在Ga3+替代的DyCrO3中进行多个旋转重定向过渡
Xiong-Han Liu1, Meng-Qi Ye1, Hai-Bo Xiao1
1Key Laboratory for Intelligent Sensing System and Security of Ministry of Education, School of Physics, Hubei University, Wuhan 430062, People's Republic of China. wangrl@hubu.edu.cn.
Physical chemistry chemical physics : PCCP
|March 11, 2025
概括
在DyCrO3中的替代引发了多个旋转重定向过渡,与纯粹的DyCrO3.3不同. 这些发现凸显了DyCr1-xGaxO3作为磁开关装置的有前途材料.
科学领域:
- 固态化学 固态化学
- 磁力学和磁性材料的使用
- 稀土化合物 稀土化合物
背景情况:
- 罕见地质石表现出复杂的磁现象.
- 旋转重定向过渡对于磁性应用至关重要.
- 了解替代效应是调整材料性质的关键.
研究的目的:
- 为了合成和描述单相DyCr1-xGaxO3 (0 ≤ x ≤ 0.5) 样品.
- 为了研究Ga3+替代对磁性特性的影响,特别是旋转重定向过渡.
- 探索这些材料在磁性开关装置中的潜力.
主要方法:
- 用于样本制备的Sol-gel合成方法.
- 磁性测量以确定磁性转换和易感性.
- 分析温度依赖的反向易感性,以识别相位.
主要成果:
- 成功合成了单相DyCr1-xGaxO3样本.
- 用Ga3+替代的样本显示出多次旋转重定向过渡 (Γ2 → Γ4 → Γ2 → Γ1),这是稀土石的新型观测.
- 在Ga3+替代样本中确定了格里菲斯阶段.
- 观察到的磁性行为归因于由于Ga3+替代而导致的弱化交换相互作用.
结论:
- 在DyCrO3中Ga3+的替代导致了前所未有的多重旋转重定向过渡.
- 格里菲斯相和多个过渡的存在表明了丰富的磁性结构.
- DyCr1-xGaxO3 材料在磁性开关设备中的应用方面表现有前途.
相关概念视频
Atomic Nuclei: Nuclear Spin State Overview
841
NMR-active nuclei have energy levels called 'spin states' that are associated with the orientations of their nuclear magnetic moments. In the absence of a magnetic field, the nuclear magnetic moments are randomly oriented, and the spin states are degenerate. When an external magnetic field is applied, the spin states have only 2 + 1 orientations available to them. A proton with = ½ has two available orientations. Similarly, for a quadrupolar nucleus with a nuclear spin value of...
841
Atomic Nuclei: Nuclear Relaxation Processes
598
In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis, the precessing magnetic moments are randomly oriented around the z-axis.
598
Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)
938
Two NMR-active nuclei bonded to a central atom can be involved in geminal or two-bond coupling. Geminal coupling is commonly seen between diastereotopic protons in chiral molecules and unsymmetrical alkenes, among others.
The central atom need not be NMR-active because its electrons are affected by the electron polarization of the spin-active atoms. However, spin information is transmitted less effectively than in one-bond coupling, and 2J values are usually weaker than 1J values. The energy of...
The central atom need not be NMR-active because its electrons are affected by the electron polarization of the spin-active atoms. However, spin information is transmitted less effectively than in one-bond coupling, and 2J values are usually weaker than 1J values. The energy of...
938
Spin–Spin Coupling: One-Bond Coupling
920
Coupling interactions are strongest between NMR-active nuclei bonded to each other, where spin information can be transmitted directly through the pair of bonding electrons. While nuclei polarize their electrons to the opposite spins, the bonding electron pair has opposite spins. Configurations with antiparallel nuclear spins are expected to be lower in energy. When coupling makes antiparallel states more favorable, J is considered to have a positive value. The one-bond coupling constant, 1J,...
920
NMR Spectroscopy: Spin–Spin Coupling
1.2K
The spin state of an NMR-active nucleus can have a slight effect on its immediate electronic environment. This effect propagates through the intervening bonds and affects the electronic environments of NMR-active nuclei up to three bonds away; occasionally, even farther. This phenomenon is called spin–spin coupling or J-coupling. Coupling interactions are mutual and result in small changes in the absorption frequencies of both nuclei involved. While nuclei of the same element are involved...
1.2K
Atomic Nuclei: Magnetic Resonance
602
The number of nuclear spins aligned in the lower energy state is slightly greater than those in the higher energy state. In the presence of an external magnetic field, as the spins precess at the Larmor frequency, the excess population results in a net magnetization oriented along the z axis. When a pulse or a short burst of radio waves at the Larmor frequency is applied along the x axis, the coupling of frequencies causes resonance and flips the nuclear spins of the excess population from the...
602


