24,106 research outputs found

    Sm-Nd isotopic systematics of the ancient Gneiss complex, southern Africa

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    In order to shed some new light on the question of the absolute and relative ages of the Ancient Gneiss Complex and Onverwacht Group, a Sm-Nd whole-rock and mineral isochron study of the AGC was begun. At this point, the whole-rock study of samples from the Bimodal Suite selected from those studied for their geochemical characteristics by Hunter et al., is completed. These results and their implications for the chronologic evolution of the Kaapvaal craton and the sources of these ancient rocks are discussed

    New broad 8Be nuclear resonances

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    Energies, total and partial widths, and reduced width amplitudes of 8Be resonances up to an excitation energy of 26 MeV are extracted from a coupled channel analysis of experimental data. The presence of an extremely broad J^pi = 2^+ ``intruder'' resonance is confirmed, while a new 1^+ and very broad 4^+ resonance are discovered. A previously known 22 MeV 2^+ resonance is likely resolved into two resonances. The experimental J^pi T = 3^(+)? resonance at 22 MeV is determined to be 3^-0, and the experimental 1^-? (at 19 MeV) and 4^-? resonances to be isospin 0.Comment: 16 pages, LaTe

    Superconducting and normal-state properties of the noncentrosymmetric superconductor Re6Zr

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    We systematically investigate the normal and superconducting properties of non-centrosymmetric Re6_{6}Zr using magnetization, heat capacity, and electrical resistivity measurements. Resistivity measurements indicate Re6_{6}Zr has poor metallic behavior and is dominated by disorder. Re6_6Zr undergoes a superconducting transition at Tc=(6.75±0.05)T_{\mathrm{c}} = \left(6.75\pm0.05\right) K. Magnetization measurements give a lower critical field, μ0Hc1=(10.3±0.1)\mu_{0}H_{\mathrm{c1}} = \left(10.3 \pm 0.1\right) mT. The Werthamer-Helfand-Hohenberg model is used to approximate the upper critical field μ0Hc2=(11.2±0.2)\mu_{0}H_{\mathrm{c2}} = \left(11.2 \pm 0.2\right) T which is close to the Pauli limiting field of 12.35 T and which could indicate singlet-triplet mixing. However, low-temperature specific-heat data suggest that Re6_{6}Zr is an isotropic, fully gapped s-wave superconductor with enhanced electron-phonon coupling. Unusual flux pinning resulting in a peak effect is observed in the magnetization data, indicating an unconventional vortex state.Comment: 11 pages, 7 figures, 2 table

    Proteins of developing, mature and germinating seeds of phaseolus vulgaris

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    A number of methods have been used to extract, purify and characterise the major storage proteins of dry seeds of Phaseolus vulgaris L. cv. 'Seafarer'. Four fractions, which together account for the majority of the proteins solubilised by alkaline salt extractants and separated by pulyacrylamide gel electrophoresis, ' are described. The predominant protein, accounting for about 60% of the total protein content of the seed, is a vicilin-like protein, and is composed of two subunits, with molecular weights 50,000 and 47,000. A second protein fraction, prepared by zonal isoelectric precipitation, is a legumin-like protein; a third fraction was found to agglutinate erythrocytes. Amino acid compositions are presented for these protein fractions and their identity with storage proteins prepared in previous studies is discussed. The fourth fraction was not characterised. The protein content of protein bodies prepared by two methods was compared; the method of preparation was found to have a significant effect on the apparent distribution of both storage proteins and trypsin inhibitor activity. Variations in the distribution of storage proteins within the cotyledon are also described. The formation of storage protein during seed development and its subsequent mobilisation during seed germination was followed by SDS gel electrophoresis. Changes in proteolytic activity during germination were determined and attempts were made to identify the in vivo location of storage protein hydrolysis and the possible effect of endogenous inhibitors on this process

    Probing the superconducting ground state of the noncentrosymmetric superconductors CaTSi3 (T = Ir, Pt) using muon-spin relaxation and rotation

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    The superconducting properties of CaTSi3 (where T = Pt and Ir) have been investigated using muon spectroscopy. Our muon-spin relaxation results suggest that in both these superconductors time-reversal symmetry is preserved, while muon-spin rotation data show that the temperature dependence of the superfluid density is consistent with an isotropic s-wave gap. The magnetic penetration depths and upper critical fields determined from our transverse-field muon-spin rotation spectra are found to be 448(6) and 170(6) nm, and 3800(500) and 1700(300) G, for CaPtSi3 and CaIrSi3 respectively. The superconducting coherence lengths of the two materials have also been determined and are 29(2) nm for CaPtSi3 and 44(4) nm for CaIrSi3.Comment: 6 pages, 7 figure

    Time-reversal symmetry breaking in noncentrosymmetric superconductor Re6Hf:further evidence for unconventional behaviour in the alpha-Mn family of materials

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    The discovery of new families of unconventional superconductors is important both experimentally and theoretically, especially if it challenges current models and thinking. By using muon spin relaxation in zero-field, time-reversal symmetry breaking has been observed in Re6Hf. Moreover, the temperature dependence of the superfluid density exhibits s-wave superconductivity with an enhanced electron-phonon coupling. This, coupled with the results from isostructural Re6Zr, shows that the Re6X family are indeed a new and important group of unconventional superconductors.Comment: 5 pages, 2 figures Accepted Physical Review B, Rapid Communicatio

    TM digital image products for applications

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    Computer compatible tapes (CCTs) of LANDSAT 4 thematic mapper (TM) digital image products are compared and reviewed. The following tape formats are discussed: (1) raw band-sequential data (CCT-BT); (2) calibrated data (CCT-AT); and (3) geometrically resampled data (CCT-PT). Each format represents different steps in the process of producing fully corrected TM data. The CCT-BT images are uncorrected radiometrically or geometrically, CCT-AT data are radiometrically calibrated, and CCT-PT images are both radiometrically and geometrically corrected

    TM digital image products for applications

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    The image characteristics of digital data generated by LANDSAT 4 thematic mapper (TM) are discussed. Digital data from the TM resides in tape files at various stages of image processing. Within each image data file, the image lines are blocked by a factor of either 5 for a computer compatible tape CCT-BT, or 4 for a CCT-AT and CCT-PT; in each format, the image file has a different format. Nominal geometric corrections which provide proper geodetic relationships between different parts of the image are available only for the CCT-PT. It is concluded that detector 3 of band 5 on the TM does not respond; this channel of data needs replacement. The empty bin phenomenon in CCT-AT images results from integer truncations of mixed-mode arithmetric operations
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