Microscopic evidence for long-range magnetic ordering in the 
ground quartet systems Sm
Al
(
: Ti, V, Cr)
基底Sm
Al
(
: Ti, V, Cr)における長距離磁気秩序の微視的証拠
伊藤 孝
; 髭本 亘
; 二宮 和彦; 酒井 明人*; 中辻 知*
Ito, Takashi; Higemoto, Wataru; Ninomiya, Kazuhiko; Sakai, Akito*; Nakatsuji, Satoru*
f電子系化合物
Al
(
: Pr, Sm,
: Ti, V, Cr)は特異な籠状構造に起因する興味深い物性を示す。
イオンは16個ものAl原子からなる「籠」に内包されており、
サイトには対称性の高い結晶場が生じる。これにより多極子自由度が活性な結晶場基底が形成され、低温において多極子秩序が生じる。一方、多数のAl原子が
イオンに配位することにより、顕著な
混成が生じる。
混成の度合いは
元素の置換によってチューン可能であることから、多極子秩序に関する量子臨界性の系統的研究が可能な系として注目を集めている。本研究では、上述の議論の前提となっている多極子秩序を微視的な観点から検証するために、PrTi
Al
及びSm
Al
(
: Ti, V, Cr)に対して
SR測定を行った。その結果、PrTi
Al
及びSm
Al
(
: Ti, V, Cr)の秩序変数が、それぞれ電気四極子と磁気多極子であることが明らかになった。
Recently,
Al
compounds (
: rare earth,
: transition metal) have attracted much attention due to interesting physical properties closely related to their caged-structure. Each
ion is confined in a Frank-Kasper cage consisting of 16 Al atoms and the large coordination number leads to strong
-
hybridization. In addition, the Frank-Kasper cage allows various multipole degrees of freedom for the
-electrons at low
because of a highly symmetric crystalline-electric-field (CEF). Among the
Al
series, Pr
Al
(
: Ti, V) and Sm
Al
(
: Ti, V, Cr) exhibit both these features. The
ground doublet systems Pr
Al
(
: Ti, V) show a phase transition at
= 2.0K (Ti) and 0.6K (V). The order parameter is believed to be an electric quadrupole active in the
subspace. A possibility of the quadrupole Kondo effect has been discussed based on characteristic
-dependence in specific heat, resistivity, and magnetic susceptibility. The
ground quartet systems Sm
Al
(
: Ti, V, Cr) also exhibit a phase transition at
= 6.4K (Ti), 2.3K (V), and 1.8K (Cr). A nuclear specific heat study in SmTi
Al
suggests that the primary order parameter is a magnetic dipole in spite of field-insensitive nature of the phase boundary. A possible importance of a secondarily ordered octupole moment was discussed. We here present a microscopic study of PrTi
Al
and Sm
Al
(
: Ti, V, Cr) using muon spin relaxation. In PrTi
Al
, no additional local field was observed in the ordered phase. This strongly supports the quadrupole ordering scenario. On the other hand, an appearance of a coherent local field was observed below
in Sm
Al
. This is consistent with the primary magnetic dipole ordering. The frequency distribution suggests that the magnetic structure is possibly different between the Sm
Al
compounds.