Static and fluctuating magnetic moments in the ferroelectric metal LiOsO3
JPS Conference Proceedings Physical Society of Japan 日本物理学会 21:011013 (2018) 1-6
Abstract:
LiOsO3 is the first example of a new class of material called a ferroelectric metal. We performed zero-field and longitudinal-field μSR, along with a combination of electronic structure and dipole field calculations, to determine the magneticground state of LiOsO3. We find that the sample contains both static Li nuclear moments and dynamic Os electronic moments. Below ≈0.7 K, the fluctuations of the Os moments slow down, though remain dynamic down to 0.08 K. We expect this could result in a frozen-out, disordered ground state at even lower temperatures.Nodal multigap superconductivity in KCa2Fe4As4F2
PHYSICAL REVIEW B 97:6 (2018) 060509(R)
Two-gap superconductivity with line nodes in CsCa2Fe4As4F2
Physical Review B American Physical Society 97:6 (2018) 060506(R)
Abstract:
We report the results of a muon-spin rotation ($\mu$SR) experiment to determine the superconducting ground state of the iron-based superconductor $CsCa_2Fe_4As_4F_2$ with $T_{\rm c} \approx 28.3\,K$. This compound is related to the fully-gapped superconductor $CaCsFe_4As_4$, but here the Ca-containing spacer layer is replaced with one containing $Ca_2F_2$. The temperature evolution of the penetration depth strongly suggests the presence of line nodes and is best modelled by a system consisting of both an $s-$ and a $d-$wave gap. We also find a potentially magnetic phase which appears below $\approx 10\,K$ but does not appear to compete with the superconductivity. This compound contains the largest alkali atom in this family of superconductors and our results yield a value for the in-plane penetration depth of $\lambda_{ab}(T=0)=423(5)\,nm$.Multigap superconductivity in RbCa2Fe4As4F2 investigated using muSR measurements
(2018)
Extreme sensitivity of a topochemical reaction to cation substitution: SrVO2H versus SrV1-xTixO1.5H1.5
Inorganic Chemistry American Chemical Society 57:5 (2018) 2890-2898