747 research outputs found

    Investigation of ββ\beta\beta decay in 150^{150}Nd and 148^{148}Nd to the excited states of daughter nuclei

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    Double beta decay of 150^{150}Nd and 148^{148}Nd to the excited states of daughter nuclei have been studied using a 400 cm3^3 low-background HPGe detector and an external source consisting of 3046 g of natural Nd2_2O3_3 powder. The half-life for the two-neutrino double beta decay of 150^{150}Nd to the excited 01+^+_1 state in 150^{150}Sm is measured to be T1/2=[1.33−0.23+0.36(stat)−0.13+0.27(syst)]⋅1020T_{1/2}=[1.33^{+0.36}_{-0.23}(stat)^{+0.27}_{-0.13}(syst)]\cdot 10^{20} y. For other (0ν+2ν)(0\nu + 2\nu) transitions to the 21+^+_1, 22+^+_2, 23+^+_3, and 02+^+_2 levels in 150^{150}Sm, limits are obtained at the level of ∼(2−8)⋅1020\sim (2-8)\cdot 10^{20} y. In the case of 148^{148}Nd only limits for the (0ν+2ν)(0\nu + 2\nu) transitions to the 21+^+_1, 01+^+_1, and 22+^+_2 excited states in 148^{148}Sm were obtained and are at the level of \sim (4-8)\cdot 10^{20}$ y.Comment: 13 pages, 6 figure

    Search for β+\beta^+EC and ECEC processes in 112^{112}Sn

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    Limits on β+\beta^+EC (here EC denotes electron capture) and ECEC processes in 112^{112}Sn have been obtained using a 380 cm3^3 HPGe detector and an external source consisting of 53.355 g enriched tin (94.32% of 112^{112}Sn). A limit with 90% C.L. on the 112^{112}Sn half-life of 4.7×10204.7\times 10^{20} y for the ECEC(0ν\nu) transition to the 03+0^+_3 excited state in 112^{112}Cd (1871.0 keV) has been established. This transition is discussed in the context of a possible enhancement of the decay rate by several orders of magnitude given that the ECEC(0ν)(0\nu) process is nearly degenerate with an excited state in the daughter nuclide. Prospects for investigating such a process in future experiments are discussed. The limits on other β+\beta^+EC and ECEC processes in 112^{112}Sn were obtained on the level of (0.6−8.7)×1020(0.6-8.7)\times 10^{20} y at the 90% C.L.Comment: 14 pages, 4 figure

    Phase stability, ordering tendencies, and magnetism in single-phase fcc Au-Fe nanoalloys

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    Bulk Au-Fe alloys separate into Au-based fcc and Fe-based bcc phases, but L10_0 and L12_2 orderings were reported in single-phase Au-Fe nanoparticles. Motivated by these observations, we study the structural and ordering energetics in this alloy by combining density functional theory (DFT) calculations with effective Hamiltonian techniques: a cluster expansion with structural filters, and the configuration-dependent lattice deformation model. The phase separation tendency in Au-Fe persists even if the fcc-bcc decomposition is suppressed. The relative stability of disordered bcc and fcc phases observed in nanoparticles is reproduced, but the fully ordered L10_0 AuFe, L12_2 Au3_3Fe, and L12_2 AuFe3_3 structures are unstable in DFT. However, a tendency to form concentration waves at the corresponding [001] ordering vector is revealed in nearly-random alloys in a certain range of concentrations. This incipient ordering requires enrichment by Fe relative to the equiatomic composition, which may occur in the core of a nanoparticle due to the segregation of Au to the surface. Effects of magnetism on the chemical ordering are also discussed.Comment: 23 pages, 11 figure

    First test of an enriched 116^{116}CdWO4_4 scintillating bolometer for neutrinoless double-beta-decay searches

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    For the first time, a cadmium tungstate crystal scintillator enriched in 116^{116}Cd has been succesfully tested as a scintillating bolometer. The measurement was performed above ground at a temperature of 18 mK. The crystal mass was 34.5 g and the enrichment level ~82 %. Despite a substantial pile-up effect due to above-ground operation, the detector demonstrated a high energy resolution (2-7 keV FWHM in 0.2-2.6 MeV γ\gamma energy range), a powerful particle identification capability and a high level of internal radiopurity. These results prove that cadmium tungstate is an extremely promising detector material for a next-generation neutrinoless double-beta decay bolometric experiment, like that proposed in the CUPID project (CUORE Upgrade with Particle IDentification)

    Searches for neutrinoless double beta decay

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    Neutrinoless double beta decay is a lepton number violating process whose observation would also establish that neutrinos are their own anti-particles. There are many experimental efforts with a variety of techniques. Some (EXO, Kamland-Zen, GERDA phase I and CANDLES) started take data in 2011 and EXO has reported the first measurement of the half life for the double beta decay with two neutrinos of 136^{136}Xe. The sensitivities of the different proposals are reviewed.Comment: 8 pages, prepared for TAUP 201

    Double beta decay: present status

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    The present status of double beta decay experiments (including the search for 2β+2\beta^{+}, ECβ+\beta^{+} and ECEC processes) are reviewed. The results of the most sensitive experiments are discussed. Average and recommended half-life values for two-neutrino double beta decay are presented. Conservative upper limits on effective Majorana neutrino mass and the coupling constant of the Majoron to the neutrino are established as <0.75 < 0.75 eV and <gee><1.9⋅10−4<g_{ee} > < 1.9 \cdot 10^{-4}, respectively. Proposals for future double beta decay experiments with a sensitivity for the at the level of (0.01-0.1) eV are considered.Comment: 33 pages included 7 figures and 14 tables; an extended version of the invited talk at 13th Lomonosov Conference of Elementary Particle Physics, 23-29 August, 2007, Moscow, Russi

    Improvement of radiopurity level of enriched 116^{116}CdWO4_4 and ZnWO4_4 crystal scintillators by recrystallization

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    As low as possible radioactive contamination of a detector plays a crucial role to improve sensitivity of a double beta decay experiment. The radioactive contamination of a sample of 116^{116}CdWO4_4 crystal scintillator by thorium was reduced by a factor ≈10\approx 10, down to the level 0.01 mBq/kg (228^{228}Th), by exploiting the recrystallization procedure. The total alpha activity of uranium and thorium daughters was reduced by a factor ≈3\approx 3, down to 1.6 mBq/kg. No change in the specific activity (the total α\alpha activity and 228^{228}Th) was observed in a sample of ZnWO4_4 crystal produced by recrystallization after removing ≈0.4\approx 0.4 mm surface layer of the crystal.Comment: 14 pages, 5 figures and 2 table

    Searches for neutrinoless double beta decay

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    Neutrinoless double beta decay is a lepton number violating process whose observation would also establish that neutrinos are their own anti-particles. There are many experimental efforts with a variety of techniques. Some (EXO, Kamland-Zen, GERDA phase I and CANDLES) started take data in 2011 and EXO has reported the first measurement of the half life for the double beta decay with two neutrinos of 136^{136}Xe. The sensitivities of the different proposals are reviewed.Comment: 8 pages, prepared for TAUP 201
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