5 research outputs found

    Peak effect in single crystal MgB2_2 superconductor for H∥c{\bf H}\parallel c-axis

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    We have studied the phase diagram of MgB2_2 superconductor using a single crystal for H∥c{\bf H}\parallel c-axis. For the first time we report the existence of peak effect in the screening current in MgB2_{2} single crystal for H∥c{\bf H}\parallel c-axis. In the magnetic field regime 10<H<13.510<H<13.5 kOe the local fundamental diamagnetic moment displays a very narrow diamagnetic step, with a temperature width of the same size as the zero dc-magnetic field transition. For higher field this step is transformed to a peak which is related with the peak effect in the screening current. Finally, for H<10H<10 kOe the diamagnetic step is transformed to a gradual transition. Our findings for the vortex matter phase diagram for the MgB2_2 are closely related with theoretical predictions concerning the vortex matter phase diagram of a type II superconductor in the presence of weak point disorder.Comment: Has been submitted for publication in PRL since 21 February 200

    Hysteretic behavior of the vortex lattice at the onset of the second peak for HgBa2_2CuO4+δ_{4+\delta} superconductor

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    By means of local Hall probe ac and dc permeability measurements we investigated the phase diagram of vortex matter for the HgBa2_2CuO4+δ_{4+\delta } superconductor in the regime near the critical temperature. The second peak line, HspH_{\rm sp}, in contrast to what is usually assumed, doesn't terminate at the critical temperature. Our local ac permeability measurements revealed pronounced hysteretic behavior and thermomagnetic history effects near the onset of the second peak, giving evidence for a phase transition of vortex matter from an ordered qausilattice state to a disordered glass

    Anomalous Peak Effect in CeRu2 and NbSe2 : Fracturing of a Flux Line Lattice?

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    CeRu2 and 2H-NbSe2 display remarkable similarities in their magnetic response, reflecting the manner in which the weakly pinned flux line lattice (FLL) loses spatial order in the Peak Effect (PE) regime. The discontinuous change in screening response near the onset of PE and the history dependence in it are attributed to a disorder-induced fracturing transition of the FLL, as an alternative to the scenario involving the appearance of a spatial modulation in superconducting order parameter in CeRu2.Comment: 4 pages of text and figures in ps for
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