Antiferromagnetic Fluctuations in Square Lattice Systems
Examining magnetic behaviors in square lattices and their significance in technology.
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The behavior of magnetic materials is an important area of study in physics, especially when looking at how different interactions between particles affect their magnetic properties. This article discusses a specific type of magnetic behavior known as antiferromagnetic fluctuations in a square lattice system. Understanding these fluctuations can provide insights into various applications, including advanced technologies like spintronics and quantum computing.
Background
In solid-state systems, the way particles interact with each other can lead to different magnetic phenomena. One type of interaction occurs in antiferromagnetic systems, where neighboring spins align in opposite directions. This can lead to interesting properties and behaviors in various materials.
When examining a square lattice, which is a grid-like structure made up of points, the movement of electrons can be influenced by several factors. Among these are Hopping Terms, which describe how electrons move between neighboring sites, and Exchange Fields, which relate to the effect of magnetism in the material.
The interaction of these factors can lead to the formation of certain energy points in the material known as Van Hove singularities. These points are essential as they affect the overall Magnetic Ordering and fluctuations in the material.
Magnetic Ordering and Symmetry
The magnetic properties of a system are heavily influenced by its symmetry. In a square lattice model with specific hopping interactions, the system generally maintains a state where spins are randomly oriented. However, when an exchange field is introduced, this symmetry is broken, leading to different possible magnetic configurations.
This change can significantly affect how the spins within the material behave. The appearance of magnetic ordering is essential for understanding how materials might respond to external influences, such as magnetic fields.
Findings on Antiferromagnetic Fluctuations
We have looked closely at magnetic fluctuations within the square lattice system. Without interactions between electrons, we found that incommensurate antiferromagnetic fluctuations can arise. This means that these fluctuations don’t perfectly line up with the lattice structure but can still exist in a disordered arrangement.
When the system has a specific filling of electrons between two critical points, the behavior shifts. Beyond a certain filling, commensurate antiferromagnetic fluctuations become prevalent, meaning that they start to align more closely with the structure of the lattice.
Upon introducing electron-electron interactions, the results indicate that the system can still maintain stable antiferromagnetic fluctuations under certain conditions. These findings suggest that this type of magnetic ordering in a system is resistant to changes, even with the added interactions from other electrons.
Influence of the Exchange Field and Hopping Terms
The study showed that adding an exchange field can split energy levels in the material, which significantly changes the available electronic states. When examining the behavior under various parameters, including different types of hopping interactions, it was evident how these interactions can lead to changes in magnetic properties.
We observed that, even with a ferromagnetic substrate influencing the exchange field, no ferromagnetic fluctuations emerged. This finding is quite interesting as it indicates that even though a magnetic influence is present, it does not lead to the expected ferromagnetic behavior. Instead, the antiferromagnetic fluctuations remain the primary feature.
Analyzing the Spin Susceptibility
A key aspect of understanding how the material responds to external magnetic fields is through spin susceptibility, which measures how the spin arrangements react. By analyzing this, we can interpret various magnetic behaviors. A peak in spin susceptibility indicates tendencies toward either ferromagnetic or antiferromagnetic order.
In our analysis of Spin Susceptibilities, we identified patterns. For small electron fillings, we observed indications of commensurate antiferromagnetic fluctuations, while larger fillings led to incommensurate behavior. This transition points to the complexity of magnetic arrangements in the material as electron density changes.
The Role of Electron-Electron Interactions
In many materials, how electrons interact with one another plays a significant role in their overall magnetic properties. This is particularly true when discussing the Hubbard model, which includes a term for interactions between electrons occupying the same site.
Our findings showed that even with the use of the Hubbard model, which accounts for these interactions, the material continued to exhibit a strong tendency for antiferromagnetic behavior. This stability indicates that the magnetic characteristics go beyond simple interactions and are intrinsically part of the material’s nature.
Conclusion
Through thorough investigation of antiferromagnetic fluctuations in a square lattice system, interesting conclusions were drawn regarding the complex interplay of various factors. The presence of an exchange field and hopping terms significantly affect the magnetic responses. Despite the potential influence from a ferromagnetic substrate, ferromagnetic fluctuations were not observed, while antiferromagnetic fluctuations remained stable and robust under varying conditions.
Overall, these findings enhance our understanding of magnetic behaviors in materials, providing potential pathways for future applications in advanced technologies. As research continues, exploring these relationships will be crucial in leveraging magnetic properties for practical uses.
Title: Commensurate Antiferromagnetic Fluctuations with Small Electron Doping
Abstract: We investigate the presence of antiferromagnetic fluctuations in the longitudinal and transversal spin susceptibilities of a square lattice. The inclusion of both first and second neighbour hopping terms, along with exchange coupling, induces anti-ferromagnetic fluctuations over a finite range of fillings in both longitudinal and transversal static spin susceptibilities. In the absence of on-site Hubbard interaction, we observe incommensurate antiferromagnetic fluctuations between the two Van Hove fillings. Beyond the second Van Hove singularity at $ n=1.03 $, commensurate antiferromagnetic fluctuations dominate in both longitudinal and transversal spin susceptibilities. When incorporating a finite Hubbard interaction strength, $ U $, we find that the commensurate anti-ferromagnetic fluctuations are preserved in both longitudinal and transversal dressed spin susceptibilities. However anti-ferromagnetic fluctuations vanish beyond a critical value of the Hubbard coupling strength, $ U_{c} $. Despite the exchange field can be induced by a ferromagnetic substrate, we do not observe any ferromagnetic fluctuations in the system.
Authors: Mohsen Shahbazi, Mohammad Ali Maleki
Last Update: 2024-10-28 00:00:00
Language: English
Source URL: https://arxiv.org/abs/2407.09814
Source PDF: https://arxiv.org/pdf/2407.09814
Licence: https://creativecommons.org/licenses/by-nc-sa/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.
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