Balasubramanian Balamurugan, Manchanda Priyanka, Pahari Rabindra, Chen Zhen, Zhang Wenyong, Valloppilly Shah R, Li Xingzhong, Sarella Anandakumar, Yue Lanping, Ullah Ahsan, Dev Pratibha, Muller David A, Skomski Ralph, Hadjipanayis George C, Sellmyer David J
Nebraska Center for Materials and Nanoscience, University of Nebraska, Lincoln, Nebraska 68588, USA.
Department of Physics and Astronomy, University of Nebraska, Lincoln, Nebraska 68588, USA.
Phys Rev Lett. 2020 Feb 7;124(5):057201. doi: 10.1103/PhysRevLett.124.057201.
Magnets with chiral crystal structures and helical spin structures have recently attracted much attention as potential spin-electronics materials, but their relatively low magnetic-ordering temperatures are a disadvantage. While cobalt has long been recognized as an element that promotes high-temperature magnetic ordering, most Co-rich alloys are achiral and exhibit collinear rather than helimagnetic order. Crystallographically, the B20-ordered compound CoSi is an exception due to its chiral structure, but it does not exhibit any kind of magnetic order. Here, we use nonequilibrium processing to produce B20-ordered Co_{1+x}Si_{1-x} with a maximum Co solubility of x=0.043. Above a critical excess-Co content (x_{c}=0.028), the alloys are magnetically ordered, and for x=0.043, a critical temperature T_{c}=328 K is obtained, the highest among all B20-type magnets. The crystal structure of the alloy supports spin spirals caused by Dzyaloshinskii-Moriya interactions, and from magnetic measurements we estimate that the spirals have a periodicity of about 17 nm. Our density-functional calculations explain the combination of high magnetic-ordering temperature and short periodicity in terms of a quantum phase transition where excess-cobalt spins are coupled through the host matrix.
具有手性晶体结构和螺旋自旋结构的磁体最近作为潜在的自旋电子材料备受关注,但其相对较低的磁有序温度是一个缺点。虽然钴长期以来一直被认为是促进高温磁有序的元素,但大多数富钴合金是非手性的,表现出共线而非螺旋磁序。从晶体学角度来看,B20有序化合物CoSi因其手性结构是个例外,但它不表现出任何类型的磁序。在此,我们采用非平衡工艺制备了最大钴溶解度为x = 0.043的B20有序Co₁₊ₓSi₁₋ₓ。在临界过量钴含量(xₑ = 0.028)以上,合金呈现磁有序,对于x = 0.043,获得了临界温度Tc = 328 K,这是所有B20型磁体中最高的。合金的晶体结构支持由Dzyaloshinskii - Moriya相互作用引起的自旋螺旋,并且通过磁性测量我们估计螺旋的周期约为17 nm。我们的密度泛函计算从量子相变的角度解释了高磁有序温度和短周期的结合,在该量子相变中过量钴自旋通过主体基质耦合。