Related Experiment Video
Updated: Aug 11, 2026

06:42
Generation and Coherent Control of Pulsed Quantum Frequency Combs
Published on: June 8, 2018
Exact Fractionalized Ground States in an Extended Spin-1 Kitaev Chain
1Indian Institute of Technology Madras, Department of Physics, Chennai 600036, India.
Physical Review Letters
|August 10, 2026
Summary
We found exact solutions for a spin-1 chain using a Kitaev-like model. This reveals fractionalized spin-1/2 excitations and exponential ground-state degeneracy, inspired by the Affleck-Kennedy-Lieb-Tasaki model.
Area of Science:
- Condensed Matter Physics
- Quantum Many-Body Systems
- Spin Chains
Background:
- The Affleck-Kennedy-Lieb-Tasaki (AKLT) model provides a framework for exactly solvable spin chains.
- Kitaev-like models are crucial for understanding exotic quantum phases.
- Spin-1 chains exhibit complex behaviors relevant to magnetism and quantum computation.
Purpose of the Study:
- To present exact solutions for a spin-1 chain with Kitaev-like couplings.
- To explore an expanded Kitaev model incorporating bilinear and biquadratic terms.
- To investigate the nature of ground-state degeneracy and fractionalized excitations.
Main Methods:
- Reformulating the Hamiltonian as a sum of projection operators at an exactly solvable point.
- Projecting the component of spin along the bond direction, differing from the AKLT model's approach.
- Expressing ground states concisely using matrix product states.
Main Results:
- Achieved exact solutions for the spin-1 Kitaev-like model.
- Demonstrated exponential ground-state degeneracy through fractionalized spin-1/2 objects.
- Constructed a phase diagram by varying bilinear and biquadratic term strengths.
Conclusions:
- The fractionalized states offer a qualitative understanding of the spin-1 Kitaev model.
- Approximate forms for ground states and low-lying excitations were derived.
- This work provides insights into novel quantum phases in spin systems.
Related Concept Videos
Atomic Nuclei: Nuclear Spin State Overview
NMR-active nuclei have energy levels called 'spin states' that are associated with the orientations of their nuclear magnetic moments. In the absence of a magnetic field, the nuclear magnetic moments are randomly oriented, and the spin states are degenerate. When an external magnetic field is applied, the spin states have only 2 + 1 orientations available to them. A proton with = ½ has two available orientations. Similarly, for a quadrupolar nucleus with a nuclear spin value of one, the...
Atomic Nuclei: Nuclear Spin State Population Distribution
Near absolute zero temperatures, in the presence of a magnetic field, the majority of nuclei prefer the lower energy spin-up state to the higher energy spin-down state. As temperatures increase, the energy from thermal collisions distributes the spins more equally between the two states. The Boltzmann distribution equation gives the ratio of the number of spins predicted in the spin −½ (N−) and spin +½ (N+) states.
Spin–Spin Coupling Constant: Overview
In bromoethane, the three methyl protons are coupled to the two methylene protons that are three bonds away. In accordance with the n+1 rule, the signal from the methyl protons is split into three peaks with 1:2:1 relative intensities. The methylene protons appear as a quartet, with the relative intensities of 1:3:3:1.
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must have a...
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must have a...
Spin–Spin Coupling: One-Bond Coupling
Coupling interactions are strongest between NMR-active nuclei bonded to each other, where spin information can be transmitted directly through the pair of bonding electrons. While nuclei polarize their electrons to the opposite spins, the bonding electron pair has opposite spins. Configurations with antiparallel nuclear spins are expected to be lower in energy. When coupling makes antiparallel states more favorable, J is considered to have a positive value. The one-bond coupling constant, 1J,...
Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)
Two NMR-active nuclei bonded to a central atom can be involved in geminal or two-bond coupling. Geminal coupling is commonly seen between diastereotopic protons in chiral molecules and unsymmetrical alkenes, among others.
The central atom need not be NMR-active because its electrons are affected by the electron polarization of the spin-active atoms. However, spin information is transmitted less effectively than in one-bond coupling, and 2J values are usually weaker than 1J values. The energy of...
The central atom need not be NMR-active because its electrons are affected by the electron polarization of the spin-active atoms. However, spin information is transmitted less effectively than in one-bond coupling, and 2J values are usually weaker than 1J values. The energy of...
Valence Bond Theory
Coordination compounds and complexes exhibit different colors, geometries, and magnetic behavior, depending on the metal atom/ion and ligands from which they are composed. In an attempt to explain the bonding and structure of coordination complexes, Linus Pauling proposed the valence bond theory, or VBT, using the concepts of hybridization and the overlapping of the atomic orbitals. According to VBT, the central metal atom or ion (Lewis acid) hybridizes to provide empty orbitals of suitable...
