anomalous local transport in microfabricatedsr 2 ruo 4 -ru eutectic junction

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Anomalous Local Anomalous Local Transport Transport in in Microfabricated Microfabricated Sr Sr 2 2 RuO RuO 4 4 -Ru -Ru Eutectic Junction Eutectic Junction 2009. 9. 4 NDSN2009@Nagoya Univ. AIST AIST Hiroshi Hiroshi Kambara Kambara Satoshi Satoshi Kashiwaya Kashiwaya Tokyo Univ of Sci. Hiroshi Yaguchi Hokkaido Univ. Yasuhiro Asano

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2009. 9. 4 NDSN2009@Nagoya Univ. Anomalous Local Transport in MicrofabricatedSr 2 RuO 4 -Ru Eutectic Junction. AIST Hiroshi Kambara Satoshi Kashiwaya Tokyo Univ of Sci. Hiroshi Yaguchi Hokkaido Univ.Yasuhiro Asano Nagoya Univ.Yukio Tanaka Kyoto Univ.Yoshiteru Maeno. - PowerPoint PPT Presentation

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  • Anomalous Local Transport in MicrofabricatedSr2RuO4-Ru Eutectic Junction

    2009. 9. 4 NDSN2009@Nagoya Univ.AISTHiroshi KambaraSatoshi Kashiwaya

    Tokyo Univ of Sci. Hiroshi YaguchiHokkaido Univ.Yasuhiro AsanoNagoya Univ.Yukio TanakaKyoto Univ.Yoshiteru Maeno

  • IntroductionHow is the local transport property?

    If chiral domain exists, how is the transport property affected?Sr2RuO4 (Tc=1.5 K)

    Chiral p-wave superconductor(spin-triplet pairing)Measurement of local transport characteristics of Sr2RuO4-Ru eutectic junction made by microfabrication.Observation of anomalous hysteresis in V-I

  • Sr2RuO4-Ru eutectic system ~3-K phase superconductivity~Sr2RuO4 Ru eutecticsMaeno et al., PRL 81, 3765 (1998).p-wave superconducting junction is naturally formed.

  • Extract a channel of Sr2RuO4-Ru junctionFocusing on the local superconducting channelby controlling the number of Ru-inclusionsKink structures appearafter FIB milling becauseonly a few channels are left.If microbridge is thin and narrow enough.

  • dV/dI-I characteristics Model of Josephson junctions in seriesTTc00Each channelS-S-SS-N-SIc0Ic1Ic2

  • Parity of the 3-K phasespsss0p03-K phase is also p-wave.( 1.5-K phase is p-wave.)ss00Monotonic increase of IcT > Tc0T < Tc0

  • Sample configuration (I // ab and I // c)

  • Anomalous hysteresis is observed for both I//ab and I//c direction.V-I & dV/dI-I characteristics (Anomalous hysteresis) I // ab

  • How are V-I characteristics anomalous?Anomalous features Voltage decreases at Isw. It switches to a lower Rn (normal resistance) branch with larger Ic.

    (3) Opposite hysteresis loop compared to typical Josephson junction (JJ) s.Sr2RuO4-Ru

  • Magnetic field effectcf) Hc1(0) 70 G (1.5-K phase) Deguchi, Mao, Maeno, JPSJ(2004). sample 1 NO influence of vortices !FCZFCNo change in the hysteresis between FC and ZFC.H // c

  • Possible origin of the hysteresis

  • Possible origin of the anomalous hysteresisdomain wall motion variation of cross section variation of IcRupx+ipypx-ipyRuinitial stateIcIcSfilament (parallel domain) NO hysteresis

    IcSDW (antiparallel domain) Hysteresis!(a) Inhomogeneous channel model

  • Possible origin of the anomalous hysteresis (b) 3-K phase+1.5-K phase coexistence model (kx or ky) (kxiky)(3) I = Isw Ic largerAssuming 3-K phase symmetry (kx) along the edge because of broken translational symmetry.

  • Questions for the chiral domain model

  • Summary of the anomalous hysteresis HysteresisInhomogeneous channelModel3-K + 1.5-K(kx) (kx+iky)VortexI // abI // c?No-magnetic field effectOK!probably OK?questioncontrarytotalMultiple switchChiral domainVortex origin is ruled out.

  • Local transport measurements have been done (I//ab, I//c) for Sr2RuO4-Ru eutectic samples made by FIB process. p-wave Josephson junctions are formed (3-K / 1.5-K / 3-K).

    Anomalous hysteresis was observed for both current directions. (voltage drop, opposite hysteresis loop) Chiral domain is a possible origin with (a) Inhomogeneous channel model or (b) 3-K phase+1.5-K phase model or others?

    Summary

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