism in the mixed Ta–Nb oxide films was of the Poole–Frenkel type, while the high field conduction in pure Ta2O5 was space-charge limited. The activation energy for dc conduction was higher in mixed Ta–Nb oxides compared to pure Ta2O5 and Nb2O5 films. Irreversible changes in the conduction mechanism took place upon heat treatment above a certain irreversibility temperature. This temperature was higher for the mixed oxides than for the binary ones. © 2001 American Institute of Physics.
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  • 10
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    Journal of Applied Physics 90 (2001), S. 4543-4548 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Current–voltage (I–V) and impedance measurements of oxidized metal/porous silicon (PS)/c-Si sandwich structures were performed at various temperatures. The I–V dependence at relatively small bias was found to be determined by the resistance of the PS layer. When the reverse bias is increased the injection of carriers commences. A power-law space charge limited current in the I–V dependence was observed at high forward bias. An exponential energy distribution of localized states with a characteristic energy of 60 meV was calculated from these. The existence of an inversion (n-type) layer with high conductivity was established in the p-type c-Si substrate adjacent to the PS layer. The presence of this inversion layer leads to an increase of the active device area, capacitance, and reverse current. © 2001 American Institute of Physics.
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  • 11
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    Journal of Applied Physics 90 (2001), S. 4549-4554 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Interfaces formed by evaporating Au on copper hexadecafluorophthalocyanine (F16CuPc) and F16CuPc on Au are studied via ultraviolet photoemission spectroscopy and x-ray photoemission spectroscopy. The energy position of the molecular levels is found to depend on the deposition sequence. The Au-on-F16CuPc interface exhibits a lower hole injection barrier than the F16CuPc-on-Au interface. This behavior is attributed to the diffusion of Au into the organic matrix at the Au-on-top interface, in which they behave as acceptors. Band bending consistent with p doping, i.e., upward away from the metal interface, is observed in Au-doped F16CuPc films. Current–voltage measurements on Au/F16CuPc/Au sandwich structures show a higher electron injection barrier at the top Au electrode contact than at the bottom electrode contact, also consistent with p-type doping F16CuPc by Au. © 2001 American Institute of Physics.
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  • 12
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    Journal of Applied Physics 90 (2001), S. 4555-4559 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Ohmic contacts comprised of the layer sequence of W/WC/TaC/SiC showed excellent thermal stability after testing at 600 °C for 1000 h. No degradation of the specific contact resistance nor a reaction of the film with the SiC substrate was observed. From Auger electron spectroscopy depth profiles, it was found that W and WC reacted to form W2C on TaC after annealing. After annealing for several hundred hours at 1000 °C, the specific contact resistance of the W/WC/TaC/SiC contacts displayed noticeable degradation. According to secondary ion mass spectrometry (SIMS) analysis, after annealing at 1000 °C for 600 h, small but measurable changes in the electrical characteristics were associated with O incorporation at the interface between TaC and SiC. Investigation of the W/WC/TaC/SiC interface by transmission electron microscopy (TEM) indicated that a reaction between the W and WC had occurred, but there was no observed reaction with the SiC substrate. After annealing for 1000 h, substantial changes in the chemistry, the microstructure, the specific contact resistance, and the spreading resistance of the contacts were observed. To understand the mechanisms associated with the degradation of the electrical properties, SIMS and TEM analyses were performed on samples annealed for 600, 700, 800, 900, and 1000 h at 1000 °C. These findings indicated that both oxidation and metallurgical reactions played important roles in the degradation of the electrical properties. © 2001 American Institute of Physics.
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  • 13
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    Journal of Applied Physics 90 (2001), S. 4565-4569 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We have characterized an InGaP/InGaAsN/GaAs NpN double-heterojunction bipolar transistor structure using polarized photoreflectance (PR) spectroscopy. The ordering parameter of the InGaP is deduced from the polarization {[110] and [11¯0]} dependence of the PR signals from the emitter region. The ordering related piezoelectric field is also found to influence the electric field, as evaluated from observed Franz–Keldysh oscillations, in the InGaP emitter region. The field in the emitter region is found to be about 25 kV/cm smaller than the theoretical value that does not take into account the possible ordering induced screening effect, while the field in the collector region agrees well with the theoretical value. In addition, the InGaAsN band gap is also determined by analyzing the PR spectrum of the base region. © 2001 American Institute of Physics.
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  • 14
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    Journal of Applied Physics 90 (2001), S. 4570-4577 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We present a tight-binding model of Zr silicate in the limit that every Zr and Si atom is bonded to four O atoms. We view the material as being composed of small, relatively uncoupled collections of atoms, called bonding units, with stoichiometries SiSiO4 and ZrSiO4. The SiSiO4 bonding unit constitutes a model for pure SiO2, and the ZrSiO4 bonding unit represents the fundamental element distinguishing tetrahedral Zr silicate from pure SiO2. In the first part of this article we look at the electronic structure of "ideal" bonding units in which the O atoms are arranged in a perfect tetrahedron and the M–O–Si angle is 180° (M=Si or Zr). We find the valence levels of both bonding units to be dominated by O p states, and the lowest conduction levels of the ZrSiO4 bonding unit to derive primarily from Zr d states, whose energy depends sensitively upon the charge transfer to the O atoms. The energy gap of the ideal ZrSiO4 bonding unit is found to be 5.9 eV, compared to 8.0 eV for the SiSiO4 bonding unit. Finally, for the ZrSiO4 bonding unit, we present a simplification which allows the energy levels of the ZrSiO4 bonding unit to be obtained approximately in terms of decoupled Zr–O and Si–O interactions. In the next part of the article we investigate how bond angle and bond length distortions affect the electronic structure of the ZrSiO4 bonding unit. In particular, we note that significant distortions of the Zr–O–Si angle could produce Zr-based localized states that could act as traps for electrons tunneling through the material. In the last part of the article we discuss the basic principles governing band lineups for Si/silicate interfaces constructed by substituting Zr atoms for Si atoms on the SiO2 side of crystalline Si/SiO2 interfaces. We calculate the band lineups as a function of Zr concentration for one particular interface. © 2001 American Institute of Physics.
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  • 15
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    Journal of Applied Physics 90 (2001), S. 4578-4582 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: In a junction system which consists of ferromagnetic- (La1−xSrx)MnO3 and band insulating-SrTiO3, the double exchange ferromagnetism in the (La, Sr)MnO3 layer was controlled by light irradiation through photocarrier injection form SrTiO3. We investigated the dependence of hole doping level (Curie temperature) on the photo control of the (La, Sr)MnO3/SrTiO3 heterojunction. Whereas magnetization and conductivity of the heterojunction with TC of 240 K is strongly reduced, including from metal–insulator transition, by light irradiation, that with TC of 280 K cannot be modulated. This result indicates that phase boundary, between the metallic and insulating region on the (La1−xSrx)MnO3 phase diagram, plays an important role in photo carrier control of the functional heterojunction. © 2001 American Institute of Physics.
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  • 16
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    Journal of Applied Physics 90 (2001), S. 4560-4564 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: For transport studies on semiconductor superlattices under optical excitation, samples with highly Si-doped (Al,Ga)As contact layers are used due to their optical transparency. These samples exhibit a giant increase of the resistance at temperatures below 200 K. Likewise, the current plateau in the I–V characteristics, which contains the region of current self-oscillations, is shifted towards higher voltages. However, the oscillation frequencies remain unchanged. The current decreases during cooling by as much as seven orders of magnitude. The giant resistance can be compensated for at low temperatures by applying a high dc voltage or by weak illumination. The optically induced current transients are shown to be controlled by thermally activated processes. On the basis of the activation energies derived, it is suggested that the dramatic resistance changes are mainly due to deep donors, i.e., well-known DX centers, in the (Al,Ga)As contact layers. The effects are negligible, if GaAs contact layers are used. Possible DX centers at the AlAs/GaAs interfaces inside the superlattice structure can be therefore neglected. © 2001 American Institute of Physics.
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  • 17
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    Journal of Applied Physics 90 (2001), S. 4583-4586 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Heat-flow changes of La1−xCaxMnO3+δ (x=0.25, 0.33, and 0.375) magnetoresistive oxides at their Curie temperatures have been detected using differential scanning calorimetry in the temperature range from 173 to 293 K. However, the transition does not occur in the samples of x=0.125 and 0.5. It was found that the heat flow reflected the transition behavior and the enthalpy change of the transition decreased as the transition temperature increased. These results indicate that the La1−xCaxMnO3+δ oxides (x=0.25, 0.33, and 0.375) undergo an endothermic phase transition from a low-temperature ferromagnetic metal to a high-temperature paramagnetic insulator. It is assumed that the transition is strongly associated with a local structure change, which is correlated with the metal–insulator transition. © 2001 American Institute of Physics.
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  • 18
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The high dielectric constant of insulators currently investigated as alternatives to SiO2 in metal–oxide–semiconductor structures is due to their large ionic polarizability. This is usually accompanied by the presence of soft optical phonons. We show that the long-range dipole field associated with the interface excitations resulting from these modes and from their coupling with surface plasmons, while small in the case of SiO2, for most high-κ materials causes a reduction of the effective electron mobility in the inversion layer of the Si substrate. We study the dispersion of the interfacial coupled phonon-plasmon modes, their electron-scattering strength, and their effect on the electron mobility for Si-gate structures employing films of SiO2, Al2O3, AlN, ZrO2, HfO2, and ZrSiO4 for "SiO2-equivalent" thicknesses ranging from 5 to 0.5 nm. © 2001 American Institute of Physics.
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  • 19
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    Journal of Applied Physics 90 (2001), S. 4609-4613 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Structural, magnetic, and transport properties of polycrystalline La0.7Ca0.3Mn1−xScxO3 have been experimentally investigated. Single-phase samples are obtained in the range 0≤x≤0.25 by the soft chemical synthesis route. The substitution of Sc3+ at the Mn site results in reductions in the Curie temperature Tc and in the magnetic moment per Mn ion. The Tc transition temperature becomes broader with x, and the magnetic spontaneous state has changed into a cluster glass state for the sample of x=0.1. In addition, great enhancement in resistance and magnetoresistance effect is observed in the Sc-doped samples. In our case the notable doping effects can be mainly ascribed to the variation in the Mn3+–O2−–Mn4+ network and to the magnetic disorder caused by the presence of the large and nonmagnetic Sc3+ ions in the Mn sublattice. © 2001 American Institute of Physics.
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  • 20
    ISSN: 1089-7550
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    Topics: Physics
    Notes: We have investigated the dependence of the critical current IC on the value and orientation of an externally applied magnetic field H for interface-engineered YBa2Cu3O7−x ramp-type Josephson junctions. The results are compared with measurements of Nb ramp-type junctions with a PdAu interlayer. The IC versus H dependences are similar to Fraunhofer patterns and their modulation period changes several orders of magnitude with the orientation of the magnetic field. For both junction types, the dependence of the modulation period on the orientation of the magnetic field can be well described by the change of the relevant projection of the junction area and the influence of flux-focusing. Therefore the features of the IC(H) curves have to be attributed to the ramp geometry and not to specific properties of the superconducting material. © 2001 American Institute of Physics.
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  • 21
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    Journal of Applied Physics 90 (2001), S. 4632-4638 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: In magnetic multilayers, the presence of sharp interfaces causes a local increase of the interaction between spin waves and conduction electrons. This leads to an increase of the Gilbert spin-damping parameter near an interface. In turn, the ferromagnetic-resonance linewidth is increased over its value in single-layer films. In addition, the precession of magnetic spins during ferromagnetic resonance induces conduction-electron transitions from the spin-up to the spin-down band. As a result, the spin-up Fermi level differs from the spin-down Fermi level by an amount Δμ¯. At high precession amplitudes, the existence of Δμ¯ causes a measurable decrease of the Gilbert parameter. At precession-cone angles exceeding 4°, the Gilbert parameter returns nearly to its single-layer value. Ferromagnetic-resonance line shapes are predicted to be non-Lorentzian, narrower and sharper near the top. This line-narrowing effect increases with increasing microwave power. The effect of Δμ¯ spreads into the entire multilayer, so that precession in one magnetic layer can cause a reduction or increase of the Gilbert parameter in other layers, or even a spontaneous spin precession in these layers. © 2001 American Institute of Physics.
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  • 22
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    Journal of Applied Physics 90 (2001), S. 4614-4622 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The relationships between both extensive and intensive properties quantifying the magnetocaloric effect, i.e., between the isothermal entropy change and the adiabatic temperature change, respectively, have been analyzed. An extensive measure of the magnetocaloric effect alone, without considering another important and also extensive thermodynamic property, i.e., the heat capacity, may lead to biased conclusions about the size of the magnetocaloric effect and, consequently, about the applicability of a magnetic material as a magnetic refrigerant. The near room temperature magnetocaloric properties of the colossal magnetoresistive manganites [(R1−xMx)MnO3, where R=lanthanide metal and M is alkaline earth metal] and the recently discovered Fe-based intermetallic material (LaFe11.47Co0.23Al1.3) have been reaccessed and correctly compared with those of the metallic Gd prototype. Our analysis has shown that these 3d materials are inferior to Gd by a factor of 2 or more because of the high values of the heat capacity per unit mass. Also a comparison of the volumetric isothermal entropy change, which is a critical parameter for the operation of a refrigeration unit, indicates that Gd is superior to these 3d materials for practical applications. © 2001 American Institute of Physics.
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  • 23
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    Journal of Applied Physics 90 (2001), S. 4639-4644 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Ac linear and nonlinear susceptibilities, χ0 and χ2, of ferrimagnetic FeCr2S4 single crystals were measured in the temperature range from 4.2 to 300 K for different driving ac and applied dc magnetic fields in the frequency range of 10−1–103 Hz. For high driving ac fields the real part of χ0 exhibits a cusp at around Tm(approximate)60 K correlated with the onset of dc magnetization irreversibilities. The imaginary part of χ0 shows a strong increase below 100 K and nonmonotonic temperature dependence with a maximum shifted toward low temperatures with an increase in the driving field. Both real and imaginary parts of the linear susceptibility, χ0′ and χ0″, show a pronounced frequency dependence between 90 and 20 K with a maximal difference at around 60 K. Below the Curie temperature the real part of the nonlinear susceptibility, χ2, exhibits a broad negative peak which is strongly shifted towards low temperatures with an increase in the driving field. No clearly divergent behavior of χ2′ around Tm is observed. The field and temperature dependencies of χ0 and χ2 are explained by domain wall pinning. Spin-glass-like magnetic anomalies at temperatures below 60 K are attributed to changes in the domain structure and the appearance of additional pinning centers suggested to result from a structural lattice transformation. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 4645-4650 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Brown's method of calculating an upper and a lower bound of the "critical size" for a single domain behavior is recalled, with a particular emphasis on the case of soft ferromagnets. The upper bound for a sphere is very slightly improved. Any further improvement, if at all needed for isolated particles of soft materials, should be done in the same direction. This improvement is used to demonstrate that this method can be extended to the case of interacting neighbors, but not to the study of very many grains, for which micromagnetics is inadequate and has to be superimposed by domain theory. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 4651-4656 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Off-aligned exchange coupling in bilayer thin film is investigated by torque curve and ferromagnetic resonance (FMR). In off-aligned exchange coupling, the unidirectional anisotropy axis makes an angle β with the anisotropy axis of the ferromagnetic layer. The torque curves of the off-aligned exchange are shifted with respect to the ones of the aligned case (β=0). From the experimental measure of the shift angle α0 and of the torque curve slope at α0, one can determine independently the exchange anisotropy field HE and β values. A description of the FMR modes in such an off-aligned exchange coupling is given. The FMR mode position and linewidth are studied as a function of the anisotropy fields, of the off-aligned angle values, and of the applied field direction. The resonance frequency and frequency linewidth present particular features which will help to do the right interpretation of FMR spectra of these systems. © 2001 American Institute of Physics.
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 90 (2001), S. 4657-4663 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: In this work we report on the experimental analysis of the time decay of magnetization in the films of amorphous TbFeCo alloys for perpendicular magnetic recording. It is shown that the experimental results can be explained on the basis of the thermally activated incoherent subnetwork magnetization reversal model. Thermally activated reversal of the transition metal subnetwork and associated reversal of the antiferromagnetically coupled rare-earth subnetwork may result in effective stabilization of the net film magnetization. Experimentally obtained activation diameter value Da∼5–6 nm corresponds to the exchange length or the domain wall width in the films under study. The small activation diameter value combined with high stability factor k∼250 mean that the TbFeCo amorphous film should be capable of supporting a thermally stable perpendicular recording at over 100 Gbit/in2 recording density. © 2001 American Institute of Physics.
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 90 (2001), S. 4664-4667 
    ISSN: 1089-7550
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    Topics: Physics
    Notes: Optically transparent SrTi1−xSbxO3 (=0.05, 0.10, 0.15, and 0.20) thin films with transmittances higher than 85% in the visible region have been grown on SrTiO3 substrates by pulsed-laser deposition. Unless overdoped, the films possess a single-crystal phase and impurity conduction. The temperature dependence of the resistivities shows a metal–semiconductor transition for the film with x=0.05, and semiconducting behaviors for the films with x=0.10 and 0.15. The overdoped film with x=0.20 is an insulator. Sb concentration has a dominant effect on the electrical properties of the films, and the Anderson localization is probably the mechanism. X-ray photoelectron spectroscopy results indicate that the Sb impurity atoms provide donor electrons to form impurity states within the band gap, which is responsible for the electrical localized impurity. The wide band gap and the low density of states in the conduction band result in the transparency of the films. The disorder increases with Sb concentration, which is the main origin of the evolution of the electrical properties. © 2001 American Institute of Physics.
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 90 (2001), S. 4668-4675 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Losses in piezoelectrics are approached by considering a description of direct stress–charge displacement hysteresis. Shortcomings of the usual loss models (viscous and Rayleigh, taken separately) are briefly demonstrated. Then, a mixed model for piezoelectric losses superimposing viscous and Rayleigh types of descriptions is proposed and validated for a modified lead titanate and lead zirconate titanate (PZT). It is shown for PZT that viscous and Rayleigh-like loss contributions can be effectively separated by fitting the piezoelectric hysteresis loop with an expression combining the two lossy responses. The possibility to obtain all the necessary parameters that describe piezoelectric stress nonlinearity from one single piezoelectric loop is also demonstrated in the case of PZT. The origins of the mixed loss behavior are interpreted as arising from domain wall motion in terms of internal friction mechanisms and of pinning energy ranges. © 2001 American Institute of Physics.
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 90 (2001), S. 4859-4861 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We observe that the emission wavelength of edge-emitting InGaAs quantum dot lasers has a much weaker temperature dependence (0.6 Å K−1) than equivalent quantum well devices (3 Å K−1). Measured gain and absorption spectra show that the gain peak wavelength due to dot states is almost independent of temperature for a given value of peak gain whereas the absorption edge shifts at a rate of about 2 Å K−1. Above 100 K the occupancy of dot states can be described by Fermi functions and on this basis we find that the measured gain and absorption spectra are in excellent quantitative agreement. Although the band edge energy reduces with increasing temperature, this analysis shows that the energy distribution of dot states matches the evolution of the Fermi functions such as to leave the quasi Fermi level separation and the wavelength of the gain peak unchanged as a function of temperature for a given value of peak gain. This energy distribution is a consequence of the dot size distribution so the match to the Fermi functions is probably fortuitous. © 2001 American Institute of Physics.
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 90 (2001), S. 4862-4864 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The application of a near-field optical device to the electrochemical deposition of submicron nickel dots on silicon is demonstrated. The silicon–electrolyte junction behaves like a Schottky diode where the electrolyte plays the role of the metal. The junction is reverse biased so that only a negligible dark current is flowing across the junction. The optical tip of the near-field device is used as a local lightsource to control a photocurrent on a submicron scale, which allows one to create submicron objects of nickel by locally triggering the electrochemical reduction of nickel ions. The effect of the lateral diffusion of the photogenerated carriers on the form of the deposited nickel dots is described by a two-dimensional carrier diffusion model. © 2001 American Institute of Physics.
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 90 (2001), S. 4865-4867 
    ISSN: 1089-7550
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    Topics: Physics
    Notes: Neodymium (III) oxide nanocrystals synthesized by the inverse microemulsion technique were dispersed in sol–gel titania/organically modified silane (ormosil) composite thin films for photonic applications. X-ray diffraction analysis and transmission electron microscopy observation show that the neodymium oxide nanoparticles have a nanocrystalline structure and that the size of the nanoparticles is in the range of 5–60 nm. An intense room-temperature yellow-to-violet upconversion emission at 402 nm (4D3/2→4I13/2) was measured from the composite thin film heated at 100 °C upon excitation with a yellow light at 587 nm. In addition to this violet emission, ultraviolet emission at 372 nm and blue emission at 468 nm were also observed. The lifetime of the violet emission was measured and the mechanism of the upconversion emission is proposed, and they indicate excited-state absorption originating from the long-lived 4F3/2 excited state should be responsible for the yellow-to-violet upconversion. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 4868-4870 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Plasma-induced molecular beam epitaxial AlInGaN heterostructures have been characterized by spatial resolved cathodoluminescence and x-ray energy dispersive microanalysis. Competitive incorporation of Al and In has been observed, with the formation of In-rich regions, showing enhanced luminescence around surface pinholes. These island-like In-rich regions are favored by growth at lower temperature due to the higher incorporation of indium into the alloy. The elastic strain relaxation associated to pinhole formation induces preferential local indium incorporation. The diffusion of carriers to these areas with reduced band gap enhances the luminescence emission of the quaternary film. The width and intensity of the luminescence appear to be sensitive to the mismatch between the quaternary film and the GaN layer below. © 2001 American Institute of Physics.
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 90 (2001), S. 4871-4873 
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    Topics: Physics
    Notes: The stopping cross sections of the III–V semiconductor materials GaN and InP for 0.3–2.5 MeV 1H have been studied by the Rutherford backscattering technique. The data are given with an estimated uncertainty better than 2% and the agreement with earlier data existing for InP below 500 keV is good. A commonly used model ZBL-85 predicts the data correctly at the high energy end of our energy interval, but overestimates the stopping values by 7% and 4% for GaN and InP, respectively, at the lower energies. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 4874-4876 
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    Topics: Physics
    Notes: Current–voltage (I–V) characteristics of Pr0.5Sr0.3Ca0.2MnO3 are measured at different temperatures and different fields. Our data of I–V curves show a crossover from linear to nonlinear behavior at the temperature lower than the charge ordering temperature. New findings in this work include (i) abrupt jumps/drops of voltage in each I–V curve below 100 K and (ii) an enhancement of magnetoresistance (MR) ratio from 15% to 20% which is associated with the unusual voltage jumps/drops in I–V curves. The enhancement of MR ratio evidences the existence of an intermediate state between the charge ordering state and the charge ordering breakdown state. Most importantly, the existence of such intermediate state provides a new route to achieve a low field colossal magnetoresistance for future applications of spintronics. © 2001 American Institute of Physics.
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 90 (2001), S. 4880-4881 
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    Topics: Physics
    Notes: Recent electronic structure calculations for the title compounds performed by Wu et al. [H. Wu et al., J. Appl. Phys. 87, 4897 (2000)] are critically reconsidered by applying highly accurate full-potential band structure methods. It is shown that due to a nonconverged basis set the band structure calculations presented here by the authors disagree considerably with those of Wu et al. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 4877-4879 
    ISSN: 1089-7550
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    Topics: Physics
    Notes: We have grown epitaxial and polycrystalline LaMnOy thin films on a LaAlO3 substrate by the off-axis magnetron sputtering technique and investigated the crystalline orientation effects on the electronic transport properties. Lattice mismatch, crystalline quality, resistivity, resistivity transition temperature Tp, and magnetoresistance (MR) in epitaxial films exhibit crystalline orientation dependence. The largest Tp and MR are observed in the (111) oriented films. In the polycrystalline films, the Tp is smaller than that of the (011)/(111) oriented films but higher than that of the (001) oriented films. The MR increases with decreasing temperature in contrast to that of the epitaxial films in which the MR experiences a peak near Tp. Oxygen annealing decreases MR and resistivity, and increases Tp in the order: (111)〈(011)〈(001)〈(polycrystalline). The above results suggest that the structure and composition of the epitaxial films improve in the order: (001)〈(011)〈(111). © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 4882-4883 
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    Topics: Physics
    Notes: An improvement is made on our previous band results of Sr2CuO3 and Sr2CuO2Cl2 by including the extended Sr 4p valence orbital in the present self-consistent calculations. The differences between our improved results and those of others are mainly due to different evaluation of the ionicity in these compounds. © 2001 American Institute of Physics.
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 90 (2001), S. 3675-3678 
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    Topics: Physics
    Notes: The construction and properties of scattering type liquid crystal depolarizers are discussed. The Mueller matrices that describe these devices are measured and compared to ideal depolarizers and ideal linear materials. The present depolarizers do not perform as well as crystal pseudodepolarizers. Nevertheless, when polarized light is incident on one of these devices the polarization of the transmitted light can be uniform to within 5%. These devices have the advantage that they can be made to areas as large as 30–30 cm or larger, are inexpensive, and can be electrically switched off and on. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 3679-3688 
    ISSN: 1089-7550
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    Topics: Physics
    Notes: We present a generalized model for the photochemical cycle of bacteriorhodopsin (bR) protein molecule. Rate equations have been solved for the detailed light-induced processes in bR for its nine states: B→K↔L↔MI→MII↔N↔O↔P→Q→B. The complete steady-state intensity-induced population densities in various states of the molecule have been computed to obtain a general, exact, and analytical expression for the nonlinear absorption coefficient for multiple modulation pump laser beams. All-optical light modulation of different probe laser beam transmissions by intensity induced population changes due to one and two modulation laser beams has been analyzed. The proposed model has been shown to accurately model experimental results. © 2001 American Institute of Physics.
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 90 (2001), S. 3689-3698 
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    Topics: Physics
    Notes: The operation of a planar diode with a large area (64 cm2) ferroelectric plasma cathode based on BaTiO3 ceramics is studied. Diode parameters and parameters of the generated electron beam are investigated under accelerating voltage of 200–350 kV and pulse duration of 250 ns. Parameters of the plasma, which forms on the surface of the ferroelectric cathode due to incomplete discharge, are reported as well. It is shown that the application of this cathode allows one to produce an electron beam simultaneously with application of the accelerating pulse. The generation of an electron beam with current density up to 20 A/cm2 and divergence of less than 1° is demonstrated. It is shown that diode operation is governed by parameters of the cathode plasma which fills the anode–cathode gap prior to application of the accelerating voltage pulse. By proper adjustment of the cathode and diode parameters the operation of the diode with almost constant impedance is achieved. Measurements of the potential distribution in the diode confirm that the diode operates in a plasma-prefilled mode. The cathode is found to be capable of operating for up to 105 pulses at a repetition rate of few Hz without any maintenance and with relatively small vacuum deterioration. © 2001 American Institute of Physics.
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 90 (2001), S. 3699-3712 
    ISSN: 1089-7550
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    Topics: Physics
    Notes: The ability to deposit power in the volume of plasma reactors at locations deeper than the conventional skin depth makes magnetically enhanced inductively coupled plasma (MEICP) and helicon sources appealing for use in materials processing. Mechanisms for power deposition and electron energy transport in MEICPs have been computationally investigated using a two-dimensional (2D) plasma equipment model. Using a tensor conductivity in the solution of Maxwell's equations, three-dimensional components of the inductively coupled electric field are produced from an m=0 antenna and 2D applied magnetic fields. These fields are then used in a Monte Carlo simulation to generate electron energy distributions (EEDs), transport coefficients, and electron impact source functions. The electrostatic component of the wave is resolved by estimating the charge density using an oscillatory perturbed electron density. For MEICPs operating at pressures less than 10 mTorr in Ar, significant power deposition occurs downstream when the radial and axial components of the electric field are commensurate with the azimuthal component. For magnetic fields above 100 G, the tail of the EED (〉20–30 eV) is enhanced in the downstream region. This enhancement results from noncollisional heating by the axial electric field for electrons in the tail of the EED which have long mean free paths, while lower energy electrons are still somewhat collisional. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 3713-3719 
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    Topics: Physics
    Notes: We studied the mechanism and behavior of a plasma in the presence of an external electric field with a one-dimensional fluid model. We used a two-fluid model, treating both electron and ion motions, rather than a commonly used one-fluid model assuming the electron thermal equilibrium. In particular, we investigated the following issues: (1) the motion of plasma electrons caused by an external static electric field and the formation of a plasma potential; (2) influence of parameters on the plasma potential, which are plasma electron temperature, plasma density, and applied voltage. The plasma potential rises and reaches a value nearly equal to the anode potential in a few nanoseconds. It is higher for a higher anode potential, a higher electron temperature, and a lower plasma density. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 3720-3725 
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    Topics: Physics
    Notes: The electron density and the electron temperature in a low-pressure neon mercury positive column are determined using Thomson scattering. Special attention has been given to the stray light reduction in the Thomson scattering setup. The results are obtained in a discharge tube with a 26 mm diam, 10 mbar of neon, a mercury pressure inbetween 0.14 and 0.85 Pa, and an electric current ranging from 100 to 400 mA. The systematic error in the electron density is 15%–45%, the statistical error is 25%–35%. The total error in the electron temperature is 15%–35%. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 3735-3742 
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    Topics: Physics
    Notes: We have performed an experimental and theoretical analysis of the rf discharges at low pressure in a small reactor for industrial applications. In particular, we focused on the plasma produced from electronegative gases (air and SF6) in the low pressure range between 0.05 and 1 mbar. The device pumping system sustains a flow velocity of about 50 cm/s, with residence time in the discharge of about 0.2 s, at P=0.1 mbar. The discharge parameters have been measured by means of movable electrostatic probes and lies in the range ne≅107–109 cm−3, ni≅1010–1012 cm−3, and Te≅5–10 eV. Particular care in the analysis of the data proved necessary due to the presence of a substantial amount of negative ions. On the other hand, we have performed simulations of the discharge composition through the implementation of a suitable numerical model of the chemical kinetics in the device. On the basis of the experiments, a comparison of charged species production with those predicted by the theory was performed and a more realistic description of the involved phenomena was obtained. In particular, several assumptions concerning the ion diffusion coefficient were tested, allowing one to pin down the relative importance of transport and bulk processes in the discharge state. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 3743-3749 
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    Topics: Physics
    Notes: In plasma immersion ion implantation (PIII), ions bombard all surfaces inside the PIII vacuum chamber, especially the negatively pulsed biased sample stage and to a lesser extent the interior of the vacuum chamber. As a result, contaminants sputtered from these exposed surfaces can be reimplanted into or adsorb on the silicon wafer. Using particle-in-cell theoretical simulation, we determine the relative ion doses incident on the top, side, and bottom surfaces of three typical sample chuck configurations: (i) a bare conducting stage with the entire sample platen and high-voltage feedthrough/supporting rod exposed and under a high voltage, (ii) a stage with only the sample platen exposed to the plasma but the high-voltage feedthrough protected by an insulating quartz shroud, and (iii) a bare stage with a silicon extension or guard ring to reduce the number of ions bombarding the side and bottom of the sample platen. Our simulation results reveal that the ratio of the incident dose impacting the top of the sample platen to that impacting the side and bottom of the sample stage can be improved to 49% using a guard ring. To corroborate our theoretical results, we experimentally determine the amounts of metallic contaminants on 100 mm silicon wafers implanted using a bare chuck and with a 150 mm silicon wafer inserted between the 100 mm wafer and sample stage to imitate the guard ring. We also discuss the effectiveness of a replaceable all-silicon liner inside the vacuum chamber to address the second source of contamination, that from the interior wall of the vacuum chamber. Our results indicate a significant improvement when an all-silicon liner and silicon guard ring are used simultaneously. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 3750-3753 
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    Topics: Physics
    Notes: Beryllium and magnesium were co-implanted with oxygen into GaN at precise donor-to-acceptor ratios of 0.5–2. High activation efficiency was achieved for Be+O co-implants at a donor–acceptor ratio of 2 and anneal temperatures of 1050–1100 °C. The activation process was not a simple, single-step mechanism. Hall data indicated a relatively low (≤100 meV) ionization energy for Be in the co-implanted samples. This process may have application in improving p-ohmic contact resistance by selective area Be+O implantation. By sharp contrast Mg+O co-implants produced n-type conductivity under all conditions. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 3754-3761 
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    Topics: Physics
    Notes: Temperature distributions in overdriven steady wave fronts in solid 2024 Al shocked up to 80 GPa, in which no melting occurred in the wave fronts, were evaluated using the equilibrium thermodynamic theory. The effective strain increments were sufficiently small and the effective temperature rise times were sufficiently long with respect to electron–phonon relaxation times to justify using equilibrium thermodynamics. In addition, the sufficiently large viscous-stress components supported the efficacy of the thermodynamic theory. The same is true of shocks up to 250 GPa in solid Pt and 230 GPa in solid Fe. Furthermore, the influence of viscous stress was examined by evaluating the temperature distributions for inviscid 2024 Al, Pt, and Fe solids using the equations for temperature derived from the Mie–Grüneisen equation. Finally, we demonstrate that there might be a solid–liquid–solid Hugoniot between the solid and liquid–solid Hugoniots for Fe and estimate the solid–liquid–solid and liquid–solid Hugoniots. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 3762-3770 
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    Topics: Physics
    Notes: We construct the Green function for an elastic medium with a plane source. This Green function is particularly helpful in the analysis of weakly nonlinear problems, such as occur in nondestructive acoustic evaluation of bonded structures. By using a perturbative approach we describe the amplitude distribution of the second harmonic of the driving frequency by linear equations with sources. In deriving the Green function we include both longitudinal and transverse polarizations and consider an arbitrary direction of the wave vector with respect to the layer normal. We show how this Green function can be combined with the transfer matrix approach to calculate the fields in layered structures. The examples of second harmonic generation from half space and a single layer are considered. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 3504-3508 
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    Topics: Physics
    Notes: Complex impedance spectroscopic data were acquired on single crystals of the morphotropic phase boundary composition of 0.68Pb(Mg1/3Nb2/3)O3-0.32PbTiO3 over a wide range of temperatures (25–525 °C) and frequencies 1 kHz–1 MHz. This study takes advantage of plotting ac data simultaneously in the form of impedance and modulus spectroscopic plots. This permits the easy interpretation of microscopic processes responsible for the measured ac response. Frequency explicit plots of imaginary components of impedance and modulus exhibit Debye-like peak shapes. The data for ac conductivity were computed from the impedance data and the activation energy for conduction at different frequencies was determined. Cole–Cole diagrams were plotted and these indicate the presence of a single relaxation process. The relaxation times determined from these plots followed an Arrhenius law, and the activation energy for relaxation was found to be 1.2 eV. The ac conductivity data was found to obey Jonscher's universal power law and resulted in a value of the exponent "n"=0.95. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 3516-3523 
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    Topics: Physics
    Notes: The luminescence of nanocrystalline cubic yttria has been measured for 300 and 80 K. A blueshift and a broadening of the absorption edge, both depending on the particle size were found. The energy of the radiation emitted due to the recombination of a bound exciton does not depend on particle size. The observations are not caused by quantum or phonon confinement. Using a quantum mechanical configurational coordinate diagram an explanation can be given. Hydrostatic pressure increasing the phonon energy of the excited state of the bound exciton, or an increase of the exciton-phonon coupling may generate the size dependent optical properties of nanocrystalline yttria. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 3524-3528 
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    Topics: Physics
    Notes: Metal–oxide–semiconductor structures with a Ge nanocrystal embedded in SiO2 films were fabricated by Ge+ ion implantation and subsequent high-temperature annealing. The Raman spectra indicate the evidence of self-assembled Ge nanocrystals in the SiO2 films. The Ge size and its density were estimated to 3–5 nm and 1×1012/cm2, respectively. Photoluminescence spectra showed a strong blue–violet band around 400 nm and a weak near-infrared band around 750 nm, respectively. The several implantation-induced deficient centers are believed to be responsible for the blue-light luminescence. Capacitance–voltage characteristics exhibit the flatband voltage shifts of 1.02 V after the electron injection into the SiO2/Ge/SiO2 potential well. An anomalous leakage current was clearly observed in the current–voltage characteristics. The precise simulation of quantum electron transport in the SiO2 film indicates that the anomalous conduction is originated from resonant tunneling in the SiO2/Ge/SiO2 double-well band structure. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 3529-3532 
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    Topics: Physics
    Notes: Anisotropically nanostructured silicon layers exhibit a strong in-plane birefringence. Their optical anisotropy parameters are found to be extremely sensitive to the presence of dielectric substances inside of the pores. Polarization-resolved transmittance measurements provide an extremely sensitive tool to analyze the adsorption of various atoms and molecules in negligible quantities. A variation of the transmitted linearly polarized light intensity up to two orders of magnitude combined with a fast optical response in the range of seconds make these layers a good candidate for sensor applications. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 3533-3538 
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    Topics: Physics
    Notes: Simple, double-rectangular spiral-type thin-film inductors with an upper Ni81Fe19 core for 5 MHz drive dc–dc converter application were investigated. Copper films 10-μm-thick covered by a 3-μm-thick NiFe film were used as the coils. The inductors fabricated in this study are 2.5×3.4–3.5×5.5 mm2. The inductors developed, with a small size of 2.97×3.1 mm2, exhibit L of 1.43 μH, quality factor of 15.8, and resistance of 2.88 Ω at 5 MHz, and show results comparable to those reported in recent literature for similar inductors sandwiched by more complex magnetic core materials. An analysis of the experimental data suggests an equivalent circuit of the fabricated inductors. From the equivalent circuit analysis, C was shown to have a negligibly small effect over the frequency ranges used. The calculated data obtained from the equivalent circuit and the well-known equation of Q described the high-frequency data of the L, Q, and impedance of the inductors developed well. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 3551-3557 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We report on a silicon single-electron tunneling device fabricated in an ultrathin (∼3 nm) silicon-on-insulator (SOI) film whose surface is undulated by an alkaline-based solution. The nanometer-scaled undulation in the ultrathin film results in great SOI thickness variations and brings about large electron-potential fluctuations, due to the difference of the quantum confinement effects from one part to another. Consequently, a number of quantum dots are effectively formed in the undulated ultrathin SOI film. This device shows clear Coulomb blockade oscillations at 80 K, as well as nonvolatile single-electron memory functions even at room temperature. The measurements of the undulation with atomic force microscopy reveal that the undulation has two correlation lengths. Based on the analysis of electrical characteristics, it is concluded that the Coulomb blockade oscillations are dominated by a quantum dot formed by the longer-correlation-length undulation and that single-electron memory effects are due to quantum dots formed by the shorter-correlation-length undulation. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 3539-3550 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Theory and line-shape analysis of carrier recombination current at interfacial electronic traps under a surface controlling gate in metal–oxide–silicon (MOS) structures is investigated using the Shockley–Read–Hall recombination statistics. The theoretical analysis demonstrates the sensitive dependence of the line shape of the peaked basewell-terminal recombination current versus gate/base voltage (IB–VGB) characteristics on the lateral variation of the impurity concentration along the surface channel. An electrical measurement method is presented based on this discovery for extracting the impurity surface concentration profile NIM(x=0, y, z) in the five regions (basewell, drain and source junction and extension) covered by the gate conductor in submicron MOS transistors. Impurity surface concentration profiles in the basewell channel region are then extracted by the analytical theory for MOS transistors fabricated by an advanced 0.13 μm complementary MOS technology. Effects of nitrogen in the gate oxide and current generated in the drain and source extension regions for profiling the NIM in the extension regions are illustrated. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 3558-3565 
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    Topics: Physics
    Notes: The effects of particle irradiation on the electrical properties of high efficiency p/n InP solar cells have been studied using a variety of techniques including current–voltage and spectral quantum efficiency measurements (QE), electron beam induced currents (EBIC), and deep level transient spectroscopy. A detailed analysis of the radiation response of the solar cell photovoltaic response is presented, and the primary damage mechanisms are identified. Data measured after irradiation by protons of various energies are correlated in terms of displacement damage dose to produce a characteristic degradation curve for the p/n InP technology. This characteristic curve is compared to that of the n/p InP technology to provide an assessment of the relative radiation hardness of the p/n devices. Radiation-induced decreases in the minority carrier diffusion length in both the p-type emitter and n-type base at low damage levels have been extracted from the QE and EBIC measurements, and damage coefficients have been determined. At high damage levels, EBIC profiles suggest that the primary device degradation mechanism is an increase in bulk resistivity due to electron trapping in the base. However, capacitance–voltage measurements did not indicate any change in the junction capacitance. A model to account for these effects based on radiation-induced defect kinetics is presented. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 3570-3577 
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    Topics: Physics
    Notes: We demonstrate that a large area Josephson junction oscillating in the fluxon oscillator mode can be synchronized to other large junctions and simultaneously pump, by emitted radiation, a small area junction. We study the synchronization of the oscillations of the long junctions as a function of relevant experimental parameters such as bias current and stripline coupling characteristics. Experimental results obtained on coupled series arrays of Josephson junctions designed on the basis of our calculations are presented. We have fabricated coupled arrays containing each up to 1500 junctions in order to estimate the usefulness of our calculations for voltage standard devices. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 3566-3569 
    ISSN: 1089-7550
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    Topics: Physics
    Notes: We describe fast recovery at a wavelength of 1550 nm in a multiple-quantum-well (MQW) saturable absorber with InGaAsP quaternary wells and barriers using electric-field-induced carrier sweepout. The MQW SA is integrated with a distributed Bragg reflector in a p-type–intrinsic–n-type structure. Pump–probe measurements show that the recovery time can be reduced from 〉900 to 28 ps by application of a 151 kV/cm sweepout field. We measure the dependence of the recovery time on the energy of the saturating pulse and explain our results in terms of carrier dynamics in the sweepout field. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 3831-3837 
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    Topics: Physics
    Notes: We investigate physical properties of polymer dispersed liquid crystal transmission gratings which influence the light diffraction efficiency behavior. Scanning electron microscopy is used to determine the orientation and shape of nanometer-sized liquid crystal droplets in a polymer host. Dependence of diffraction efficiency on light polarization suggests that the orientation of a liquid crystal within the ellipsoidal droplets is axial. The distribution of droplet orientations appears to vary for different grating spacings. The switching properties of the gratings are investigated and analyzed with a sinusoidal dielectric tensor modulation model. The analysis also takes into account orientational distribution of average directors and spatial distribution of the droplets. Temperature dependence of diffraction efficiency is tentatively explained by a structural transition within the droplets and the presence of impurities in droplets. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 3595-3601 
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    Topics: Physics
    Notes: The property of extreme ultraviolet (EUV) generation from Xe clusters irradiated with intense lasers was studied. The Xe cluster jet was well characterized by the interferometric method. In order to obtain the adequate irradiation condition for strong EUV generation, EUV spectra were taken with various laser systems. Then, the wavelength, the pulse width, and the pump energy were widely varied. Through this survey, even with the comparatively low-density Xe jet of ≤5×1018 cm−3 average atomic density, the highest conversion efficiency of over 10% from laser energy to EUV (5–18 nm) was obtained with a subpicosecond KrF laser pulse, where a 4π source was assumed. This EUV source is considered to be attractive as an EUV lithography light source because of its low average atomic density and small Xe cluster. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 3873-3878 
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    Topics: Physics
    Notes: Arsenic implants performed in Si at ultralow energy have been extensively studied with structural, chemical, and electrical analysis. The near-surface damage annealing and its influence on the electrical activation of ultrashallow As in Si as a function of the anneal ambient has been investigated. Double alignment medium energy ion scattering, high resolution transmission electron microscopy, and low energy secondary ion mass spectrometry have been used to assess the dopant behavior and crystal recovery in the near-surface regions. The electrical activation of As in Si has been measured with spreading resistance profiling, four point probe, and van der Pauw methods. Major redistribution of the dopant into the SiO2–Si interface region occurred during crystal regrowth of the damaged Si layer. An inactive meta-stable As solid solution was formed in the near-surface region after amorphous layer regrowth. Electrical activation of the dopant occurred upon dissociation of the As solid solution, when the dopant concentration fell to the steady state level. The As diffusion observed has been shown to be enhanced for short (10 s) anneal times at 1100 °C. When annealing at high temperature in an oxidizing ambient the dopant is retained at a high concentration in the solid and a higher level of electrical activation is observed. Significant outdiffusion of the dopant is observed during high temperature annealing in nonoxidizing conditions which reduced the level of activation. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 3894-3898 
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    Topics: Physics
    Notes: The AgInS2 epilayers with a chalcopyrite structure grown using a hot-wall epitaxy method have been confirmed to be a high quality crystal. From the optical absorption measurement, the temperature dependence of the energy band gap on AgInS2/GaAs was found to be Eg(T)=2.1365 eV−(9.89×10−3 eV)T2/(2930+T). After the as-grown AgInS2/GaAs was annealed in AgInS2/GaAs has been investigated by using the photoluminescence (PL) at 10 K. The native defects of VAg, VS, Agint, and Sint obtained from PL measurements were classified as a donors or acceptors type AgInS2/GaAs to an optical p type. Also, we confirmed that In in AgInS2/GaAs did not form the native defects because In in AgInS2 did exist in the form of stable bonds. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 3887-3893 
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    Topics: Physics
    Notes: This article reports a selective-area deposition process using chlorosilane-treated ultrathin SiO2 masks on which the patterns are directly defined by irradiation of a focused electron beam (EB). Three different chlorosilane gases (SiH2Cl2, SiHCl3, and SiCl4) were first adsorbed on the SiO2 surfaces, and the regions with reactive sites were defined by taking advantage of electron-stimulated desorption (ESD) of the surface adsorbates. For the SiHCl3- and SiH2Cl2-treated surfaces, the nucleation density was remarkably high in the EB-irradiated regions. Such nucleation enhancement was less significant for the SiCl4-treated surface. For the purpose of direct patterning and selective growth, we conclude that SiHCl3 is the optimum treatment gas because it effectively suppresses Si nucleation outside of the EB-irradiated patterns. The overall ESD sensitivity of the SiHCl3-adsorbed mask was 50 mC/cm2, and a significant nucleation enhancement was observed by irradiation of 7 mC/cm2. We also report an extension of this selective-area processing to window opening through the ultrathin SiO2 mask layer. The factors limiting the minimum feature size of the grown Si structures and the opened windows are discussed. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 3905-3909 
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    Topics: Physics
    Notes: We predict that singular photonic Bloch modes with extremely narrow bandwidths occur in dual-periodic dielectric multilayer structures. The electromagnetic field of these modes is shown to be strongly localized around the troughs of undulated periodic dielectric structures, which leads to an extraordinary high-Q value effect in the dual-periodic one-dimensional photonic crystals. We also propose several real systems suitable for experimental confirmation of the features predicted. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 3899-3904 
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    Topics: Physics
    Notes: Despite their technological importance for nanoscale technologies, the initial stages of reaction at interfaces (and their dependence on experimental conditions) are still poorly understood. In this article we analyze the initial stages of solid state reaction (SSR) in Al/Pt multilayers (period: 54 nm, overall composition: Al4Pt) and compare the results to those recently obtained by high temperature sequential deposition (HTSD). These two methods differ in several aspects, the most important being the state of reacting Pt (solid in SSR, vapor in HTSD) and its flux (limited in HTSD by the deposition rate). The chemical driving force for the Al/Pt reaction are thus different. We have shown that: (i) The first reaction product observed during SSR or HTSD is the same: namely, a metastable amorphous Al2Pt phase (a-Al2Pt): (ii) This amorphous phase grows in a layer by layer mode. Its growth is diffusion controlled during SSR and stops when all the available Pt is consumed. In the case of HTSD the layer growth is limited by the Pt evaporation rate and diffusion only controls the "critical" thickness that the amorphous layer can reach. (iii) The Al diffusion coefficients in a-Al2Pt deduced from the a-Al2Pt growth rate (SSR) or "critical" thickness (HTSD), using the Nernst–Einstein equation in order to take into account the difference in the chemical driving forces, are similar. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 3910-3918 
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    Topics: Physics
    Notes: Epitaxial metastable Ge1−yCy alloy layers with y≤0.035 were grown on Ge(001) from hyperthermal Ge and C atomic beams at deposition temperatures Ts of 250 and 300 °C. The use of hyperthermal beams allows us to controllably vary the concentration of C incorporated as Ge–C split interstitials. Ge1−yCy layers grown with incident Ge-atom energy distributions corresponding to ≤0.14 lattice displacement per incident atom (dpa) are in a state of in-plane tension and contain significant concentrations of C atoms incorporated in substitutional sites. Increasing the dpa to 0.24 yields layers in compression with C incorporated primarily as Ge–C split interstitials. Ab initio density functional calculations of the formation energies and strain coefficients associated with C atomic arrangements in Ge show that configurations containing multiple C atoms, referred to collectively as C nanoclusters, are energetically more favorable than substitutional C and Ge–C split interstitials and yield a nearly zero average strain. In contrast, substitutional C and Ge–C split interstitials produce large tensile and compressive strains, respectively. Using the calculated strain coefficients, measured layer strains obtained from high-resolution reciprocal lattice maps, and substitutional C concentrations determined by Raman spectroscopy, we obtain the fraction of C atoms incorporated in substitutional, Ge–C split interstitial, and nanocluster sites as a function of the total C concentration y and Ts. We find that at low y and Ts values, all C atoms are incorporated in single-C configurations: substitutional C and Ge–C split interstitials. Their relative concentrations are controlled by the dpa through the production of near-surface Ge self-interstitials which are trapped by substitutional C atoms to form Ge–C split interstitials. Increasing y and Ts, irrespective of the dpa, leads to an increase in the fraction of C nanoclusters, while the fractions of substitutional C and Ge–C split interstitials decrease, due to the higher C–C encounter probability at the growth surface. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 2792-2795 
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    Topics: Physics
    Notes: Microscopic observation and imaging of Cu damascene interconnect grains were carried out using the x-ray microbeam of the BL-16XU at SPring-8. The x-ray focusing system of the beamline consists of a bent-cylindrical prefocusing mirror and elliptical mirrors with a Kirkpatric–Baez configuration. Diffraction spots from the microscopic area irradiated by the intense x-ray microbeam (7×6 μm full width at half maximum) at the boundary between the metal line and the dielectric were observed. The diffraction spots observed show that Cu(111) grains grow normally on the sidewall and Cu(200) grain orientation distribution is quite broad, suggesting that crystallographic texture near the trench is quite disordered. Two-dimensional images of grains with a specific orientation angle were also obtained. Grains as large as about 10 μm caused by self-annealing were observed. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 3942-3951 
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    Topics: Physics
    Notes: Direct current and alternating current electrical measurements were performed to investigate the electrical conductivity of α-Al2O3:Mg samples with different concentrations of [Mg]0 centers (Mg ions each with a trapped hole) in the temperature interval 250–800 K. The concentration of [Mg]0 centers was monitored by the optical absorption peak at 2.56 eV. These centers were produced by oxidation at temperatures above 1050 K. The formation rate of [Mg]0 centers depends on the previous thermal history of the sample in either reducing or oxidizing atmosphere. At low electrical fields, dc measurements reveal blocking contacts. At high fields, the I–V characteristic is similar to that of a diode (corresponding to a blocking contact at one side of the sample and an ohmic contact at the other side) connected in series with the bulk resistance of the sample. Steady electroluminescence is emitted at the negative electrode when a current in excess of (approximate)10 μA passes through the sample, indicating that the majority of carriers are holes. Low voltage ac measurements show that the equivalent circuit for the sample is the bulk resistance in series with the junction capacitance (representing the blocking contacts) connected in parallel with a capacitance, which represents the dielectric constant of the sample. The values determined for the bulk resistance in both dc and ac experiments are in good agreement. The electrical conductivity of Al2O3:Mg crystals increases linearly with the concentration of [Mg]0 centers, regardless of the amount of other impurities also present in the crystals, and is four times higher in the c(parallel) than in the c⊥ direction. The conductivity is thermally activated with an activation energy of 0.68 eV, which is independent of: (1) the [Mg]0 content, (2) the crystallographic orientation, and (3) the concentration of other impurities. These results favor the small-polaron-motion mechanism. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 3965-3972 
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    Topics: Physics
    Notes: The spectroscopic properties of crystals of CaF2:U4+ have been examined in light of recent interest expressed for this material as a saturable absorber in the passive Q switching of near infrared solid state lasers. The detailed crystal-field splitting of the energy levels of U4+(5f2 ) is analyzed for the ion in different charge-compensated sites. Identification of the site is based on laser excited site-selective spectroscopic studies reported earlier. Experimental Stark levels are compared with calculated levels based on lattice-sum models that include charge compensation in the lattice structure. The final set of atomic parameters for U4+ is in good agreement with values reported for the ion in UF4. The predicted non-Kramers' doublet as the ground-state Stark level for U4+ in C3V sites is in agreement with the spectroscopic analysis and with results reported earlier from electron spin-resonance studies of CaF2:U4+. Using pump–probe methods, we have investigated excited state absorption (ESA) at 1.54 μm. Consistent with the interpretation of the absorption spectra, we find that the measured ESA is quite small in these crystals. In turn, we use this conclusion to model CaF2:U4+ as a passive Q switch, with good results. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 3979-3983 
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    Topics: Physics
    Notes: We propose a mechanism for negative differential conductance in nanometric single barrier heterostructures when transport is controlled by tunneling processes and space charge effects. Theoretical expectations are confirmed by Monte Carlo simulations of a model GaAs–GaAlAs–GaAs semiconductor heterostructure. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 3988-3992 
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    Topics: Physics
    Notes: Mid-infrared photoluminescence has been observed from interface transitions in high quality, abrupt P–Ga0.84In0.16As0.22Sb0.78/p-InAs heterojunctions grown by liquid phase epitaxy from an In-rich melt. The Ga0.84In0.16As0.22Sb0.78 quaternary epitaxial layer was unintentionally doped and grown lattice matched on to a (100) oriented p-type InAs substrate, resulting in a P–p isotype heterojunction. The photoluminescence emission spectra were investigated and exhibited three pronounced emission bands in the spectral region from 0.30 to 0.68 eV; hν1=0.317 eV, hν2=0.380 eV, and hνL=0.622 eV. The emission band hν1 was identified with radiative transitions between electron and hole quantum well subbands in the semimetal channel at the P–GaIn0.03As0.10Sb/p-InAs interface, while the hν2 band originates from radiative transitions involving deep acceptor states in the InAs substrate. The high-energy recombination hνL is characteristic of the Ga0.84In0.16As0.22Sb0.78 bulk quaternary layer. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 4019-4026 
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    Topics: Physics
    Notes: Here we investigate dc characteristics, impedance versus frequency, and low frequency noise. The effect of current distribution on 1/f noise in polycrystalline silicon thin film transistors (TFTs) is discussed. We show that the channel impedance versus frequency roll induces spectra that could be misinterpreted above a corner frequency in terms of a frequency index γ in 1/fγ with γ higher than 2. Moreover, ignoring the inhomogeneous current distribution leads to overestimation of the noise parameter. Whereas it seemed evident that the noise in TFTs can be interpreted in terms of carrier number fluctuation, the noise parameter variation versus the gate bias can be also understood in terms of mobility fluctuations by including the potential barrier evolution. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 4032-4038 
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    Topics: Physics
    Notes: The properties of p-AlGaN/GaN modulation doped superlattices (SLs) prepared by molecular beam epitaxy were studied by means of conductivity versus temperature, admittance spectroscopy, photoinduced current spectroscopy, microcathodoluminescence (MCL) spectra measurements, and measurements of effective diffusion lengths. It is shown that in SLs grown on GaN underlayers the sheet resistivity is about two orders of magnitude lower than for reference p-GaN films and the resistivity of SLs remains lower up to temperatures of about 350 °C. For SLs grown on AlGaN underlayers the gain in resistivity is much more moderate and certain advantages in using such SLs are envisaged only for temperatures below room temperature. The reason for this lower gain is a considerable decrease in hole mobility compared to p-GaN. The effect is somewhat tentatively attributed to worse crystalline perfection of these SLs. It is also shown that such SLs are characterized by a strongly broadened MCL peak and the presence of additional hole traps with activation energy of about 0.4 eV. Despite that, the photosensitivity and MCL intensity of these SLs are much better than for reference p-GaN samples. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 4039-4043 
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    Topics: Physics
    Notes: Ta/NiOx/Ni81Fe19/Ta multilayers were prepared by rf reactive and dc magnetron sputtering. The exchange-coupling field (Hex) and the coercivity (Hc) of NiOx/Ni81Fe19 as a function of the ratio of Ar to O2 during the deposition process were studied. The composition and chemical states at the interface region of NiOx/NiFe were also investigated using the x-ray photoelectron spectroscopy (XPS) and peak decomposition technique. The results show that the ratio of Ar to O2 has a great effect on the nickel chemical states in NiOx film. When the ratio of Ar to O2 is equal to 7 and the argon sputtering pressure is 0.57 Pa, the x value is approximately 1 and the valence of nickel is +2. At this point, NiOx is antiferromagnetic NiO and the corresponding Hex is the largest. As the ratio of Ar/O2 deviates from 7, the exchange-coupling field (Hex) will decrease due to the presence of magnetic defects such as Ni+3 or metallic Ni at the interface region of NiOx/NiFe, while the coercivity (Hc) will increase due to the metallic Ni. XPS studies also show that there are two thermodynamically favorable reactions at the NiO/NiFe interface: NiO+Fe=Ni+FeO and 3NiO+2Fe=3Ni+Fe2O3. These interface reaction products are magnetic defects at the interface region of NiO/NiFe, it is believed that these magnetic defects would have an effect on the exchange-coupling field (Hex) and the coercivity (Hc) of NiO/NiFe. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 4056-4062 
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    Topics: Physics
    Notes: In this study we examine the role of crystallographic structure on the magnetization reversal of two CoCrPtTa thin films grown on different underlayers which provide either a [112¯0] or a [101¯0] preferred orientation. We report synchrotron x-ray measurements and find that the stacking fault density in a CoCrPtTa thin film with a (101¯0) texture is greater than that in a sample having the (112¯0) bicrystal texture (13% compared to 8%). However, we also find that the degree of in-plane texture is poorer in the (101¯0) film. We report extensive magnetic measurements on the two films and find that increased switching at low fields correlates well with the observed level of fcc-like regions. In particular we show that a significant increase in magnetic viscosity at low fields in the (101¯0) film is most probably due to the increased level of low anisotropy fcc-like regions of Co formed by the stacking faults rather than small grains or poor texture. This is supported to some extent by the bimodal behavior observed in the activation volumes for the [101¯0] film, one peak being observed as expected around the coercivity (∼3 kOe) and another at a much lower field (∼1.2 kOe). © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 4063-4077 
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    Topics: Physics
    Notes: Recent comparative studies of quasiparticle injection from colossal magnetoresistance (CMR) materials and normal metals into high transition temperature superconductors (HTS) have led several investigators to conclude that spin-polarized injection from CMR electrodes is far more efficient than ordinary injection in suppressing superconductivity. On the other hand, some ordinary quasiparticle injection experiments have shown greater suppression of superconductivity than was claimed in any of the published spin-injection experiments. Careful analysis and numerical simulations lead us to argue that all spin-injection experiments to date have been hampered by inadequate control samples and that the reported results can be explained by ordinary (unpolarized) quasiparticle injection or simple current summation. We conclude that there is no conclusive evidence that spin-polarized injection into HTS behaves differently from ordinary quasiparticle injection and we discuss criteria for future experiments that could differentiate between the two types of injection. © 2001 American Institute of Physics.
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 90 (2001), S. 4089-4094 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Ferroelectric properties along the a(b) axis and c axis in single crystals of various bismuth layer-structured ferroelectrics (BLSFs) were investigated. By measuring saturated P-E hysteresis curves of BLSFs, values of the saturated remanent polarization and the coercive electric field were found to be related to the Curie temperature and the number of BO6 octahedra (m) between bismuth layers, respectively, along the a(b) axis. The saturated remanent polarization was larger in the BLSF with a higher Curie temperature. This is attributed to a large atomic displacement accompanied by a high Curie temperature. In contrast, the saturated coercive electric field was smaller in the BLSF with a larger number of m. This phenomenon is assumed to be caused by the decrease in the strain energy of the octahedra from the bismuth layer, which leads to an easy movement of the octahedral cations in the direction of an applied external electric field. Along the c axis, the BLSFs with an odd number of m had the same relationship, that is, the saturated remanent polarization was larger with the high Curie temperature, and the saturated coercive field was smaller with the large m number. However, no remanent polarization was confirmed in the BLSFs with an even number of m. © 2001 American Institute of Physics.
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 90 (2001), S. 4103-4107 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We report a comparative study of the electrical properties of some oxides e.g., Gd2O3, Ga2O3(Gd2O3), Y2O3, and Ga2O3 as gate dielectric for strained Si0.74Ge0.26 metal–oxide–semiconductor devices. Secondary ion mass spectroscopy spectra of the Ga2O3(Gd2O3)/SiGe sample showed a significant amount of GaO and GdO along with Ga and Gd signals. The depth profile taken for O, Si, SiO, Ga, Ge, Gd, and GdO showed sharp interface at about 20 nm. Though Gd2O3 and Y2O3 showed the highest resistivity and breakdown strength, Ga2O3(Gd2O3) was found to be most effective for surface passivation of SiGe giving lowest interface state density while pure Ga2O3 was incapable of passivating the SiGe surface. The positive fixed oxide charge and interface state density for Ga2O3(Gd2O3) film were found to be 8.4×1010 cm−2 and 4.8×1011 eV−1 cm−2, respectively, which are the lowest among all the oxide films of the present study. © 2001 American Institute of Physics.
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 90 (2001), S. 4122-4129 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Lead zirconate titanate (PZT)/epoxy 1–3 piezocomposite rings were fabricated with PZT volume fractions φ ranging from 0.82 to 0.94 and with a small epoxy width of 77 μm in order to investigate their resonance characteristics and to reveal the mode coupling. Four major resonance modes were observed, namely the coupled longitudinal-thickness fH and lateral fL1 and fL2 mode resonances of individual PZT elements inside the rings as well as the radial fR and wall-thickness fW mode resonances of the whole rings. No stopband resonances were observed in the frequency range of 1 to 10 MHz. fH was found to increase linearly with the decrease in element height while fL1 and fL2 remained constant. When the height and width of the elements became comparable, coupling of fH with fL1 and fL2 occurred. The observed fH, fL1, and fL2 for all samples agreed with those calculated by the mode-coupling theory. fR and fW were almost independent of the ring thickness but increased as φ increased. A guide of operating fH in the rings without causing mode coupling was presented to optimize the composite structure for transducer design. © 2001 American Institute of Physics.
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 90 (2001), S. 4138-4142 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Co0.2Zn0.8Fe2O4 nanoparticles have been synthesized by the coprecipitation method. Nanoparticles with average particle size of 5–∼65 nm were obtained by sintering the samples from 393 to 1173 K. Magnetic measurements show that samples with particle size ≤13 nm are superparamagnetic above the blocking temperature TB. Samples with average particle size larger than 13 nm have a wide particle size distribution and show the presence of two magnetic phases: superparamagnetic and cluster glass. Cation distribution of the samples show that in the samples with particle size 〈13 nm Fe ions are distributed between the tetrahedral and octahedral sites of the spinel lattice but in the larger particle size samples the tetrahedral sites have very few Fe ions that form Fe–Fe clusters and hence the high temperature sintered samples show a mixed phase, consisting of superparamagnetic and cluster glass. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 4143-4151 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We present a critical theoretical study of electronic properties of silicon nanoclusters, in particular the roles played by symmetry, relaxation, and hydrogen passivation on the stability, the gap states and the energy gap of the system using the order N [O(N)] nonorthogonal tight-binding molecular dynamics and the local analysis of electronic structure. We find that for an unrelaxed cluster with its atoms occupying the regular tetrahedral network, the presence of undistorted local bonding configuration is sufficient for the appearance of a small clean energy gap. However, the energy gap of the unrelaxed cluster does not start at the highest occupied molecular orbital (HOMO). In fact, between the HOMO and the lower edge of the energy gap, localized dangling bond states are found. With hydrogen passivation, the localized dangling bond states are eliminated, resulting in a wider and clean energy gap. Relaxation of these hydrogen passivated clusters does not alter either the structure or the energy gap appreciably. However, if the silicon clusters are allowed to relax first, the majority of the dangling bonds are eliminated but additional defect states due to bond distortion appear, making the energy gap dirty. Hydrogen passivation of these relaxed clusters will further eliminate most of the remnant dangling bonds but no appreciable effect on the defect states associated with bond distortions will take place, thus still resulting in a dirty gap. For the hydrogen-passivated SiN nanoclusters with no bond distortion and no overall symmetry, we have studied the variation of the energy gap as a function of size of the cluster for N in the range of 80〈N〈6000. The dependence of the energy gap on the size shows similar behavior to that for silicon nanoclusters with no bond distortion but possessing overall symmetry. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 3118-3120 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The persistent photoconductivity (PPC) induced by visible light of a He–Ne laser with a wavelength of 632.8 nm in perovskite manganite films of (La0.3Nd0.7)2/3Ca1/3MnO3 at low temperatures, below ∼50 K, was observed. Based on the measurements of transport and magnetic properties, it is suggested that the samples undergo a transition of cluster-glass state below ∼50 K. The PPC phenomenon can be qualitatively explained in terms of a photoinduced ferromagnetic cluster growth model. © 2001 American Institute of Physics.
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 90 (2001), S. 4169-4174 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Uniformly dispersed zinc ferrite nanoparticles were successfully synthesized in a silica matrix with both the magnetic properties and optical transparency designed in the visible wavelength region. The phases and morphologies of these zinc ferrite particles were examined using x-ray diffraction, Raman spectroscopy and transmission electron microscopy. A much lower formation temperature of ZnFe2O4 in nanocomposites was observed in this study compared to in conventional ceramic processing. The particle size of zinc ferrite was found to vary with the initial drying temperature, suggesting that a well-established silica network provides more confinement to the growth of ZnFe2O4 particles. The magnetic properties, measured at both 78 K and room temperature, exhibit strong dependence on the particle size, and are related to the unusual cation distribution and the surface effect of nanoparticles. The optical properties of the nanocomposites can be adjusted by varying the concentration of the zinc ferrite nanoparticles. Their absorption coefficient remains below 400 cm−1 in the red visible light region. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 3925-3933 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The epitaxial growth of Y (hydride) films on CaF2(111) has been investigated using x-ray photoelectron spectroscopy, x-ray photoelectron diffraction, and low energy electron diffraction (LEED). For Y deposition at 700 °C the formation of high-quality epitaxial hcp(0001) oriented Y films is observed. Whenever the Y films showed good surface quality, the surface is rich in F. Only when the deposition temperature was chosen so low that the LEED reflexes were very broad was no fluorine detected. This is a strong indication that F acts as a surfactant. For Y deposition at room temperature under a H2 partial pressure of 5×10−6 mbar we observe the formation of a F-free, transparent YH2.3 film of a red/yellow color and poor crystallinity. Hydrogen unloading is accomplished by annealing to 600 °C. The film loses its transparency, the poorly ordered fcc(111) lattice converts to a well-ordered hcp(0001) lattice, and F contamination is restored. © 2001 American Institute of Physics.
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    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 90 (2001), S. 3952-3955 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The formation energies of planar defects such as lamellar twins and intrinsic and extrinsic stacking faults in CdTe are calculated using first-principles total-energy calculations. We find that the formation energies, 16 erg/cm2 for lamellar twins and 34 and 31 erg/cm2 for intrinsic and extrinsic stacking faults, are very small. This explains why high densities of planar defects are always present in the fast-grown CdTe thin films. The effects of the planar defects on the formations of important point defects in p-type CdTe are also investigated. We find that the planar defects have negligible effects on Cd vacancies and substitutional Cu, whereas they lower the formation energy of Te antisites by about 0.1 eV compared to the perfect regions. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 4219-4223 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Etching characteristics of nondoped GaN films with the polar surface in KOH solution have been investigated. It is confirmed that the continuous etching in KOH solution takes place only for the GaN films with N-face (−c) polarity independent of the deposition method and growth condition. It is found by x-ray photoelectron spectroscopy (XPS) analysis for the Ga face (+c) and N-face (−c) GaN films that the atomic composition of the +c surface is not changed before and after dipping in KOH solution and that on the other hand, the amount of oxygen (oxide) on the −c surface is significantly decreased by the etching. It is also found that the band bending increases by −0.4±0.2 and 0.6±0.2 eV for the +c and −c surfaces after etching, respectively. This is discussed in terms of the surface chemistry. Based on the XPS result, the selective etching of the GaN polar surface is pointed out to originate from bonding configuration of nitrogen at the surface. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 4231-4236 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Among the various techniques that have been investigated to produce Hydroxyapatite (HA) coatings in order to promote fixation and osteointegration of cementless prosthesis, the plasma spray (PS) technique is the most popular method commercially in use. PS presents some disadvantages such as the poor coating-to-substrate adhesion, low mechanical strength, and brittleness of the coating. In order to overcome the drawbacks of plasma spraying, an approach on how to bind HA to the Ti alloy will be introduced in this work, using a well-known technique in the metallurgical field: laser surface cladding. Different techniques were applied to characterize the coated samples, including x-ray diffraction, scanning electron microscopy, and energy dispersive x-ray analysis. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 4251-4255 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We used the microwave technique to measure electrical properties of heavily boron doped diamond films. This technique overcomes problems such as the presence of parasitic resistance due to the electrical contacts. The conductivity of these films is rather high (about 104 S m−1). The measured microwave conductivity has the same values as the dc conductivity. The conductivity varies with the doping. The highest value of conductivity does not appear for the highest value of doping, because of the presence of a parasitic phase. This will be proved by electron spin resonance and Raman spectra. Theoretical calculation rules out the skin effect in our measurements. It will be also possible to perform microwave photoconductivity measurements. The photoconductivity behavior varies in the opposite way to the conductivity. One explanation, based on the recombination time which decreases with the conductivity, will be presented. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 4272-4280 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: In this study, we present a detailed structural characterization by means of transmission electron microscopy and Raman spectroscopy of polymorphous silicon (pm-Si:H) thin films deposited using radio-frequency dust-forming plasmas of SiH4 diluted in Ar. Square-wave modulation of the plasma and gas temperature was varied to obtain films with different nanostructures. Transmission electron microscopy and electron diffraction have shown the presence of Si crystallites of around 2 nm in the pm-Si:H films, which are related to the nanoparticles formed in the plasma gas phase coming from their different growth stages, named particle nucleation and coagulation. Raman scattering has proved the role of the film nanostructure in the crystallization process induced "in situ" by laser heating. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 4281-4283 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A wide optical gain spectrum with full width at half maximum Δλ(approximate)350 nm has been demonstrated in midinfrared (2.2–2.5 μm) room-temperature-operated InGa(As)Sb/GaSb quantum-well (QW) ridge-waveguide diode lasers. A QW width of 200 Å ensured a small energy separation between the first and second quantized states in the QW. Transitions from both quantized states contributed equally to the overall gain spectrum when the optical loss was optimized. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 4287-4289 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We report the growth of a transparent, p-type semiconductor, CuSCN, in nanometer sized channels of a thin polyester foil. High energy heavy ion irradiation and subsequent etching is used to prepare vertical cylindrical channels in polymers with diameters in the range 30–3000 nm. Electrodeposition is then used to fill these channels with polycrystalline CuSCN. The embedding is robust against mechanical stress on the foil. Since the bulk modulus of the inorganic CuSCN is larger than that of the polymeric matrix, only small forces act on the embedded semiconductor, resulting in low electrical changes upon bending or flexing of the foil. Dissolving the polyester matrix results in free-standing semiconductor columns with height-to-diameter ratios in excess of 100. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 4007-4018 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: WO3 films, either prepared by sputtering or evaporation under high or ultrahigh vacuum conditions, were irradiated with He+ and Ar+ ions (energy range 300–350 keV) at ambient and low temperatures (77–100 K). The resulting ion induced changes of the optical absorption as well as of the electrical conductivity could be determined on one and the same sample, which enables the variable range hopping (VRH) model to be tested under the assumption that the density of irradiation induced color centers is proportional to the electronic density of states contributing to the hopping conductivity. It is found that the data obtained at 300 K for He+ and Ar+ bombardment can be described within the VRH model by one common conductivity versus absorption curve, even though the effectiveness per projectile of the heavier ion for coloration as well as for increasing the conductivity is much higher. This is different at low temperatures. While the ion induced coloration is practically independent of the irradiation temperature for both projectiles, the effectiveness per projectile to enhance the conductivity is interchanged. This is attributed to the additional damage produced by the heavier ion at low temperatures resulting in strongly impeded hopping processes. Consistent with the VRH model, the temperature dependence of the conductivity of ion bombarded WO3 films follow the Mott "T−1/4" law, if the ion induced conductivity is not too high. For very high ion fluences clear deviations from the VRH model are observed for the conductivity versus absorption curves accompanied by a shift of the above power laws from T−1/4 towards T−1/2. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 2314-2320 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Reported here are some temperature-dependent and excitation-dependent photoluminescence (PL) results from chlorine-doped ZnSe layers grown by molecular beam epitaxy. The PL spectrum is characterized by an overwhelming exciton recombination emission at 2.797 eV (10 K) near the band edge, and no other PL features are found. This overwhelming neutral donor-bound exciton (Cl0X) emission line at 2.797 eV (10 K) with a full width at half maximum (FWHM) of ∼13 meV reveals the high crystalline quality of the samples. The quick quenching of this exciton line above 200 K is due to the presence of a nonradiative center with a thermal activation energy of ∼90 meV. The decrease of the Cl0X line over the temperature range from 10 to 200 K is due to the thermal activation of Cl0X bound excitons to free excitons with an activation energy of ∼9.0 meV. The change of the emission nature occurs at about ∼200 K from Cl0X bound exciton recombination to free exciton recombination; accordingly, a kink appears on the temperature-dependent FWHM curve at ∼190 K. The broadening behavior of the Cl0X line over the temperature range 10–200 K can be understood within the theoretical framework of the phonon scattering model, while the impurity scattering mechanisms are responsible for the broadening of the exciton line above 200 K. This PL peak does not shift with the change in excitation power, while the integrated intensity increases exponentially with the increase in excitation power, i.e., IPL∝Iex1.21, indicating the competition between the radical recombination process and the nonradical recombination process of photogenerated carriers. The FWHM remains unchanged when the excitation power was varied from 0.5 to 50 W cm−2, and then increases exponentially when the excitation power exceeds 50 W cm−2. However, the PL peak consists of four exciton subpeaks, and these subpeaks do not broaden. The PL peak is found to broaden due to recombination competition among the four kinds of excitons. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 2329-2332 
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    Source: AIP Digital Archive
    Topics: Physics
    Notes: The deactivation of nitrogen acceptors confined in Cd0.96Zn0.04Te/Cd0.86Zn0.14Te quantum well structures by hydrogen (deuterium) have been investigated by optical spectroscopy. Hydrogen (deuterium) was incorporated into the samples by annealing them in an atmosphere of hydrogen and cadmium. The annealing temperature and annealing time were varied to determine the optimum condition at which the maximum passivation is achieved without causing structural degradation. The emissions related to nitrogen acceptors were monitored in low-temperature photoluminescence measurements in order to deduce the passivation effect. The results indicate that hydrogen can effectively neutralize the nitrogen acceptors in cadmium zinc telluride quantum well structures. It is estimated that as much as 90% of the nitrogen acceptors can be passivated by this method. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 2347-2351 
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    Topics: Physics
    Notes: The effect of hydrostatic pressure P up to 1 GPa and applied magnetic fields H up to 1.5 T on the magnetic and transport properties of La0.91Mn0.95O3 doped with 7 at. % Zn at the temperature range of 15–350 K is reported. It was found that the doping by Zn changes the low temperature conductance from a metallic-like to a nonmetallic one. Doping by Zn of the initial self-doped sample shifts the Curie temperature from 252 to 204 K. In both compounds the applied pressure enhances the ferromagnetic coupling and Curie temperature. The pressure coefficients of the Curie temperature are equal for both compounds being dTC/dP(approximate)13 K/GPa. Above the Curie temperature the resistivity of Zn-doped manganite obeys Mott's law rather than the Arrhenius behavior. Both parameters, A and T0 of Mott localization law decrease under pressure indicating a reduction in the localization energy. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 2370-2379 
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    Topics: Physics
    Notes: A significantly large thermoelectric "figure of merit" in a bipolar semiconductor is achieved by converting it, by doping, into an essentially monopolar semiconductor. We show here, that for a bipolar semiconductor film, having a thickness smaller than the screening length, there is an alternative to doping to obtain a practically monopolar semiconductor. The electric-field effect (EFE) or the ferroelectric-field effect can be used to quench the concentration of one type of charge carriers. We show that this method is particularly suited for narrow-gap semiconductors and for semimetals, having sufficiently high dielectric permittivity. We also show that this "EFE doping" is free from the drawbacks of conventional doping. Our analysis demonstrates that increased values of the figure of merit are feasible. We present here the theory and the figure-of-merit calculation for typical cases of the bipolar semiconductor thermoelectric film under EFE doping. Numerical results for a film of the PbTe type are presented. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 2416-2421 
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    Topics: Physics
    Notes: The properties of the Barkhausen noise in a series of permalloy squares have been measured with a magneto-optical hysteresigraph. The magnetic structures have been litographically defined in a permalloy film (thickness 160 nm) as squares having a size from 20 to 320 μm. The statistical distributions of the most significant parameters of the Barkhausen jumps have been extracted from the original data. At variance with respect to bulk and thin films, the jump amplitude distribution does not follow a well-defined power-law behavior. This observation is explained in terms of a transition between a discrete magnetization regime typical of small magnetic structures and the more usual regime observed in extended samples. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 2397-2404 
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    Source: AIP Digital Archive
    Topics: Physics
    Notes: The minority carrier lifetime in boron-doped oxygen-contaminated Czochralski (Cz) silicon is strongly reduced under illumination or carrier injection. This process can be fully reversed by a 200 °C anneal step. In several recent studies it was shown that boron and oxygen are the major components of the underlying metastable Cz-specific defect. The energy level of the defect in its active state A was determined to be around midgap [Schmidt et al., J. Appl. Phys. 86, 3175 (1999)] while the energy level of the defect in its passive state P is very shallow. The Cz-specific defect in its passive state can be identified with the shallow thermal donor. The kinetics of the excess carrier-induced transformation from state P to state A can be described using recombination-enhanced defect reaction theory. On the basis of these experimental facts different solutions for the reduction or elimination of the metastable defect are suggested. Two promising solutions are discussed in more detail: the use of gallium-doped Cz silicon and the introduction of high-temperature anneals into the process sequence. Gallium-doped Cz silicon shows no degradation and excellent lifetimes over a wide resistivity range, although the concentration of interstitial oxygen is in the same range as in standard Cz silicon. Stable solar cell efficiencies comparable to FZ silicon have been achieved. If standard boron-doped Cz silicon is used, the defect concentration can be reduced permanently by a high-temperature anneal using conventional tube or rapid thermal processing. This leads to an improvement of the carrier lifetime by a factor of 2–3. Nevertheless, it is always necessary to use an optimized set of process parameters because otherwise the lifetime of all oxygen-contaminated materials (including gallium-doped Cz silicon) is severely reduced © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 2433-2439 
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    Topics: Physics
    Notes: We present experimental results for [1–3] magnetostrictive composites containing a 20% volume-fraction of Terfenol-D coarse particles ((very-much-greater-than)1 μm) suspended in a nonmetallic binder. Results from magnetostrictive strain and magnetoelastic measurements are provided for particle distributions that differ in particle size and range of size distribution. Particle size and packing density are shown to effect strain response and are attributed to demagnetization and loading (prestress) effects. Both a decreasing and increasing ΔE effect are measured for low and high fields, respectively, and found to be independent of particle distribution. The response of an optimized bimodal distribution increases packing density and produces 15% larger magnetostrictive strains than the other widely dispersed (polydispersed) (〈106, 〈212, and 〈300 μm) and narrowly dispersed (monodispersed) (〈45, 98, and 275 μm) distributions at comparable magnetic field levels. © 2001 American Institute of Physics.
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    Journal of Applied Physics 90 (2001), S. 2455-2458 
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    Source: AIP Digital Archive
    Topics: Physics
    Notes: In this study, the dielectric, magnetic, and transport properties of Gd0.33Sr0.67FeO3 have been analyzed. The temperature dependence of resistivity exhibits the adiabatic small polaron hopping conduction; i.e., ρ/T=A exp(E/kBT), E being the small polaron hopping energy. The dielectric loss anomaly was found to be around 170 K. The activation energy corresponding to the relaxation process of this dielectric anomaly was 0.16 eV. A dielectric relaxation process shows up with an activation energy nearly equal to that of dc conduction. The dielectric anomaly and resistivity of Gd0.33Sr0.67FeO3, which arises due to the presence of Fe4+ and Fe3+ ions, has been analyzed in the light of the small polaron hopping conduction mechanism. © 2001 American Institute of Physics.
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