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<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant="normal">He</mml:mi></mml:mrow><mml:mprescripts/><mml:mrow/><mml:mrow><mml:mn>3</mml:mn></mml:mrow><mml:mrow/><mml:mrow/></mml:mmultiscripts></mml:mrow></mml:math>melting curve below 15 mK

Hiroshi FukuyamaInstitute for Solid State Physics, University of Tokyo, Roppongi, Tokyo 106, JapanHidehiko IshimotoInstitute for Solid State Physics, University of Tokyo, Roppongi, Tokyo 106, JapanTetsurou TazakiInstitute for Solid State Physics, University of Tokyo, Roppongi, Tokyo 106, JapanShinji OgawaInstitute for Solid State Physics, University of Tokyo, Roppongi, Tokyo 106, Japan
1987lv
ABI

Annotatsiya

We have performed new measurements of the $P\ensuremath{-}T$ relation along the $^{3}\mathrm{He}$ melting curve for temperatures between 0.4 and 15 mK in zero magnetic field. The temperature was determined by a Pt-wire nuclear-magnetic-resonance thermometer calibrated against the National Bureau of Standards scale (1983) above 15 mK. Three distinct points on the melting curve (the two superfluid transitions and the nuclear-spin ordering in the solid phase) were observed at temperatures lower than the currently accepted values by about 10%. Our results are in good agreement with the $P\ensuremath{-}T$ relation recently proposed by Greywall using a La-cerium magnesium nitrate thermometer, but differ seriously from the thermodynamic measurements by Halperin et al. From the measured melting curve, we could determine the ground-state energy of a nuclear spin in solid $^{3}\mathrm{He}$ to be -1.24 mK at the melting density. This value can be quantitatively explained by the current four-spin exchange theory.

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