115 research outputs found

    Influence of carbon and nitrogen on electronic structure and hyperfine interactions in fcc iron-based alloys

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    Carbon and nitrogen austenites, modeled by Fe8N and Fe8C superstructures are studied by full-potential LAPW method. Structure parameters, electronic and magnetic properties as well as hyperfine interaction parameters are obtained. Calculations prove that Fe-C austenite can be successfully modeled by ordered Fe8C superstructure. The results show that chemical Fe-C bond in Fe8C has higher covalent part than in Fe8N. Detailed analysis of electric field gradient formation for both systems is performed. The calculation of electric field gradient allow us to carry out a good interpretation of Moessbauer spectra for Fe-C and Fe-N systems.Comment: 8 pages, 3 figures, IOP-style LaTeX, submitted to J. Phys. Condens. Matte

    A self-organized synthetic morphogenic liposome responds with shape changes to local light cues

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    Reconstituting artificial proto-cells capable of transducing extracellular signals into cytoskeletal changes can reveal fundamental principles of how non-equilibrium phenomena in cellular signal transduction affect morphogenesis. Here, we generated a Synthetic Morphogenic Membrane System (SynMMS) by encapsulating a dynamic microtubule (MT) aster and a light-inducible signaling system driven by GTP/ATP chemical potential into cell-sized liposomes. Responding to light cues in analogy to morphogens, this biomimetic design embodies basic principles of localized Rho-GTPase signal transduction that generate an intracellular MT-regulator signaling gradient. Light-induced signaling promotes membrane-deforming growth of MT-filaments by dynamically elevating the membrane-proximal tubulin concentration. The resulting membrane deformations enable recursive coupling of the MT-aster with the signaling system, which generates global self-organized morphologies that reorganize towards local external cues in dependence on prior shape. SynMMS thereby signifies a step towards bio-inspired engineering of self-organized cellular morphogenesis

    COBRA - Double beta decay searches using CdTe detectors

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    A new approach (called COBRA) for investigating double beta decay using CdTe (CdZnTe) semiconductor detectors is proposed. It follows the idea that source and detector are identical. This will allow simultaneous measurements of 5 ÎČ−ÎČ−\beta^-\beta^- - and 4 ÎČ+ÎČ+\beta^+\beta^+ - emitters at once. Half-life limits for neutrinoless double beta decay of Cd-116 and Te-130 can be improved by more than one order of magnitude with respect to current limits and sensitivities on the effective Majorana neutrino mass of less than 1 eV can be obtained. Furthermore, for the first time a realistic chance of observing double electron capture processes exists. Additional searches for rare processes like the 4-fold forbidden Cd-113 ÎČ\beta-decay, the electron capture of Te-123 and dark matter detection can be performed. The achievable limits are evaluated for 10 kg of such detectors and can be scaled accordingly towards higher detector masses because of the modular design of the proposed experiment.Comment: 13 pages, 3 eps-figures, submitte

    Complementary use of TEM and APT for the investigation of steels nanostructured by severe plastic deformation

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    The properties of bulk nanostructured materials are often controlled by atomic scale features like segregation along defects or composition gradients. Here we discuss about the complimentary use of TEM and APT to obtain a full description of nanostructures. The advantages and limitations of both techniques are highlighted on the basis of experimental data collected in severely deformed steels with a special emphasis on carbon spatial distribution

    Nuclear deformation and the two neutrino double-\beta decay in ^{124,126}Xe,^{128,130}Te, ^{130,132}Ba and ^{150}Nd isotopes

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    The two neutrino double beta decay of 124,126^{124,126}Xe,128,130^{128,130}Te, 130,132 ^{130,132}Ba and 150^{150}Nd isotopes is studied in the Projected Hartree-Fock-Bogoliubov (PHFB) model. Theoretical 2Îœ\nu ÎČ−ÎČ−\beta^{-}\beta ^{-} half-lives of 128,130^{128,130}Te, and 150^{150}Nd isotopes, and 2ÎœÎČ+ÎČ+\nu \beta^{+}\beta^{+}, 2Îœ\nu ÎČ+EC\beta^{+}EC and 2Îœ\nu ECECECEC for 124,126 ^{124,126}Xe and 130,132^{130,132}Ba nuclei are presented. Calculated quadrupolar transition probabilities B(E2: 0+→2+0^+\to 2^+), static quadrupole moments and gg factors in the parent and daughter nuclei reproduce the experimental information, validating the reliability of the model wave functions. The anticorrelation between nuclear deformation and the nuclear transition matrix element M2ÎœM_{2\nu} is confirmed.Comment: 19 page

    First Results from the AMoRE-Pilot neutrinoless double beta decay experiment

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    The Advanced Molybdenum-based Rare process Experiment (AMoRE) aims to search for neutrinoless double beta decay (0ÎœÎČÎČ\nu\beta\beta) of 100^{100}Mo with ∌\sim100 kg of 100^{100}Mo-enriched molybdenum embedded in cryogenic detectors with a dual heat and light readout. At the current, pilot stage of the AMoRE project we employ six calcium molybdate crystals with a total mass of 1.9 kg, produced from 48^{48}Ca-depleted calcium and 100^{100}Mo-enriched molybdenum (48depl^{48\textrm{depl}}Ca100^{100}MoO4_4). The simultaneous detection of heat(phonon) and scintillation (photon) signals is realized with high resolution metallic magnetic calorimeter sensors that operate at milli-Kelvin temperatures. This stage of the project is carried out in the Yangyang underground laboratory at a depth of 700 m. We report first results from the AMoRE-Pilot 0ÎœÎČÎČ0\nu\beta\beta search with a 111 kg⋅\cdotd live exposure of 48depl^{48\textrm{depl}}Ca100^{100}MoO4_4 crystals. No evidence for 0ÎœÎČÎČ0\nu\beta\beta decay of 100^{100}Mo is found, and a upper limit is set for the half-life of 0ÎœÎČÎČ\nu\beta\beta of 100^{100}Mo of T1/20Îœ>9.5×1022T^{0\nu}_{1/2} > 9.5\times10^{22} y at 90% C.L.. This limit corresponds to an effective Majorana neutrino mass limit in the range ⟹mÎČÎČ⟩≀(1.2−2.1)\langle m_{\beta\beta}\rangle\le(1.2-2.1) eV
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