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Relevant bibliographies by topics / Two Dimensional Triangular Lattice Antiferromagnetic AgFeO2

Academic literature on the topic 'Two Dimensional Triangular Lattice Antiferromagnetic AgFeO2'

Author: Grafiati

Published: 7 September 2023

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Journal articles on the topic "Two Dimensional Triangular Lattice Antiferromagnetic AgFeO2"

1

Zvereva, E. A., T. M. Vasilchikova, M. I. Stratan, A. A. Belik, and A. N. Vasiliev. "Spin Dynamics of Two-Dimensional Triangular-Lattice Antiferromagnet 3R-AgFeO2." Applied Magnetic Resonance 50, no. 5 (December 11, 2018): 637–48. http://dx.doi.org/10.1007/s00723-018-1106-y.

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2

Adhikary, Souren, Sudipta Dutta, and Sasmita Mohakud. "Antiferromagnetic spin ordering in two-dimensional honeycomb lattice of SiP3." Nanoscale Advances 3, no. 8 (2021): 2217–21. http://dx.doi.org/10.1039/d1na00101a.

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3

Yao, Xiaoyan. "Partially disordered antiferromagnetic state in two-dimensional triangular-lattice antiferromagnet." Physics Letters A 374, no. 6 (January 2010): 886–90. http://dx.doi.org/10.1016/j.physleta.2009.12.001.

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4

Sim, Hasung, Joosung Oh, Jaehong Jeong, Manh Duc Le, and Je-Geun Park. "HexagonalRMnO3: a model system for two-dimensional triangular lattice antiferromagnets." Acta Crystallographica Section B Structural Science, Crystal Engineering and Materials 72, no. 1 (January 23, 2016): 3–19. http://dx.doi.org/10.1107/s2052520615022106.

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The hexagonalRMnO3(h-RMnO3) are multiferroic materials, which exhibit the coexistence of a magnetic order and ferroelectricity. Their distinction is in their geometry that both results in an unusual mechanism to break inversion symmetry and also produces a two-dimensional triangular lattice of Mn spins, which is subject to geometrical magnetic frustration due to the antiferromagnetic interactions between nearest-neighbor Mn ions. This unique combination makes theh-RMnO3a model system to test ideas of spin-lattice coupling, particularly when both the improper ferroelectricity and the Mn trimerization that appears to determine the symmetry of the magnetic structure arise from the same structure distortion. In this review we demonstrate how the use of both neutron and X-ray diffraction and inelastic neutron scattering techniques have been essential to paint this comprehensive and coherent picture ofh-RMnO3.

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5

Fujita, Wataru. "Crystal structures, and magnetic and thermal properties of basic copper formates with two-dimensional triangular-lattice magnetic networks." RSC Advances 8, no. 57 (2018): 32490–96. http://dx.doi.org/10.1039/c8ra07134a.

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6

Dong, Zhan-Hai, and Shiping Feng. "Spin-Liquid State for Two-Dimensional Heisenberg Antiferromagnets on a Triangular Lattice." Modern Physics Letters B 12, no. 17 (July 20, 1998): 677–83. http://dx.doi.org/10.1142/s0217984998000792.

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The spin liquid state of the antiferromagnetic Heisenberg model on a triangular lattice is studied within the self-consistent Green's function method. It is shown that the spin excitation spectra is gapless, and ground-state energy per site is Eg/NJ=-0.966, which is in very good agreement with the results obtained within the variational Monte Carlo method based on the resonating-valence-bond state. Some thermodynamic properties are also discussed.

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7

Zhang, Bingwen, Xuejiao Chen, Fenglin Deng, Xiaodong Lv, Cheng Zhang, Biao Zheng, Huining Wang, and Jun Wang. "Spin direction tunable topological transition in two-dimensional frustrate antiferromagnetic triangular lattice T-FeO₂ monolayer." Applied Physics Letters 121, no. 23 (December 5, 2022): 232405. http://dx.doi.org/10.1063/5.0123488.

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Recently, numerous two-dimensional (2D) magnetic materials are predicted with various promising properties, whereas noncollinear antiferromagnetic 2D materials are rarely reported. In this paper, we predicted a stable 2D noncollinear antiferromagnetic triangular lattice T-FeO2. The ground state is [Formula: see text] antiferromagnetic with stronger next nearest neighbor exchange coupling than that of nearest neighbor exchange coupling because of the RKKY interaction. Our Monte Carlo simulations reveal that the magnetic phase transition is from a [Formula: see text] antiferromagnetic state to a stripy state and then to a paramagnetic state with increasing temperature. In addition, by tuning the spin direction from an in plane antiferromagnetic state to a canted weak ferromagnetic state, a nontrivial topological phase transition could be induced. Our investigation about magnetic property and nontrivial topological phase transition is very promising for antiferromagnetic spintronics.

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8

Murtazaev, A. K., and A. B. Babaev. "Phase transitions in the two-dimensional antiferromagnetic Potts model on a triangular lattice." Bulletin of the Russian Academy of Sciences: Physics 77, no. 10 (October 2013): 1272–74. http://dx.doi.org/10.3103/s1062873813100237.

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9

Babaev, A. B., and A. K. Murtazaev. "Weak Universality in the Disordered Two-Dimensional Antiferromagnetic Potts Model on a Triangular Lattice." JETP Letters 107, no. 10 (May 2018): 624–28. http://dx.doi.org/10.1134/s0021364018100053.

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10

Babaev, A. B., A. K. Murtazaev, and Rashid A. Murtazaliev. "Influence of Quenched Nonmagnetic Impurities on Phase Transitions in Two-Dimensional 3-State Antiferromagnetic Potts Model on Triangular Lattice." Solid State Phenomena 233-234 (July 2015): 79–81. http://dx.doi.org/10.4028/www.scientific.net/ssp.233-234.79.

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An influence of quenched nonmagnetic disorder on the phase transitions in the two dimensional antiferromagnetic Potts model with a number of spin state q=3 on a triangular lattice is calculated by the Monte-Carlo method. The systems with linear sizes L=20÷144 at spin concentrations p=1.00, 0.90, 0.80 are studied. By means of the fourth order Binder cumulant method, the inclusion of a quenched disorder as nonmagnetic impurities into a pure antiferromagnetic Potts model is shown to be the cause of the change of the first order phase transition into the second one.

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Books on the topic "Two Dimensional Triangular Lattice Antiferromagnetic AgFeO2"

1

Staples, I. Application of the coupled cluster method to the two dimensional triangular lattice frustrated spin-1/2 system with an antiferromagnetic Heisenberg Hamiltonian. Manchester: UMIST, 1994.

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