6,630 research outputs found

    Single-crystal growth of the ternary BaFe2_2As2_2 phase using the vertical Bridgman technique

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    Ternary Ba-Fe-As system has been studied to determine a primary solidification field of the BaFe2_2As2_2 phase. We found that the BaFe2_2As2_2 phase most likely melts congruently and primarily solidifies either in the FeAs excess or Bax_{x}As100−x_{100-x} excess liquid. Knowing the primary solidification field, we have performed the vertical Bridgman growth using the starting liquid composition of Ba15_{15}Fe42.5_{42.5}As42.5_{42.5}. Large single crystals of the typical size 10x4x2 mm3^3 were obtained and their quality was confirmed by X-ray Laue and neutron diffraction.Comment: Submitted to Jpn. J. Appl. Phys.; revise

    Nonlinear magnetic susceptibility and aging phenomena in reentrant ferromagnet: Cu0.2_{0.2}Co0.8_{0.8}Cl2_{2}-FeCl3_{3} graphite bi-intercalation compound

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    Linear and nonlinear dynamic properties of a reentrant ferromagnet Cu0.2_{0.2}Co0.8_{0.8}Cl2_{2}-FeCl3_{3} graphite bi-intercalation compound are studied using AC and DC magnetic susceptibility. This compound undergoes successive phase transitions at the transition temperatures ThT_{h} (= 16 K), TcT_{c} (= 9.7 K), and TRSGT_{RSG} (= 3.5 K). The static and dynamic behaviors of the reentrant spin glass phase below TRSGT_{RSG} are characterized by those of normal spin glass phase with critical exponent β\beta = 0.57 ±\pm 0.10, a dynamic critical exponent xx = 8.5 ±\pm 1.8, and an exponent pp (= 1.55 ±\pm 0.13) for the de Almeida -Thouless line. A prominent nonlinear susceptibility is observed between TRSGT_{RSG} and TcT_{c} and around ThT_{h}, suggesting a chaotic nature of the ferromagnetic phase (TRSG≤T≤TcT_{RSG} \leq T \leq T_{c}) and the helical spin ordered phase (Tc≤T≤ThT_{c} \leq T \leq T_{h}). The aging phenomena are observed both in the RSG and FM phases, with the same qualitative features as in normal spin glasses. The aging of zero-field cooled magnetization indicates a drastic change of relaxation mechanism below and above TRSGT_{RSG}. The time dependence of the absorption χ′′\chi^{\prime \prime} is described by a power law form (≈t−b′′\approx t^{-b^{\prime \prime}}) in the ferromagnetic phase, where b′′≈0.074±0.016b^{\prime \prime} \approx 0.074 \pm 0.016 at ff = 0.05 Hz and TT = 7 K. No ωt\omega t-scaling law for χ′′\chi^{\prime \prime} [≈(ωt)−b′′\approx (\omega t)^{-b^{\prime \prime}}] is observed.Comment: 14 pages, 16 figures, and 2 table

    ΛN\Lambda N correlations from the stopped K−K^- reaction on 4{}^4He

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    We have investigated correlations of coincident ΛN\Lambda N pairs from the stopped K−K^- reaction on 4{}^4He, and clearly observed Λp\Lambda p and Λn\Lambda n branches of the two-nucleon absorption process in the ΛN\Lambda N invariant mass spectra. In addition, non-mesonic reaction channels, which indicate possible exotic signals for the formation of strange multibaryon states, have been identified.Comment: 5 pages, 3 figures, submitted to Physical Review Letter

    Kondo Effects and Multipolar Order in the cubic PrTr2Al20 (Tr=Ti, V)

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    Our single crystal study reveals that PrTr2Al20 (Tr = Ti and V) provides the first examples of a cubic {\Gamma}3 nonmagnetic ground doublet system that shows the Kondo effect including a -ln T dependent resistivity. The {\Gamma}3 quadrupolar moments in PrV2Al20 induce anomalous metallic behavior through hybridization with conduction electrons, such as T^{1/2} dependent resistivity and susceptibility below ~ 20 K down to its ordering temperature T_O = 0.6 K. In PrTi2Al20, however, quadrupoles are well-localized and exhibit an order at T_O = 2.0 K. Stronger Kondo coupling in PrV2Al20 than in PrTi2Al20 suppresses quadrupolar ordering, and instead promotes hybridization between the {\Gamma}3 doublet and conduction electrons, leading to most likely the quadrupolar Kondo effect.Comment: 12 pages, 4 figure

    The (K-,p) reaction on nuclei with in-flight kaons

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    We perform a theoretical study of the spectrum of protons with kinetic energies of around 600 MeV, emitted following the interaction of 1 GeV/c kaons with nuclei. A recent experimental analysis of this (K-,p) reaction on 12C, based on the dominant quasielastic process, has suggested a deeply attractive kaon nucleus potential. Our Monte Carlo simulation considers, in addition, the one-and two-nucleon K- absorption processes producing hyperons that decay into \pi N pairs. We find that this kaon in-flight reaction is not well suited to determine the kaon optical potential due, essentially, to the limited sensitivity of the cross section to its strength, but also to unavoidable uncertainties from the coincidence requirement applied in the experiment. A shallow kaon nucleus optical potential obtained in chiral models is perfectly compatible with the observed spectrum.Comment: To appear in the proceedings of the 10th International Conference on Hypernuclear and Strange Particle Physics, Tokai, Ibaraki (Japan), 14-18 September, 200

    Absolute Energy Calibration of X-ray TESs with 0.04 eV Uncertainty at 6.4 keV in a Hadron-Beam Environment

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    A performance evaluation of superconducting transition-edge sensors (TESs) in the environment of a pion beam line at a particle accelerator is presented. Averaged across the 209 functioning sensors in the array, the achieved energy resolution is 5.2 eV FWHM at Co KαK_{\alpha} (6.9 keV) when the pion beam is off and 7.3 eV at a beam rate of 1.45 MHz. Absolute energy uncertainty of ±\pm0.04 eV is demonstrated for Fe KαK_{\alpha} (6.4 keV) with in-situ energy calibration obtained from other nearby known x-ray lines. To achieve this small uncertainty, it is essential to consider the non-Gaussian energy response of the TESs and thermal cross-talk pile-up effects due to charged-particle hits in the silicon substrate of the TES array.Comment: Accepted for publication in J. Low Temperature Physics, special issue for the proceedings of the Low Temperature Detectors 16 conferenc

    Signals for strange quark contributions to the neutrino (antineutrino) scattering in quasi-elastic region

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    Strange quark contributions to the neutrino (antineutrino) scattering are investigated on the elastic neutrino-nucleon scattering and the neutrino-nucleus scattering for 12C target in the quasi-elastic region on the incident energy of 500 MeV, within the framework of a relativistic single particle model. For the neutrino-nucleus scattering, the effects of final state interaction for the knocked-out nucleon are included by a relativistic optical potential. In the cross sections we found some cancellations of the strange quark contributions between the knocked-out protons and neutrons. Consequently, the asymmetries between the incident neutrino and antineutrino which is the ratio of neutral current to charged current, and the difference between the asymmetries are shown to be able to yield more feasible quantities for the strangeness effects. In order to explicitly display importance of the cancellations, results of the exclusive reaction 16O(\nu, \nu' p) are additionally presented for detecting the strangeness effects.Comment: 14 pages, 8 figures, submitted to Phys. Lett.

    The BAT-Swift Science Software

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    The BAT instrument tells the Swift satellite where to point to make immediate follow-up observations of GRBs. The science software on board must efficiently process gamma-ray events coming in at up to 34 kHz, identify rate increases that could be due to GRBs while disregarding those from known sources, and produce images to accurately and rapidly locate new Gamma-ray sources.Comment: 4 pages, no figures, to appear in Santa Fe proceedings "Gamma-Ray Bursts: 30 Years of Discovery", Fenimore and Galassi (eds), AIP, 200
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