Spin Gap And Susceptibility Of Spherical Kagome Cluster Mo72V30
- Theoretical study of spherical kagomé clusters in Mo72 V30 and W72 V30.
- Singlet ground state and spin gap in S = 1/2 Kagomé antiferromagnet.
- Title: Spin susceptibility anomaly in cluster Mott insulators on a.
- Muon spin relaxation and susceptibility studies of the pure and diluted.
- Vanishing spin gap in a competing spin-liquid phase in the kagome.
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- Evidence for a gapped spin-liquid ground state in a kagome... - AAAS.
- Magnetic susceptibility and spin dynamics of a polyoxovanadate cluster.
- Theoretical study of spherical kagomé clusters in Mo72... - OUP Academic.
- Spin cluster operator theory for the kagome lattice... - NASA/ADS.
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- Evidence for a gapped spin-liquid ground state in a kagome Heisenberg.
- [2112.07923] Effects of bond-randomness and Dzyaloshinskii-Moriya.
Theoretical study of spherical kagomé clusters in Mo72 V30 and W72 V30.
The kagome Heisenberg antiferromagnet formed by frustrated spins arranged in a lattice of corner-sharing triangles is a prime candidate for hosting a quantum spin liquid (QSL) ground state. The interplay between geometric frustration (GF) and bond disorder is studied in the Ising kagome lattice within a cluster approach. The model considers antiferromagnetic short-range couplings and long-range intercluster disordered interactions.... , potentializing the intercluster-disordered coupling and bringing the cluster spin-glass state. Using exact diagonalization for a 12-site kagome cluster, we analyzed the magnetic susceptibility and evaluated individual exchange interactions. The causes leading to the different ground states in Cs 2 Cu 3 SnF 12 and Rb 2 Cu 3 SnF 12 are discussed. Vanishing spin gap in a competing spin-liquid phase in the kagome Heisenberg antiferromagnet. ×.
Singlet ground state and spin gap in S = 1/2 Kagomé antiferromagnet.
The susceptibility indicates a Curie-Weiss temperature ofCW' 300K; however, no magnetic order is observed down to 50 mK. Inelastic neutron scattering reveals a spectrum of low energy spin excitations with no observable gap down to 0.1 meV. The specific heat at low-Tfollows a power law temperature dependence. Spin-1/2 spherical kagomé clusters, or quantum-spin icosidodecahedrons, occurring in Mo 72 V 30 and W 72 V 30 are analyzed using the Lanczos method. Magnetic susceptibility analysis reveals that, whereas Mo 72 V 30 contains some degree of structural distortion that decreases its spin gap, the structure of W 72 V 30 can be described as a regular (non-distorted) icosidodecahedron. 2 Laboratory for Muon Spin Spectroscopy, Paul Scherrer Insititut, 5232 Villigen PSI, Switzerland. 3 LPTMC, UMR 7600 of CNRS, UPMC, Paris-Sorbonne, F-75252 Paris Cedex 05, France. 4 School of Chemistry and EaStChem, University of St. Andrews, St. Andrews, Fife KY16 9ST, United Kingdom.
Title: Spin susceptibility anomaly in cluster Mott insulators on a.
Abstract: For the spherical kagome system {W 72 V 30 }, which is a magnetic cluster with 30 V 4+ ions, recent experimental and theoretical studies on the magnetization process at low temperatures have indicated that Dzyaloshinskii-Moriya interaction is an important ingredient in this material. Local spin susceptibility of the S = 1 2 kagome lattice in ZnCu 3 (OD) 6 Cl 2 Abstract We report a single-crystal 2D NMR investigation of the nearly ideal spin S= 1/2 kagome lattice ZnCu 3 (OD) 6 Cl 2. We successfully identify 2D NMR signals originating from the nearest neighbors of Cu 2+ defects occupying Zn sites.
Muon spin relaxation and susceptibility studies of the pure and diluted.
We present a comprehensive list of the ground-state energies and the spin gaps of finite Kagome clusters with up to 42 spins obtained using large-scale exact diagonalization techniques. This represents the current limit of this exact approach. For a fixed number of spins N, we study several cluster shapes under periodic boundary conditions in both directions resulting in a toroidal geometry. DOI: 10.1093/PTEP/PTU036 Corpus ID: 124590041. Theoretical study of spherical kagomé clusters in Mo72 V30 and W72 V30 @article{Kunisada2014TheoreticalSO, title={Theoretical study of spherical kagom{\'e} clusters in Mo72 V30 and W72 V30}, author={N. Kunisada and Y. Fukumoto}, journal={Progress of Theoretical and Experimental Physics}, year={2014}, volume={2014} }. Muon spin relaxation and magnetic susceptibility measurements have been performed on the pure and diluted spin 1/2 kagomé system (CuxZn(1-x))3V2O7(OH)2 2H2O. In the pure x=1 system we found a slowing down of Cu spin fluctuations with decreasing temperature towards T approximately 1 K, followed by slow and nearly temperature-independent spin.
Vanishing spin gap in a competing spin-liquid phase in the kagome.
Combined with the magnetic field dependence of χ kagome that we observed at low temperatures, these results imply that the kagome Heisenberg antiferromagnet has a spin-liquid ground state with a finite gap. The realization and characterization of a kagome Heisenberg antiferromagnet (KHA) with a corner-shared triangle structure ( Fig. 1A) is. Using the power law represented by 1/ ( a + bHα) with α = 0.46, where a and b depend on the fluctuation rate and fluctuating field, we obtain a good fitting to the LF dependence of the muon spin.
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Spin gap and ground state phase diagram 3. Magnetic susceptibility 4. Magnetization curve 5. Specific heat and entropy in the magnetic field 6. Integrated DOS and Raman intensity 7. Summary Acknowledgements References Next > Article Navigation Article Navigation Theoretical study of spherical kagomé clusters in Mo72V30and W72V30. The longest time to spin a basketball on one finger using one hand is 11 min 22.22 sec, achieved by Narayan Bhattarai (Nepal), at the Imadol Banquet, Mahalaxmi, Lalitpur, Nepal, on 8 May 2018. Narayan practiced for more than 15 months to break this record. All records listed on our website are current and up-to-date. Spin susceptibility anomaly in cluster Mott insulators on a partially-filled anisotropic Kagome lattice: applications to LiZn2Mo3O8 Item Preview.
Evidence for a gapped spin-liquid ground state in a kagome... - AAAS.
Thermodynamics of the spin-half square-kagome lattice antiferromagnet. Over the last decade, the interest in the spin- Heisenberg antiferromagnet (HAF) on the square-kagome (also called shuriken) lattice has been growing as a model system of quantum magnetism with a quantum paramagnetic ground state, flat-band physics near the saturation field.
Magnetic susceptibility and spin dynamics of a polyoxovanadate cluster.
Vanishing spin gap in a competing spin-liquid phase in the kagome Heisenberg antiferromagnet. Physical Review B, 2014. Yasir Iqbal. Download PDF. Download Full PDF Package. This paper. A short summary of this paper. 37 Full PDFs related to this paper. Read Paper. In condensed matter physics, a quantum spin liquid is a phase of matter that can be formed by interacting quantum spins in certain magnetic materials. Quantum spin liquids (QSL) are generally characterized by their long-range quantum entanglement, fractionalized excitations, and absence of ordinary magnetic order.. The quantum spin liquid state was first proposed by physicist Phil Anderson in.
Theoretical study of spherical kagomé clusters in Mo72... - OUP Academic.
Centred charge donor related diamagnetic susceptibility and optical properties of a spherical GaAs quantum dot are presented. In particular, effects of intrinsic parabolic and shifted parabolic potentials on these quantities are investigated. This is theoretically achieved by solving the Schrödinger equation within the effective mass approximation. It is observed that the parabolic potential.
Spin cluster operator theory for the kagome lattice... - NASA/ADS.
Spin Gap And Susceptibility Of Spherical Kagome Cluster Mo72V30. Door With Mail Slot For Sale Nyc. Best Spin Cycle App. The small spin gap of Mo70V30 can be interpreted to indicate the system in close proximity to the ferrimagnetic phase [13]. In 2009, Todae et al. synthesized W70V30 and measured its magnetic susceptibility [15]. This material was independently synthesized by Li et al., and they also carried out a high-energy Raman scattering experiment [16].
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Abstract: Motivated by recent experiments on the quantum-spin-liquid candidate material LiZn2Mo3O8, we study a single-band extended Hubbard model on an anisotropic Kagome lattice with the 1/6 electron filling. Due to the partial filling of the lattice, the inter-site repulsive interaction is necessary to generate Mott insulators, where electrons are localized in clusters, rather than at. The magnetic susceptibility for the ideal spherical kagome cluster, eq. (1) with Ji,j = J,by using the quantum Monte-Carlomethod. (In this case, the model has I. Title: Uniform spin susceptibility and spin-gap phenomenon in the BCS-BEC crossover regime of an ultracold Fermi gas. Authors: H. Tajima, T. Kashimura,... We also clarify how the spin-gap phenomenon is related to the pseudogap phenomenon appearing in the single-particle density of states. Our results indicate that an ultracold Fermi gas in the.
Evidence for a gapped spin-liquid ground state in a kagome Heisenberg.
We present a comprehensive list of ground state energies and spin gaps of finite kagome clusters with up to 42 spins obtained using large-scale exact... Skip to main content A line drawing of the Internet Archive headquarters building façade.... Ground-State Energy and Spin Gap of Spin-1/2 Kagome Heisenberg Antiferromagnetic Clusters: Large. For the spin-1/2 spherical kagomé cluster, as well as for the 2D kagomé lattice, many low-energy singlet excitations have been expected to exist in the energy region below the spin gap,... Global Survey. In just 3 minutes, help us better understand how you perceive arXiv.
[2112.07923] Effects of bond-randomness and Dzyaloshinskii-Moriya.
Phys. Rev. B 105, 024418 (2022) - Gapless spin liquid behavior in a kagome Heisenberg antiferromagnet with randomly distributed hexagons of alternate bonds Physical Review B Abstract We demonstrate that the single crystal of YCu3 [OH (D)]6.5Br2.5 (YCOB) is a kagome Heisenberg antiferromagnet without evident orphan spins ( ≪ 0.8 %).
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