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Rotating Superfluid 3He in Aerogel
Authors:M. Yamashita  A. Matsubara  R. Ishiguro  Y. Sasaki  O. Ishikawa  M. Kubota  Yu.M. Bunkov  T. Mizusaki
Affiliation:2. Department of Physics, Graduate School of Science, Kyoto University, Kyoto, 606-8502, Japan
4. Research Center for Low Temperature and Materials Sciences, Kyoto University, Kyoto, 606-8502, Japan
1. Institute for Solid State Physics, The University of Tokyo, Chiba, 277-8581, Japan
3. Graduate School of Science, Osaka City University, Osaka, 558-8585, Japan
5. CRTBT, MRS, BP 166, 38042, Grenoble Cedex 9, France
Abstract:
Rotational effects on textures of superfluid 3He in aerogel with 98% porosity at a pressure 3.0 MPa were investigated by cw-NMR measurement at 700 kHz (H 0=22 mT) under rotation up to 2π rad/s. At rest, the superfluidtransition to the A phase occurred at T aerogel c =2.07 mK and the A phase was supercooled down to T aerogel A→B==1.73~1.80 mK and became the B phase in the cooling process. In the warming process, the B phase was superheated up to T aerogel c . In the B phase, a new peak appeared in the NMR spectrum by rotating the sample. The intensity of this peak increased as the rotation speed increased almost linealy to Ω and started to be saturated for ΩΩ c. We attributed the new peak to the textural change caused by the counter flow and the onset of the saturation at Ω c to the onset of vortex nucleation in aerogel. On deceleration, the peak intensity decreased and disappeared at Ω=Ω v. Further decreasing Ω, the peak intensity increased even at Ω=0. The counterflow peak observed at Ω=0 indicates the existence of persistent current induced by pinned vortices in aerogel. In the A phase, we did not find any noticeable change in the NMR spectrum under the rotation speed up to 2π rad/s, or by cooling through T c with or without rotation. We concluded that the ${hat ell }$ texture in the A phase was strongly pinned to aerogel. No spin wave satellite signal localized at a soft, core vortex was observed in contrast to the bulk A phase.
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