Magnetic Behavior of KBaCr(PO4)2: A Study
Investigating the unique magnetic properties of KBaCr(PO4)2 reveals complex interactions.
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Table of Contents
The material KBaCr(PO4)2 has a special structure known as the double trillium lattice, which includes triangular units. This structure is used to study magnetic behavior, particularly the complex interactions of magnetic moments. Frustrated magnets, like this one, do not easily settle into a single magnetic configuration due to competing interactions, making their study fascinating.
Structure of KBaCr(PO4)2
KBaCr(PO4)2 has a crystal structure formed by two types of chromium sites connected through phosphorous and oxygen units. This structure allows for interesting magnetic behavior due to its geometry. The materials formed in this way can exhibit various magnetic phases, depending on the arrangement of magnetic moments.
Magnetic Behavior
The magnetic properties of KBaCr(PO4)2 were examined using several techniques, including x-ray diffraction, magnetization measurements, Heat Capacity tests, and nuclear magnetic resonance (NMR). These methods provided insights into the phase transitions and magnetic interactions present in the compound.
Magnetic Transitions
KBaCr(PO4)2 shows magnetic transitions at specific temperatures. Initially, at around a certain temperature, a magnetic order begins. As the temperature decreases further, another transition occurs under weak magnetic fields. Observations from NMR experiments confirm that the first transition corresponds to a three-dimensional structure.
Experimental Techniques
To study the properties of KBaCr(PO4)2, scientists prepared a polycrystalline sample using standard solid-state methods. They mixed stoichiometric quantities of relevant compounds and processed them in a controlled environment to achieve the desired structure.
Characterization Techniques
Various characterization techniques were employed to confirm the material's structure and magnetic properties:
- X-Ray Diffraction (XRD): This technique provided insights into the crystal structure, confirming the double trillium lattice.
- Magnetization Measurements: These measurements assessed how the material responds to magnetic fields at different temperatures.
- Heat Capacity Measurements: Changes in heat capacity were monitored to identify phase transitions and assess the contributions from magnetic and lattice vibrations.
- Nuclear Magnetic Resonance (NMR): NMR was used to investigate the local magnetic environment and dynamics of the magnetic moments.
Magnetic Susceptibility
Magnetic susceptibility refers to how a material reacts to an external magnetic field. For KBaCr(PO4)2, a unique pattern emerged. Initially, the susceptibility increased as the temperature lowered, followed by a broad peak indicating the onset of magnetic order. In weak applied fields, the behavior shifts, and the susceptibility displays characteristics of both ferromagnetic and antiferromagnetic interactions.
Heat Capacity Analysis
The heat capacity of KBaCr(PO4)2 was measured at different temperatures to identify the contributions of magnetic behavior and phonon vibrations. The data revealed a distinct peak at a particular temperature, indicating a change in the magnetic state. Analysis of the heat capacity provided information on the magnetic transition temperatures and the nature of magnetic interactions.
Thermal Conductivity
Thermal conductivity measurements offered insights into the behavior of magnetic spin excitations. The thermal conductivity showed an increase with temperature and displayed a notable feature at the point of magnetic transition. No clear signs of the second transition were observed under the same conditions, suggesting a complex interaction in the material's magnetic properties.
NMR Studies
Nuclear magnetic resonance (NMR) was crucial for understanding the static and dynamic magnetic properties of KBaCr(PO4)2. With a well-defined phosphorus site in the structure, NMR offered local insights into magnetic behavior. The NMR spectra became broader and asymmetric as temperature decreased, indicating interactions within the material.
Spin-Lattice Relaxation
The spin-lattice relaxation rate, a measure of how quickly a system returns to equilibrium after being disturbed, was studied using NMR. Two key anomalies were observed during spin-lattice relaxation measurements, corresponding to the magnetic transitions identified in previous analyses. This behavior indicated the presence of complex dynamics associated with the magnetic moments.
Spin-Spin Relaxation
Spin-spin relaxation, which concerns interactions between spins, was also analyzed. This part of the study confirmed the existence of two transitions, shedding light on the interactions between magnetic moments in KBaCr(PO4)2. Temperature dependence revealed how these interactions change as the system undergoes transitions.
Microscopic Magnetic Model
Building a microscopic model of the magnetic interactions in KBaCr(PO4)2 illuminated the role of different exchange interactions. The model explained the observed magnetic behavior through the coupling between chromium sites. The study highlighted the delicate balance of magnetic interactions that leads to the unusual properties of this material.
Conclusion
KBaCr(PO4)2 serves as an interesting example of a non-frustrated magnetic system. The combination of antiferromagnetic and ferromagnetic interactions leads to intricate behavior, marked by multiple magnetic transitions. Insights gained from various experimental techniques lay the groundwork for better understanding similar materials and their magnetic properties.
Future Directions
Further research could explore the effects of temperature and magnetic field variations on KBaCr(PO4)2. Additionally, investigating similar compounds could reveal more about the nature of magnetic frustration and phase transitions in materials with complex geometries.
Title: Ground-state properties of the double trillium lattice antiferromagnet KBaCr$_2$(PO$_4$)$_3$
Abstract: Trillium lattices formed by corner-shared triangular units are the platform for magnetic frustration in three dimensions. Herein, we report structural and magnetic properties of the Cr-based double trillium lattice material KBaCr$_2$(PO$_4$)$_3$ studied by x-ray diffraction, magnetization, heat capacity, thermal conductivity, and $^{31}$P nuclear magnetic resonance (NMR) measurements complemented by density-functional band-structure calculations. Heat capacity and $^{31}$P NMR measurements reveal the magnetic transition at $T_{\rm N1} \simeq 13.5$ K in zero field followed by another transition at $T_{\rm N2} \simeq 7$ K in weak applied fields. The NMR sublattice magnetization confirms that the transition at $T_{\rm N1}$ is 3D in nature. The $^{31}$P spin-lattice relaxation rate in the ordered state follows the $T^3$ behavior indicative of the two-magnon Raman process. The spin lattice of KBaCr$_2$(PO$_4$)$_3$ comprises two crystallographically nonequivalent ferromagnetic sublattices that are coupled antiferromagnetically, thus eliminating frustration in this trillium network.
Authors: R. Kolay, Qing-Ping Ding, Y. Furukawa, A. A. Tsirlin, R. Nath
Last Update: 2024-07-12 00:00:00
Language: English
Source URL: https://arxiv.org/abs/2407.09376
Source PDF: https://arxiv.org/pdf/2407.09376
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.
Reference Links
- https://doi.org/
- https://doi.org/10.1146/annurev.ms.24.080194.002321
- https://doi.org/10.1103/RevModPhys.89.025003
- https://doi.org/10.1103/RevModPhys.58.801
- https://doi.org/10.1126/science.1064761
- https://doi.org/10.1088/1361-648X/ab724e
- https://doi.org/10.1103/PhysRevLett.98.107204
- https://doi.org/10.1038/s41567-019-0577-6
- https://doi.org/10.1038/s41567-018-0317-3
- https://doi.org/10.1038/s41467-020-15594-1
- https://doi.org/10.1103/PhysRevLett.115.047201
- https://doi.org/10.1126/science.1166767
- https://doi.org/10.1126/sciadv.1602562
- https://doi.org/10.1038/nmat2916
- https://doi.org/10.1103/PhysRevLett.102.186602
- https://doi.org/10.1103/PhysRevLett.106.156603
- https://doi.org/10.1103/PhysRevLett.128.177201
- https://doi.org/10.1103/PhysRevLett.127.157204
- https://doi.org/10.1103/PhysRevLett.131.146701
- https://doi.org/10.1063/5.0096942
- https://doi.org/10.1103/PhysRevB.109.184432
- https://doi.org/10.1016/0022-4596
- https://doi.org/10.1016/0921-4526
- https://doi.org/10.1016/0927-0256
- https://doi.org/10.1103/PhysRevB.54.11169
- https://doi.org/10.1103/PhysRevLett.77.3865
- https://doi.org/10.1103/PhysRevB.84.224429
- https://doi.org/10.1103/PhysRevLett.87.047203
- https://doi.org/10.1016/j.jmmm.2006.10.304
- https://doi.org/10.1021/ed085p532
- https://doi.org/10.1103/PhysRevB.109.134401
- https://doi.org/10.1103/PhysRevB.98.144436
- https://doi.org/10.1103/PhysRevB.84.094445
- https://doi.org/10.1103/PhysRevB.90.024431
- https://doi.org/10.1103/PhysRevB.94.014415
- https://doi.org/10.1103/PhysRevB.108.104424
- https://doi.org/10.1103/PhysRevB.108.014429
- https://doi.org/10.1126/science.1188200
- https://doi.org/10.48550/arXiv.2206.08866
- https://doi.org/10.1103/PhysRevB.107.184423
- https://doi.org/10.1103/PhysRevB.91.024413
- https://doi.org/10.1103/PhysRevB.78.024418
- https://doi.org/10.1143/PTP.16.23
- https://doi.org/10.1103/PhysRevB.80.214430
- https://doi.org/10.1103/PhysRevB.74.184408
- https://doi.org/10.1103/PhysRev.166.359
- https://doi.org/10.1103/PhysRevB.106.024426
- https://doi.org/10.1088/0370-1328/80/6/119
- https://doi.org/10.1103/PhysRevB.71.174436
- https://doi.org/10.1143/JPSJ.69.2660
- https://doi.org/10.1143/JPSJ.55.1751
- https://doi.org/10.1143/JPSJ.39.672
- https://doi.org/10.1103/PhysRevB.87.064417
- https://doi.org/10.1103/PhysRevB.90.214424
- https://doi.org/10.1002/pssa.2211210162
- https://doi.org/10.1103/PhysRevB.95.045142
- https://doi.org/10.1103/PhysRevB.83.144412