Magnetic Plateaus and Jumps in a Spin‐1/2 Ladder with Alternate Ising–Heisenberg Rungs: A Field‐Dependent Study

A frustrated two‐legged spin‐1/2 ladder featuring alternating Ising and isotropic Heisenberg exchange interactions on the rungs is investigated, while Ising exchanges are present along the legs and diagonals. This model exhibits the following four ground‐state phases: (i) stripe rung ferromagnet (SRFM), (ii) anisotropic antiferromagnet, (iii) dimer, and (iv) stripe leg ferromagnet. In this work, different magnetization plateaus are analyzed by studying the spin density, quantum fidelity, and quantum concurrence in the presence of longitudinal and transverse magnetic fields. The exact diagonalization and transfer matrix methods are used to solve the model Hamiltonian. In the presence of a longitudinal field, the discrete magnetization plateaus appear at 0, 1/2, and 1 of the saturation value across all phases [(i)–(iv)]. Interestingly, in the presence of an externally applied transverse field, the SRFM phase [(i)] exhibits a continuous change in magnetization. The other three phases [(ii)–(iv)] show both discrete jump and continuous change in magnetization in different limits of the transverse field.

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Publication Details

Journal
physica status solidi (b)
Published
2025-03-24
DOI
https://doi.org/10.1002/pssb.202500027
Citations
1
Primary Topic
Quantum many-body systems
Type
article
Field-Weighted Citation Impact
1.25

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article

Magnetic Plateaus and Jumps in a Spin‐1/2 Ladder with Alternate Ising–Heisenberg Rungs: A Field‐Dependent Study

Manoranjan Kumar, Shaon Sahoo, Sk Saniur Rahaman
1 citations
physica status solidi (b)
Quantum many-body systems
1.25
article

Magnetic Plateaus and Jumps in a Spin‐1/2 Ladder with Alternate Ising–Heisenberg Rungs: A Field‐Dependent Study

Manoranjan Kumar, Shaon Sahoo, Sk Saniur Rahaman
article en
1 citations

Abstract

A frustrated two‐legged spin‐1/2 ladder featuring alternating Ising and isotropic Heisenberg exchange interactions on the rungs is investigated, while Ising exchanges are present along the legs and diagonals. This model exhibits the following four ground‐state phases: (i) stripe rung ferromagnet (SRFM), (ii) anisotropic antiferromagnet, (iii) dimer, and (iv) stripe leg ferromagnet. In this work, different magnetization plateaus are analyzed by studying the spin density, quantum fidelity, and quantum concurrence in the presence of longitudinal and transverse magnetic fields. The exact diagonalization and transfer matrix methods are used to solve the model Hamiltonian. In the presence of a longitudinal field, the discrete magnetization plateaus appear at 0, 1/2, and 1 of the saturation value across all phases [(i)–(iv)]. Interestingly, in the presence of an externally applied transverse field, the SRFM phase [(i)] exhibits a continuous change in magnetization. The other three phases [(ii)–(iv)] show both discrete jump and continuous change in magnetization in different limits of the transverse field.

physica status solidi (b)Vol. 262(9)
Indian Institute of Technology Tirupati (IN), S.N. Bose National Centre for Basic Sciences (IN)
Science and Engineering Research Board
Openalex Percentile: Top 23%
Quantum many-body systems
1.25
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