Magnetic phase diagram of Cr1/3NbS2: SANS study

被引:1
|
作者
Bykov, A. A. [1 ]
Chubova, N. M. [2 ]
Altinbaev, E. V. [1 ,3 ]
Kousaka, Yu [4 ]
Ovchinnikov, A. S. [5 ]
Kishine, J. [6 ]
Grigoriev, S. V. [1 ,3 ]
机构
[1] NRC Kurchatov Inst PNPI, Gatchina 188300, Russia
[2] NRC Kurchatov Inst, Moscow 123182, Russia
[3] St Petersburg State Univ, St Petersburg 198504, Russia
[4] Hiroshima Univ, Ctr Chiral Sci, Hiroshima 7398526, Japan
[5] Ural Fed Univ, Inst Nat Sci & Math, Ekaterinburg 620075, Russia
[6] Open Univ Japan, Tokyo 2618586, Japan
关键词
SANS; Chiral soliton lattice; Phase diagram; TANTALUM DICHALCOGENIDES; NIOBIUM;
D O I
10.1016/j.jssc.2023.123951
中图分类号
O61 [无机化学];
学科分类号
070301 ; 081704 ;
摘要
The magnetic structure of the Cr1/3NbS2 compound was studied with help of small-angle neutron scattering under an applied magnetic field in a wide temperature range below TN = 130 K. At zero magnetic field the magnetic moments of Cr3+ ions build the helix structure with the wave vector k oriented along the c-axis of the chiral structure of P6322 space group. The detected diffraction ring is interpreted as scattering on the magnetic helices of randomly oriented crystallites within powder sample. The intensity of the diffraction peak decreases with temperature and dissolves at T = 115 K. The magnetic field differently affects the crystallites with helix wave vector k along the field and those with k perpendicular to the field. The magnetic field, when applied, leads to appearance of the chiral soliton lattice in the grains with k oriented perpendicularly to the field. The period of the chiral soliton lattice increases rapidly as H approaches HC1 = 0.25 T. The transition from chiral soliton lattice to the field-induced ferromagnet, however, is not homogeneous but is accompanied by strong ferromagnetic fluctuations in the wide field range around HC1. These fluctuations are well visible in the experiment as scattering centered at Q = 0. In the grains with k parallel to the field, the chiral soliton lattice undergoes a series of transitions from helimagnet to the conical state, and then to the field-induced ferromagnet at HC2 = 1.25 T. The period of the conical helix increases slightly (for 5%) with the field, while the transition to the field-induced ferromagnetic state is again accompanied by strong ferromagnetic fluctuations. The magnetic field-temperature phase diagrams for H perpendicular to the c-axis and for H parallel to the c-axis are plotted on the basis of the data obtained.
引用
收藏
页数:6
相关论文
共 50 条
  • [1] Magnetic phase transition in single crystals of the chiral helimagnet Cr1/3NbS2
    Ghimire, N. J.
    McGuire, M. A.
    Parker, D. S.
    Sipos, B.
    Tang, S.
    Yan, J. -Q.
    Sales, B. C.
    Mandrus, D.
    PHYSICAL REVIEW B, 2013, 87 (10)
  • [2] Comparative Electronic Structures of the Chiral Helimagnets Cr1/3NbS2 and Cr1/3TaS2
    Xie, Lilia S. S.
    Gonzalez, Oscar
    Li, Kejun
    Michiardi, Matteo
    Gorovikov, Sergey
    Ryu, Sae Hee
    Fender, Shannon S.
    Zonno, Marta
    Jo, Na Hyun
    Zhdanovich, Sergey
    Jozwiak, Chris
    Bostwick, Aaron
    Husremovic, Samra
    Erodici, Matthew P.
    Mollazadeh, Cameron
    Damascelli, Andrea
    Rotenberg, Eli
    Ping, Yuan
    Bediako, D. Kwabena
    CHEMISTRY OF MATERIALS, 2023, 35 (17) : 7239 - 7251
  • [3] Giant topological and planar Hall effect in Cr1/3NbS2
    Mayoh, D. A.
    Bouaziz, J.
    Hall, A. E.
    Staunton, J. B.
    Lees, M. R.
    Balakrishnan, G.
    PHYSICAL REVIEW RESEARCH, 2022, 4 (01):
  • [4] Structural disorder versus chiral magnetism in Cr1/3NbS2
    Dyadkin, V.
    Mushenok, F.
    Bosak, A.
    Menzel, D.
    Grigoriev, S.
    Pattison, P.
    Chernyshov, D.
    PHYSICAL REVIEW B, 2015, 91 (18)
  • [5] Electronic structure of the chiral helimagnet and 3d-intercalated transition metal dichalcogenide Cr1/3NbS2
    Sirica, N.
    Mo, S. -K.
    Bondino, F.
    Pis, I.
    Nappini, S.
    Vilmercati, P.
    Yi, J.
    Gai, Z.
    Snijders, P. C.
    Das, P. K.
    Vobornik, I.
    Ghimire, N.
    Koehler, M. R.
    Li, L.
    Sapkota, D.
    Parker, D. S.
    Mandrus, D. G.
    Mannella, N.
    PHYSICAL REVIEW B, 2016, 94 (07)
  • [6] Magnetic structure investigation of the intercalated transition metal dichalcogenide V1/3NbS2
    Hall, A. E.
    Khalyavin, D. D.
    Manuel, P.
    Mayoh, D. A.
    Orlandi, F.
    Petrenko, O. A.
    Lees, M. R.
    Balakrishnan, G.
    PHYSICAL REVIEW B, 2021, 103 (17)
  • [7] Role of intercalated cobalt in the electronic structure of Co1/3NbS2
    Popcevic, Petar
    Utsumi, Yuki
    Bialo, Izabela
    Tabis, Wojciech
    Gala, Mateusz A.
    Rosmus, Marcin
    Kolodziej, Jacek J.
    Tomaszewska, Natalia
    Garb, Mariusz
    Berger, Helmuth
    Batistic, Ivo
    Barisic, Neven
    Forro, Laszlo
    Tutis, Eduard
    PHYSICAL REVIEW B, 2022, 105 (15)
  • [8] Intercalation-induced states at the Fermi level and the coupling of intercalated magnetic ions to conducting layers in Ni1/3NbS2
    Boucher, Yuki Utsumi
    Bialo, Izabela
    Gala, Mateusz A.
    Tabis, Wojciech
    Rosmus, Marcin
    Olszowska, Natalia
    Kolodziej, Jacek J.
    Gudac, Bruno
    Novak, Mario
    Muniraju, Naveen Kumar Chogondahalli
    Batistic, Ivo
    Barisic, Neven
    Popcevic, Petar
    Tutis, Eduard
    PHYSICAL REVIEW B, 2024, 109 (08)
  • [9] The Magneto-Transport Properties of Cr1/3TaS2 with Chiral Magnetic Solitons
    Obeysekera, Dimuthu
    Gamage, Kasun
    Gao, Yunpeng
    Cheong, Sang-wook
    Yang, Junjie
    ADVANCED ELECTRONIC MATERIALS, 2021, 7 (10)
  • [10] Bulk properties of the chiral metallic triangular antiferromagnets Ni1/3NbS2 and Ni1/3TaS2
    An, Yeochan
    Park, Pyeongjae
    Kim, Chaebin
    Zhang, Kaixuan
    Kim, Hyeoncheol
    Avdeev, Maxim
    Kim, Jaewon
    Han, Myung-Joon
    Noh, Han-Jin
    Seong, Seungho
    Kang, J. -s.
    Kim, Hyeong-Do
    Park, Je-Geun
    PHYSICAL REVIEW B, 2023, 108 (05)