Interplay of Spin and Spatial Anisotropy in Low-Dimensional Quantum Magnets with Spin 1/2

Quantum Heisenberg chain and square lattices are important paradigms of a low-dimensional magnetism. Their ground states are determined by the strength of quantum fluctuations. Correspondingly, the ground state of a rectangular lattice interpolates between the spin liquid and the ordered collinear N...

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Main Authors: Alžbeta Orendáčová, Róbert Tarasenko, Vladimír Tkáč, Erik Čižmár, Martin Orendáč, Alexander Feher
Format: Article
Language:English
Published: MDPI AG 2018-12-01
Series:Crystals
Subjects:
Online Access:http://www.mdpi.com/2073-4352/9/1/6
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author Alžbeta Orendáčová
Róbert Tarasenko
Vladimír Tkáč
Erik Čižmár
Martin Orendáč
Alexander Feher
author_facet Alžbeta Orendáčová
Róbert Tarasenko
Vladimír Tkáč
Erik Čižmár
Martin Orendáč
Alexander Feher
author_sort Alžbeta Orendáčová
collection DOAJ
description Quantum Heisenberg chain and square lattices are important paradigms of a low-dimensional magnetism. Their ground states are determined by the strength of quantum fluctuations. Correspondingly, the ground state of a rectangular lattice interpolates between the spin liquid and the ordered collinear Néel state with the partially reduced order parameter. The diversity of additional exchange interactions offers variety of quantum models derived from the aforementioned paradigms. Besides the spatial anisotropy of the exchange coupling, controlling the lattice dimensionality and ground-state properties, the spin anisotropy (intrinsic or induced by the magnetic field) represents another important effect disturbing a rotational symmetry of the spin system. The S = 1/2 easy-axis and easy-plane XXZ models on the square lattice even for extremely weak spin anisotropies undergo Heisenberg-Ising and Heisenberg-XY crossovers, respectively, acting as precursors to the onset of the finite-temperature phase transitions within the two-dimensional Ising universality class (for the easy axis anisotropy) and a topological Berezinskii–Kosterlitz–Thouless phase transition (for the easy-plane anisotropy). Experimental realizations of the S = 1/2 two-dimensional XXZ models in bulk quantum magnets appeared only recently. Partial solutions of the problems associated with their experimental identifications are discussed and some possibilities of future investigations in quantum magnets on the square and rectangular lattice are outlined.
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spelling doaj.art-2ad9c67ce98f41e8ad6e49b849cef5c42022-12-22T02:55:21ZengMDPI AGCrystals2073-43522018-12-0191610.3390/cryst9010006cryst9010006Interplay of Spin and Spatial Anisotropy in Low-Dimensional Quantum Magnets with Spin 1/2Alžbeta Orendáčová0Róbert Tarasenko1Vladimír Tkáč2Erik Čižmár3Martin Orendáč4Alexander Feher5Institute of Physics, Faculty of Science, P.J. Šafárik University, Park Angelinum 9, 041 54 Košice, SlovakiaInstitute of Physics, Faculty of Science, P.J. Šafárik University, Park Angelinum 9, 041 54 Košice, SlovakiaInstitute of Physics, Faculty of Science, P.J. Šafárik University, Park Angelinum 9, 041 54 Košice, SlovakiaInstitute of Physics, Faculty of Science, P.J. Šafárik University, Park Angelinum 9, 041 54 Košice, SlovakiaInstitute of Physics, Faculty of Science, P.J. Šafárik University, Park Angelinum 9, 041 54 Košice, SlovakiaInstitute of Physics, Faculty of Science, P.J. Šafárik University, Park Angelinum 9, 041 54 Košice, SlovakiaQuantum Heisenberg chain and square lattices are important paradigms of a low-dimensional magnetism. Their ground states are determined by the strength of quantum fluctuations. Correspondingly, the ground state of a rectangular lattice interpolates between the spin liquid and the ordered collinear Néel state with the partially reduced order parameter. The diversity of additional exchange interactions offers variety of quantum models derived from the aforementioned paradigms. Besides the spatial anisotropy of the exchange coupling, controlling the lattice dimensionality and ground-state properties, the spin anisotropy (intrinsic or induced by the magnetic field) represents another important effect disturbing a rotational symmetry of the spin system. The S = 1/2 easy-axis and easy-plane XXZ models on the square lattice even for extremely weak spin anisotropies undergo Heisenberg-Ising and Heisenberg-XY crossovers, respectively, acting as precursors to the onset of the finite-temperature phase transitions within the two-dimensional Ising universality class (for the easy axis anisotropy) and a topological Berezinskii–Kosterlitz–Thouless phase transition (for the easy-plane anisotropy). Experimental realizations of the S = 1/2 two-dimensional XXZ models in bulk quantum magnets appeared only recently. Partial solutions of the problems associated with their experimental identifications are discussed and some possibilities of future investigations in quantum magnets on the square and rectangular lattice are outlined.http://www.mdpi.com/2073-4352/9/1/6HeisenbergS = 1/2 XXZ modelspin anisotropysquare latticechainrectangular latticeBerezinskii-Kosterlitz-Thouless phase transitionphase diagramquantum magnet
spellingShingle Alžbeta Orendáčová
Róbert Tarasenko
Vladimír Tkáč
Erik Čižmár
Martin Orendáč
Alexander Feher
Interplay of Spin and Spatial Anisotropy in Low-Dimensional Quantum Magnets with Spin 1/2
Crystals
Heisenberg
S = 1/2 XXZ model
spin anisotropy
square lattice
chain
rectangular lattice
Berezinskii-Kosterlitz-Thouless phase transition
phase diagram
quantum magnet
title Interplay of Spin and Spatial Anisotropy in Low-Dimensional Quantum Magnets with Spin 1/2
title_full Interplay of Spin and Spatial Anisotropy in Low-Dimensional Quantum Magnets with Spin 1/2
title_fullStr Interplay of Spin and Spatial Anisotropy in Low-Dimensional Quantum Magnets with Spin 1/2
title_full_unstemmed Interplay of Spin and Spatial Anisotropy in Low-Dimensional Quantum Magnets with Spin 1/2
title_short Interplay of Spin and Spatial Anisotropy in Low-Dimensional Quantum Magnets with Spin 1/2
title_sort interplay of spin and spatial anisotropy in low dimensional quantum magnets with spin 1 2
topic Heisenberg
S = 1/2 XXZ model
spin anisotropy
square lattice
chain
rectangular lattice
Berezinskii-Kosterlitz-Thouless phase transition
phase diagram
quantum magnet
url http://www.mdpi.com/2073-4352/9/1/6
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AT erikcizmar interplayofspinandspatialanisotropyinlowdimensionalquantummagnetswithspin12
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