116 research outputs found

    Pressure-Induced Antiferromagnetic Bulk Superconductor EuFe2_2As2_2

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    We present the magnetic and superconducting phase diagram of EuFe2_2As2_2 for BcB \parallel c and BabB \parallel ab. The antiferromagnetic phase of the Eu2+^{2+} moments is completely enclosed in the superconducting phase. The upper critical field vs. temperature curves exhibit strong concave curvatures, which can be explained by the Jaccarino-Peter compensation effect due to the antiferromagnetic exchange interaction between the Eu2+^{2+} moments and conduction electrons.Comment: submitted to the proceedings of the M2S-IX Toky

    Cyclotron resonance and mass enhancement by electron correlation in KFe2_2As2_2

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    Cyclotron resonance (CR) measurements for the Fe-based superconductor KFe2_2As2_2 are performed. One signal for CR is observed, and is attributed to the two-dimensional α\alpha Fermi surface at the Γ\Gamma point. We found a large discrepancy in the effective masses of CR [(3.4±\pm0.05)mem_e (mem_e is the free electron mass)] and de-Haas van Alphen (dHvA) results, a direct evidence of mass enhancement due to electronic correlation. A comparison of the CR and dHvA results shows that both intra- and interband electronic correlations contribute to the mass enhancement in KFe2_2As2_2.Comment: 5 pages, 4 figure

    Physical properties of the Dome Fuji deep ice core (review)

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    Recent results of physical analyses of the Dome Fuji ice core are summarized with special attention to new methods introduced in the present studies. Microphysical processes which affect the ice core records are reviewed to better understand the paleoclimatic and paleoenvironmental signals stored

    The 2006 November outburst of EG Aquarii: the SU UMa nature revealed

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    We report time-resolved CCD photometry of the cataclysmic variable EG Aquarii during the 2006 November outburst During the outburst, superhumps were unambiguously detected with a mean period of 0.078828(6) days, firstly classifying the object as an SU UMa-type dwarf nova. It also turned out that the outburst contained a precursor. At the end of the precursor, immature profiles of humps were observed. By a phase analysis of these humps, we interpreted the features as superhumps. This is the second example that the superhumps were shown during a precursor. Near the maximum stage of the outburst, we discovered an abrupt shift of the superhump period by {\sim} 0.002 days. After the supermaximum, the superhump period decreased at the rate of P˙/P\dot{P}/P=8.2×105-8.2{\times}10^{-5}, which is typical for SU UMa-type dwarf novae. Although the outburst light curve was characteristic of SU UMa-type dwarf novae, long-term monitoring of the variable shows no outbursts over the past decade. We note on the basic properties of long period and inactive SU UMa-type dwarf novae.Comment: 9 pages, 7 figures, accepted for PAS
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