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Investigating Spin Pumping in Altermagnets

Study reveals how altermagnet orientation influences spin pumping effects.

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Spin Pumping is a process that generates Spin Currents, which are flows of tiny magnetic moments, in magnetic materials. This happens when the magnetic orientation of one material affects the adjacent material, creating a flow of spin without the need for charge flow. In this case, we focus on the interaction between a Ferromagnetic Insulator and a unique type of material known as an altermagnet. Altermagnets are intriguing because they have a particular kind of magnetic ordering that allows for spin-polarized electrons, yet they have no overall magnetization. This unique property opens up exciting possibilities in the field of spintronics, where the goal is to use the spin of electrons, rather than their charge, for information processing.

What is Spin Pumping?

Spin pumping occurs when the magnetization in a magnetic material oscillates, transferring its angular momentum to a nearby non-magnetic material. In simple terms, think of it as a spinning top passing some of its energy to a nearby object. In spintronics, magnetic insulators, like yttrium iron garnet (YIG), are particularly valuable because they can produce spin currents with minimal energy loss. When a spin current passes into a non-magnetic material, it can affect the magnetic properties of that material.

The Appeal of Altermagnets

Recently, scientists have shown increasing interest in altermagnets due to their potential applications in advanced technologies. These materials possess a special feature: they can have spin-polarized electrons without having a net magnetic moment. This means that they combine properties from both ferromagnetic and antiferromagnetic materials, making them versatile. Altermagnets can be found in various forms, including insulators, semiconductors, and even superconductors.

The Study of Spin Pumping into Altermagnets

In this study, we explore how spin pumping behaves when it interacts with an altermagnet. We specifically look at how the orientation of the altermagnet affects this process. We examine two different configurations of the altermagnet, with slight differences in their structure. These orientations change how the spin-polarized electrons interact with the layers at the interface, leading to different outcomes.

Connection Between Spin Pumping and Crystallographic Orientation

The behavior of spin pumping can significantly vary depending on how the altermagnet is oriented concerning the interface. The altermagnetic state can either boost or reduce spin pumping. Essentially, the spin-splitting nature of the altermagnet alters how much spin current can flow through. By considering factors like how electrons flip their spin when they reach the interface, we can begin to explain these observations.

Interfacial Effects and Rashba Spin-orbit Coupling

A critical aspect of our study is the impact of interfacial Rashba spin-orbit coupling, which refers to a phenomenon that occurs at the boundary between different materials. This effect can amplify the spin-pumping process but can also lead to complex behavior based on the strength of the spin-orbit coupling. We find that there is an optimal level of this coupling that can enhance the spin current significantly, even in orientations where spin pumping would typically be suppressed.

The Mechanism Behind the Spin Pumping Effect

To generate spin currents, we consider a scenario where electrons are incident from the altermagnet side. The behavior of these electrons can be described using a framework that captures their energy and spin states. The incident electrons can reflect or transmit through the interface into the ferromagnetic insulator, and this interaction leads to the generation of a spin current.

Variations in Spin Pumping for Different Altermagent Orientations

By analyzing two specific orientations of the altermagnet, we can see how they affect the spin pumping current. In one scenario, the alignment of the spin-polarized lobes enables a more significant flow of spin current, while in another orientation, this flow is restricted. The difference arises because the interaction between the incoming electrons and their respective wave vectors varies based on the alignment of the altermagnet and insulator.

Importance of the Fermi Surface

A key concept in understanding how spin currents flow in different materials is the Fermi surface. This is essentially a representation of how energy levels are filled with electrons in the material. In our case, the shape of the Fermi surface in the altermagnet adjusts depending on its orientation, which directly impacts how many states are available for the electrons to occupy and thus how they can contribute to the spin pumping process.

Observing Trends in Spin Currents

Through our investigations, we observe that the total spin current can be understood by looking at the quality of the contact between the ferromagnetic insulator and the altermagnet. A strong contact allows for better transmission of spin currents. As the interface gets better (in terms of transparency), the spin pumping effects become more pronounced.

Spin-Flip Probability

In our studies, we also look at the probability of spin-flip events. This refers to the chance that an electron will change its spin state when it transmits through the interface. We discover that this probability behaves differently depending on the configuration of the altermagnet. In some cases, aligning the interface correctly can enhance the effectiveness of spin-flip events, leading to a more substantial overall spin current.

Rashba Spin-Orbit Coupling Effects

The introduction of Rashba spin-orbit coupling creates additional complexity. As we increase the strength of this effect, we notice a non-linear relationship between the coupling strength and the spin pumping current. At certain levels, the spin current reaches a peak and then starts to decline as the coupling becomes stronger. This suggests an optimal point where configurations can be tuned to maximize the flow of spin current effectively.

Conclusion

Our exploration of spin pumping into altermagnets opens up new avenues for research and application in the field of spintronics. By understanding how different orientations of the altermagnet affect spin current, and how interfacial effects play into this mechanism, we can better harness these materials for future technologies. As we delve deeper into the characteristics of altermagnets, we can envision their roles in driving innovation in information processing and storage.

Future Directions

Moving forward, it will be essential to continue investigating various materials and configurations to fully understand their properties. The interplay between crystallographic orientation, interfacial effects, and material characteristics will likely lead to new and exciting findings in the realm of quantum materials and spintronics. By leveraging these advances, we can enhance the performance and efficiency of future electronic devices, making them significantly more effective than their predecessors.

Original Source

Title: Spin pumping from a ferromagnetic insulator into an altermagnet

Abstract: A class of antiferromagnets with spin-polarized electron bands, yet zero net magnetization, called altermagnets is attracting increasing attention due to their potential use in spintronics. Here, we study spin injection into an altermagnet via spin pumping from a ferromagnetic insulator. We find that the spin pumping behaves qualitatively different depending on how the altermagnet is crystallographically oriented relative the interface to the ferromagnetic insulator. The altermagnetic state can enhance or suppress spin pumping, which we explain in terms of spin-split altermagnetic band structure and the spin-flip probability for the incident modes. Including the effect of interfacial Rashba spin-orbit coupling, we find that the spin-pumping effect is in general magnified, but that it can display a non-monotonic behavior as a function of the spin-orbit coupling strength. We show that there exists an optimal value of the spin-orbit coupling strength which causes an order of magnitude increase in the pumped spin current, even for the crystallographic orientation of the altermagnet which suppresses the spin pumping.

Authors: Chi Sun, Jacob Linder

Last Update: 2023-08-23 00:00:00

Language: English

Source URL: https://arxiv.org/abs/2308.12335

Source PDF: https://arxiv.org/pdf/2308.12335

Licence: https://creativecommons.org/licenses/by/4.0/

Changes: This summary was created with assistance from AI and may have inaccuracies. For accurate information, please refer to the original source documents linked here.

Thank you to arxiv for use of its open access interoperability.

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