物理
μ介子自旋谱学
凝聚态物理
量子涨落
塞曼效应
量子相变
μ介子
拉莫尔进动
顺磁性
反铁磁性
量子临界点
自旋(空气动力学)
磁场
量子
相变
量子力学
超导电性
热力学
作者
M. Pregelj,Zurab Guguchia,Marie-Cécile de Weerd,Pascal Boulet,S. Vrtnik,J. Dolinšek
标识
DOI:10.1038/s41598-022-17298-6
摘要
We report on the dynamics of a magnetic-field-driven antiferromagnetic-to-paramagnetic quantum phase transition in monocrystalline Ce3Al via transverse-field muon spin rotation (TF-µSR) experiments down to low temperature of [Formula: see text] 80 mK. The quantum phase transition is of a spin-flip type and takes place on the Ce-Al magnetic chains as a result of competition between the indirect exchange and the Zeeman interaction of the Ce moments with the external field, applied along the chain direction (also the direction of the antiferromagnetic axis). The Ce moments are not static at [Formula: see text] 0, but fluctuate in their direction due to the Heisenberg uncertainty principle. Upon applying the magnetic field sweep, the fluctuations exhibit the largest amplitude at the quantum critical point, manifested in a maximum of the muon transverse relaxation rate at the critical field. The quantum nature of fluctuations observed in the TF-µSR experiments is reflected in the temperature independence of the average local magnetic field component along the external magnetic field at the muon stopping site(s) and the muon transverse relaxation rate within the investigated temperature range 1.5 K-80 mK. Quantum fluctuations are fast on the muon Larmor frequency scale, [Formula: see text] 10-10 s.
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