Magnetic Fluctuation and First-Order Transition in Trillium Lattice of EuPtSi Observed by 151Eu Mossbauer Spectroscopy

被引:10
作者
Homma, Yoshiya [1 ]
Kakihana, Masashi [2 ]
Tokunaga, Yo [3 ]
Yogi, Mamoru [4 ]
Nakashima, Miho [5 ]
Nakamura, Ai [1 ]
Shimizu, Yusei [1 ]
Li, Dexin [1 ]
Maurya, Arvind [1 ]
Sato, Yoshiki J. [1 ,6 ]
Honda, Fuminori [1 ]
Aoki, Dai [1 ]
Amako, Yasushi [5 ]
Hedo, Masato [4 ]
Nakama, Takao [4 ]
Onuki, Yoshichika [4 ]
机构
[1] Tohoku Univ, Inst Mat Res, Oarai, Ibaraki 3111313, Japan
[2] Univ Ryukyus, Grad Sch Engn & Sci, Nishihara, Okinawa 9030213, Japan
[3] Japan Atom Energy Agcy, Adv Sci Res Ctr, Tokai, Ibaraki 3191195, Japan
[4] Univ Ryukyus, Fac Sci, Nishihara, Okinawa 9030213, Japan
[5] Shinshu Univ, Fac Sci, Matsumoto, Nagano 3908621, Japan
[6] Tohoku Univ, Grad Sch Engn, Sendai, Miyagi 9808577, Japan
关键词
HELICAL SPIN STRUCTURE; HYPERFINE FIELDS; ISOMER-SHIFTS; PHASE; RELAXATION; MNSI;
D O I
10.7566/JPSJ.88.094702
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
We report the results of Eu-151 Mossbauer spectroscopy on EuPtSi with a chiral structure belonging to the P2(1)3 (#198) space group at zero magnetic field. The paramagnetic single absorption forms a magnetic splitting profile directly below T-N = 4.0 K and the spectrum at 3.9 K consists of the sum of the paramagnetic single absorption and the magnetic splitting absorption, which indicates a first-order transition at T-N = 4.0 K. The temperature dependence of the effective hyperfine fields H-hf at the Eu nucleus follows a power law of H-hf = H-0(1 - T/T-N)(beta) with H-0 = 25.6 +/- 0.4T and beta = 0.16 +/- 0.01 indicates a full moment of Eu2+ ions. The relative integral intensity I of the Eu-151 Mossbauer spectroscopy for EuPtSi is enhanced using a Debye calculation below T-0 similar or equal to 15 K, which indicates the development of magnetic correlations. The line width Gamma of the (151) Eu Mossbauer spectra increases below T-FD (similar or equal to 8K) close to the Weiss temperature theta(p) and shows a sharp peak at T-N. The magnetic behavior of EuPtSi can be divided into three magnetic regions: the paramagnetic (PM) phase, the fluctuation-disordered (FD) phase and the antiferromagnetic phase with fluctuation disordering (AF with FD). The magnetic fluctuation is realized around the first-order transition between the paramagnetic and helimagnetic states in EuPtSi.
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页数:8
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