Magnetic Properties and Magnetic Phase Diagrams of Trigonal DyNi<sub>3</sub>Ga<sub>9</sub>

Ninomiya, Hiroki; Matsumoto, Yuji; Nakamura, Shota; Kono, Yohei; Kittaka, Shunichiro; Sakakibara, Toshiro; Inoue, Katsuya; Ohara, Shuichi

doi:10.7566/jpsj.86.124704

Cited by 14 publications

(18 citation statements)

References 30 publications

Supporting

Mentioning

Contrasting

Order By: Relevance

“…The bending may be caused by the ab-plane component, where the c-axis is not perpendicular to the ab-plane in Yb 4 Ga 24 Pt 9 -type crystal structure. Multiple magnetization plateaus are also observed in R 0.67 T n M 2n+m family (R = Dy) [2,4,8]. The magnetic ordered temperature and paramagnetic Curie temperature of Dy 4 Pd 9 Ga 24 are almost the same as those of Dy 0.67 T n M 2n+m , although the distance between the honeycomb layers is different.…”

Section: Dy 4 Pd 9 Ga 24mentioning

confidence: 85%

See 1 more Smart Citation

New Rare-earth Intermetallic Compounds Dy₄Pd₉Ga₂₄ and Er₄Pd₉Ga₂₄

Nakamura

Yada

Ohara

2020

Proceedings of J-Physics 2019: International Conference on Multipole Physics and Related Phenomena

Self Cite

View full text Add to dashboard Cite

We have discovered new rare-earth intermetallic compounds Dy 4 Pd 9 Ga 24 and Er 4 Pd 9 Ga 24. These materials crystallize in a monoclinic Yb 4 Ga 24 Pt 9-type crystal structure (space group: C2/m). This crystal structure is a laminated structure, and rare earth ions form a honeycomb structure on the ab-plane. We have measured the specific heat and magnetization of these compounds. Dy 4 Pd 9 Ga 24 exhibits antiferromagnetic ordering at 12 K, and multiple plateaus are observed in the magnetization curve for a magnetic field in the ab-plane. Er 4 Pd 9 Ga 24 antiferromagnetically orders at 5.4 K, and a metamagnetic transition occurs when a magnetic field is applied along the magnetization easy c axis.

show abstract

Section: Dy 4 Pd 9 Ga 24mentioning

confidence: 85%

“…DyNi 3 Ga 9 , ErNi 3 Ga 9 , and YbNi 3 Al 9 are famous in this family, when n = 2 and m = 2. Quadrupole order, helical magnetism, and canted magnetic structures are observed in DyNi 3 Ga 9 [2,3], and the magnetization curve shows multiple plateaus. ErNi 3 Ga 9 exhibits metamagnetic transition [4].…”

Section: Introductionmentioning

confidence: 95%

New Rare-earth Intermetallic Compounds Dy₄Pd₉Ga₂₄ and Er₄Pd₉Ga₂₄

Nakamura

Yada

Ohara

2020

Proceedings of J-Physics 2019: International Conference on Multipole Physics and Related Phenomena

Self Cite

View full text Add to dashboard Cite

show abstract

“…[40][41][42] In general, Dzyaloshinskii-Moriya interaction plays a key role in the formation of magnetic skyrmions in chiral magnets, which is induced by the relativistic spin-orbit coupling. 57,58) The typical skyrmions in magnetic materials are Bloch-type skyrmion, Néel-type skyrmion, and intermediatetype skyrmion. 59,60) However, the skyrmions in trapped BECs are expected to display more novel properties and richer structures due to the precise controllability of many experimental parameters of ultracold atoms.…”

Section: Effect Of Rotation In the Absence Of Socmentioning

confidence: 99%

Topological Defects of Spin–Orbit Coupled Bose–Einstein Condensates in a Rotating Anharmonic Trap

et al. 2018

View full text Add to dashboard Cite

We investigate the topological defects and spin structures of binary Bose-Einstein condensates (BECs) with Dresselhaus spin-orbit coupling (D-SOC) in a rotating anharmonic trap. Our results show that for initially mixed BECs without SOC the increasing rotation frequency can lead to the structural phase transition of the system. In the presence of isotropic D-SOC, the system sustains vortex pair, Anderson-Toulouse coreless vortices, circular vortex sheets, and combined vortex structures. In particular, when the rotation frequency is fixed above the radial trapping frequency the strong D-SOC results in a peculiar topological structure which is comprised of multi-layer visible vortex necklaces, hidden vortex necklaces and a hidden giant vortex. In addition, the system exhibits rich spin textures including basic skyrmion, meron cluster, skyrmion string and various skyrmion lattices. The skyrmions will be destroyed in the limit of large D-SOC or rotation frequency. Furthermore, the effects of anisotropic D-SOC and Rashba-Dresselhaus SOC on the topological structures of the system are discussed.

show abstract

“…VESTA was used to draw the figure [24]. (b) Temperature dependences of magnetization at low field, specific heat, and C66 elastic modulus of DyNi3Ga9 reproduced from the literatures [19,20].…”

Section: Introductionmentioning

confidence: 99%

Competition between helimagnetic and ferroquadrupolar orderings in a monoaxial chiral magnet DyNi$_3$Ga$_{9}$ studied by resonant x-ray diffraction

Tsukagoshi,

Matsumura,

Michimura

et al. 2022

Preprint

Self Cite

View full text Add to dashboard Cite

Successive phase transitions in a rare-earth monoaxial chiral magnet DyNi3Ga9 have been investigated by resonant x-ray diffraction. Magnetic dipole and electric quadrupole degrees of freedom arising from the large angular moment of J = 15/2, in combination with the symmetric and antisymmetric exchange interactions and the crystal field anisotropy, give rise to competing ordered phases. We show that the antiferromagnetically coupled Dy moments in the ab-plane form an incommensurate helimagnetic order with q ∼ (0, 0, 0.43) just below TN = 10 K, which further exhibits successive first-order transitions to the commensurate helimagnetic order with q = (0, 0, 0.5) at T ′ N = 9.0 K, and to the canted antiferromagnetic order with q = (0, 0, 0) at T ′′ N = 8.5 K, both with large coexistence regions. The relation of the magnetic helicity and the crystal chirality in DyNi3Ga9 is also uniquely determined. Splitting of the (6, 0, 0) Bragg peak is observed below T ′′ N , reflecting the lattice distortion due to the ferroquadrupole order. In the canted antiferromagnetic phase, a spin-flop transition takes place at 5 K when the temperature is swept in a weak magnetic field. We discuss these transitions from the viewpoint of competing energies described above.

show abstract

Magnetic Properties and Magnetic Phase Diagrams of Trigonal DyNi₃Ga₉

Cited by 14 publications

References 30 publications

New Rare-earth Intermetallic Compounds Dy₄Pd₉Ga₂₄ and Er₄Pd₉Ga₂₄

New Rare-earth Intermetallic Compounds Dy₄Pd₉Ga₂₄ and Er₄Pd₉Ga₂₄

Topological Defects of Spin–Orbit Coupled Bose–Einstein Condensates in a Rotating Anharmonic Trap

Competition between helimagnetic and ferroquadrupolar orderings in a monoaxial chiral magnet DyNi$_3$Ga$_{9}$ studied by resonant x-ray diffraction

Contact Info

Product

Resources

About

Magnetic Properties and Magnetic Phase Diagrams of Trigonal DyNi3Ga9

Cited by 14 publications

References 30 publications

New Rare-earth Intermetallic Compounds Dy4Pd9Ga24 and Er4Pd9Ga24

New Rare-earth Intermetallic Compounds Dy4Pd9Ga24 and Er4Pd9Ga24

Topological Defects of Spin–Orbit Coupled Bose–Einstein Condensates in a Rotating Anharmonic Trap

Competition between helimagnetic and ferroquadrupolar orderings in a monoaxial chiral magnet DyNi$_3$Ga$_{9}$ studied by resonant x-ray diffraction

Contact Info

Product

Resources

About

Magnetic Properties and Magnetic Phase Diagrams of Trigonal DyNi₃Ga₉

New Rare-earth Intermetallic Compounds Dy₄Pd₉Ga₂₄ and Er₄Pd₉Ga₂₄

New Rare-earth Intermetallic Compounds Dy₄Pd₉Ga₂₄ and Er₄Pd₉Ga₂₄