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New mechanism explains behaviour of materials exhibiting giant magnetoresistance
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一项新研究揭示了量子双交换铁磁材料的特性,这些材料因其在巨磁电阻效应(GMR)方面的应用而备受关注。研究表明,这些材料的独特行为,如磁振子模式软化和磁振子阻尼,并非源于晶格振动,而是纯粹由量子自旋效应和多轨道物理学引起。这一发现挑战了之前的观点,并为深入理解这些材料提供了新的视角,有助于改进硬盘驱动器等技术。

💡量子双交换铁磁材料自20世纪80年代末以来引起科学家的兴趣,因为其电阻受外部磁场强度的影响,即巨磁电阻(GMR)效应。该效应促成了现代硬盘驱动器存储容量的巨大提升,并于2007年为发现者赢得了诺贝尔奖。

🔬研究的核心问题在于,多个电子之间的库仑相互作用如何导致这些铁磁体中的电子自旋对齐。对于绝缘铁磁体,Goodenough-Kanamori规则可以预测自旋对齐;而对于金属铁磁体,双交换机制更为适用,电子的运动和自旋对齐内在相关,常占据多个轨道,需要采用不同的建模方式。

💫研究人员使用两轨道Hubbard-Kanamori模型和Kondo晶格模型来探索量子双交换铁磁体的两个显著特征:磁振子模式软化和磁振子阻尼。研究表明,这些现象可以纯粹源于量子自旋效应和多轨道物理学,无需晶格振动。

🔍研究结果表明,量子自旋效应和多轨道物理学是导致这些材料特性的关键因素,挑战了之前认为晶格振动是主导因素的观点。这为深入理解这些材料提供了新视角,并暗示了一些先前被认为次要的相互作用可能对实验结果产生重要影响。

Two distinctive features of materials known as quantum double-exchange ferromagnets are purely due to quantum spin effects and multiorbital physics, with no need for the lattice vibrations previously invoked to explain them. This theoretical result could lead to new insights into these technologically important materials, as it suggests that some of their properties may arise from interactions hitherto regarded as less important.

Quantum double-exchange ferromagnets have interested scientists since the late 1980s, when physicists led by Albert Fert and Peter Grünberg found that their electrical resistance depends strongly on the magnitude of an external magnetic field. This phenomenon is known as giant magnetoresistance (GMR), and its discovery led to an enormous increase in the storage capacity of modern hard-disk drives, which incorporate GMR structures into their magnetic field sensors. It also led, in 2007, to a Nobel Prize for Fert and Grünberg.

Modelling strategies

Despite these successes, however, physicist Jacek Herbrych of the Institute of Theoretical Physics at Wrocław University of Science and Technology in Poland, who led the new research effort, says that these materials remain somewhat mysterious. “They are theoretically complex, and even today, there is no exact solution to fully solve these systems,” he says.

The key question, Herbrych continues, is how Coulomb interactions between many individual electrons lead to the electron spins in these ferromagnets becoming aligned. “Physicists broadly distinguish two mechanisms,” he explains. “For insulating ferromagnets, the Goodenough-Kanamori rules (based on electron shell occupancy and geometrical arguments) can predict spin alignment. For metallic ferromagnets, the double-exchange mechanism is more appropriate.”

In this latter case, Herbrych explains, the electrons’ motion and the alignment of their spins are intrinsically linked, and the electrons often occupy multiple orbitals. This means they need to be modelled in a fundamentally different way.

The approach Herbrych and his colleagues took, which they describe in Rep. Prog. Phys., was conceptually simple, using a basic yet realistic model of interacting electrons to predict the quantum behaviour of electron spins. “In quantum mechanics, ‘simple’ can quickly become complex, however,” Herbrych notes. “Materials in which the double-exchange mechanism dominates typically exhibit multiorbital behaviour, as mentioned. A minimal model must therefore include electron mobility (or ‘itinerancy’), Coulomb interactions and orbital degrees of freedom.”

Two distinctive features

Herbrych and colleagues identified the two-orbital Hubbard-Kanamori model and the Kondo lattice model with interactions as fitting these requirements. They then used these models to explore two distinctive features of quantum double-exchange ferromagnets.

Both features involve magnons, which are collective oscillations of the materials’ spin magnetic moments. In basic “toy” models of ferromagnets, magnons exhibit a well-defined energy-momentum correspondence known as the dispersion relation. Quantum double-exchange ferromagnets, however, experience a phenomenon known as magnon mode softening: at short wavelengths, their magnons become nearly dispersionless, or momentum independent. “This implies that there are fundamental differences between long- and short-distance spin dynamics,” Herbrych says. “Magnons can travel over long distances but appear localized at short scales.”

The second distinctive feature is called magnon damping. This occurs when magnons lose coherence, meaning that the standard picture of spin flips propagating through the material’s lattice breaks down. “It was previously thought that Jahn-Teller phonons (lattice vibrations) were responsible for these features, and that a classical spin model with phonons would do, but our work challenges this view,” says Herbrych. “We show that these phenomena can arise purely from quantum spin effects and multiorbital physics, without requiring lattice vibrations.”

This is, he tells Physics World, “a remarkable result” as it suggests that some experimental features of quantum double-exchange ferromagnets may arise from interactions previously considered secondary.

Limitations and extensions

The researchers’ present work is restricted to one dimension, and they acknowledge that extending it to two or three dimensions will be a challenge. “Still, our approach offers a conceptual framework that can be approximately extended to higher dimensions,” Herbrych says. “The results not only provide insights into the physics of strongly correlated systems, but also into the interplay of competing phases, such as ferromagnetism, orbital order and superconductivity, observed in these materials.”

The post New mechanism explains behaviour of materials exhibiting giant magnetoresistance appeared first on Physics World.

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量子物理 铁磁材料 巨磁电阻 量子自旋
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