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  • 1
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The local atomic environment of the Sb dopant in 2 and 5×1016 ions/cm2 implanted Si samples has been studied by near grazing incidence fluorescence extended x-ray absorption fine structure at different stages of the Sb deactivation process. The annealings were performed at high temperature (900–1000 °C) during various periods: 30 s–4 h. The Sb out-diffusion and the high percentage of Sb precipitates are put into evidence especially for Sb-only implanted samples. The comparison of the Sb and B codiffusion data with the corresponding ones obtained by the diffusion of Sb alone revealed several anomalous effects due to dopant interaction. Moreover, a simulation program including dopant precipitation and donor–acceptor pairing allows us to foresee most of the anomalous phenomena occurring in high-concentration codiffusion experiments. © 1996 American Institute of Physics.
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  • 2
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 75 (1994), S. 126-133 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Backscattering and ion channeling measurements have been carried out on 〈100〉 silicon wafers implanted with a dose of 3×1016 As+/cm2. These samples have been submitted to laser annealing and then to various thermal annealings in the 350–1000 °C temperature range. Three different crystallographic directions, 〈100〉, 〈110〉, and 〈111〉, have been explored. The deactivated As atom displacement with respect to the lattice sites has occurred already by the first stage of electrical deactivation at 350 °C. The average displacement is constant in the considered temperature range and has been found equal to 0.23±0.06 A(ring) making an angle of 23±8° with the [100] direction. By comparing this finding with the local atomic As arrangement, deduced from previously reported extended x-ray absorption fine structure measurements performed on the same samples, new cluster models are presented. These models consist of As2V and As4V clusters during the very early stage of deactivation, and of several As4V clusters grouped together giving rise to larger AsmVn agglomerates (m up to 12 and n up to 5). In this context, the average As displacement mainly results from the combined displacements of As atoms inside the clusters. The thermal evolution of the As agglomerates at higher temperatures is also discussed.
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  • 3
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Magnetic resonance spectra of iron and manganese in black obsidians from Teotihuacan (Central Mexico) were investigated at 9 GHz (X band) and 35 GHz (Q band). The specimens were found to be magnetically very heterogeneous. The X band spectrum exhibited, at g=4.28, the classical paramagnetic signal of isolated high spin Fe(III) ions. At g=2.0 a ferromagnetic resonance occured, associated with magnetite-like particles previously characterized by Mössbauer spectroscopy. At Q band there are two signals, a superparamagnetic signal at g=2.00 and a weak hyperfine sextet, superimposed on the g(approximately-equal-to)2.00 signal, attributed to isolated Mn(II) free ions. At X band a strong grain-size dependence of the overall line shape was also observed. The temperature, frequency, and grain-size dependence of the spectral lines of these natural glasses indicate, in addition to isolated high spin Fe(III) and Mn(II) ions, the presence of superparamagnetic clusters of magnetite and a range order, in these obsidians, larger than the common short-range order of the glassy state.
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  • 4
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Magnetic resonance spectra of Fe3+ and Mn2+ ions in natural volcanic glasses, black obsidians from Lipari (Island of Southern Italy), have been investigated at 9 (X band) and 35 GHz (Q band). The spectrum in the X band is found to exhibit at g=4.3 the classical signal of isolated Fe3+ ions.1 At g=2 it is found the superposition of a superparamagnetic signal and a ferromagnetic resonance arising from the small and not so small magnetite particles previously found.2 It was also observed at X band a granular dependence of the g=2 line shape, similar to that observed in polycrystalline powders. At Q band there were two signals, one due to iron clusters at g=2 and a weak hyperfine sextet attributed to Mn2+ free ions. The magnetization for a given temperature (from 1.75 to 20 K) and very high magnetic fields (up to 150 kOe) shows the lack of hysteresis loops and the absence of remanent magnetization, both indicative of superparamagnetism. However, the magnetization curves do not superpose to a Langevin function L[M(H/T)], which reflects the presence of inhomogeneous ferrimagnetic magnetite particles.〈ks〉
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  • 5
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 61 (1987), S. 3565-3567 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We have studied by 57Fe Mössbauer spectroscopy and low field magnetization on oriented powders the temperature and hydrogen dependence of the magnetic structure of R2Fe14B compounds with R=Dy, Ho, and Y. We show that the iron sublattice may be canted by an angle (approximately-equal-to)15° at high temperature. Hydrogen increases this canting at low temperature. It increases the spin reorientation temperature measured by bulk magnetization for Ho2Fe14B and induces a spin reorientation in the Dy alloys. These effects show that the strength of the crystal field terms of fourth (and maybe sixth) order compared to the terms of second order is increased by hydrogen.
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  • 6
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Laser-annealed and further thermally annealed arsenic implanted silicon specimens have been investigated in a range of doses from 1×1016 to 5×1016 As/cm2, with different experimental techniques: electrical measurements, transmission electron microscopy (TEM), double-crystal x-ray diffractometry (DCD), and extended x-ray absorption fine structure analysis (EXAFS). On the as laser-annealed samples, in the whole range of doses examined, a lattice contraction of the doped layer has been evidenced by DCD, whereas, on the same specimens, EXAFS measurements have shown the presence of a local expansion around substitutional As atoms. The relationship between strain and carrier concentration has been found to be approximately linear and can be described by the presence of a size and an electronic effect, as recently proposed in the literature. The former effect represents the atomic size contribution, while the latter is the strain induced by the variation of the conduction-band minima due to the doping. After a subsequent thermal annealing in a low-temperature range (350–550 °C), a strong deactivation of the dopant has been evidenced by electrical measurements. From the experimental results, a new model of the first step of the As deactivation phenomenon at low temperature is proposed. It is described by the capture of two electrons from a pair of As atoms in the second neighbor position in the Si lattice, leading to the formation of a positively charged arsenic-vacancy cluster (As2V)+, and to the emission of a negatively charged Si self-interstitial I−. This model takes into account the main phenomena that are experimentally observed simultaneously to the As deactivation, i.e., the transition from a contraction to a dilatation of the strain observed by DCD and the formation of interstitial loops. At relatively high temperatures (650–900 °C), the hypothesis of the coexistence of the clusters and of the observed precipitates has to be taken into account in order to explain the nature of the inactive As. However, whether clustering or precipitation is the dominant phenomenon still remains an open question.
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  • 7
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 61 (1992), S. 264-266 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The electrical deactivation of Sb atoms highly implanted (2 and 5×1016 ions/cm2) in crystalline silicon is studied by the extended x-ray absorption fine structure (EXAFS) method. By following the evolution of the local atomic environment around the Sb atoms it is shown that the description of the deactivation process must take into account the existence of vacancy complexes, SbV2, in addition to the usual antimony rhombohedric precipitates. These vacancy complexes are already present after laser annealing in the 5×1016 ions/cm2 case. Co-implantation with boron delays the precipitation of Sb particles, by forming new complexes, SbBV or SbB2, with a Sb atom surrounded by two sites (B and/or vacancy).
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  • 8
    Electronic Resource
    Electronic Resource
    Amsterdam : Elsevier
    Solid State Communications 57 (1986), S. 499-504 
    ISSN: 0038-1098
    Source: Elsevier Journal Backfiles on ScienceDirect 1907 - 2002
    Topics: Physics
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 31 (1998), S. 783-788 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: The structural evolution of co-sputtered Ag–20 (and 35) at.% Co and Ag–20 (and 35) at.% Ni was studied by anomalous small-angle X-ray scattering in the as-deposited state and after different anneals for 10 min at 573, 623 and 723 K. Anomalous scattering was used to separate the part of the scattering signal due to the transition metal particles from the signal of other heterogeneities. Strong segregation, involving about two-thirds of the Co (or Ni) atoms, already exists for the as-deposited state. After a 573 K anneal, the phases (Ag matrix and Co or Ni well defined particles) have almost reached equilibrium, i.e. complete immiscibility. Most of the magnetic particles are three dimensional with an average radius of 5–25 Å and the average distance between the particles varies from 17 to 110 Å, depending on the magnetic element and its concentration, and on the annealing conditions. The size distribution does not correspond to that of usual coarsening, but becomes broader after extended annealing. This is probably due to heterogeneous precipitation at grain boundaries of the Ag matrix.
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  • 10
    Electronic Resource
    Electronic Resource
    Springer
    Physics and chemistry of minerals 12 (1985), S. 246-254 
    ISSN: 1432-2021
    Source: Springer Online Journal Archives 1860-2000
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: Abstract We report in the present paper the main results concerning the evolution of the structural, magnetic and hyperfine properties of natural and synthetic wolframites Fe x Mn1−x WO4 in the composition range 0.16〈x〈1. The iron and the manganese content of the samples are obtained by atomic absorption spectrophotometry. The lattice parameters are determined from least-squares fits of the X-ray diffraction data. Mössbauer experiments have been carried out between 200 and 4.2 K. Their parameters can be attributed to a high spin ferrous ion in a quite distorted octahedral symmetry. From the magnetic spectra, we deduce a very weak value for the magnetic hyperfine field (≃50 kG), a negative sign for the quadrupole interaction and an asymmetry parameter η different from zero for x〉0.3 ( $$\bar \eta$$ ≃0.7). In addition we discuss the variation of the magnitude of H hf and of the angle ϑ between the H hf direction and the principal axis of the electric field gradient (EFG) V zz with the iron content. A single crystal Mössbauer study has also been performed to determine the orientation of the principal axis of the EFG and of the H hf direction relative to the crystallographic axes. Mössbauer spectroscopy and magnetic susceptibility techniques have been used to obtain the magnetic ordering temperature T N. One finds a linear variation of T N with x for 0.4〈x〈1 and a deviation from the linear behavior for 0.16〈x〈0.3. These results are discussed in terms of the contributions of the different Fe-Fe, Fe-Mn and Mn-Mn exchange interactions.
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