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In condensed matter physics, the Kitaev chain is a simplified model for a topological superconductor. It models a one dimensional lattice featuring Majorana bound states . The Kitaev chain have been used as a toy model of semiconductor nanowires for the development of topological quantum computers .
This is a list of models and meshes commonly used in 3D computer graphics for testing and demonstrating rendering algorithms and visual effects. Their use is important for comparing results, similar to the way standard test images are used in image processing .
A model of the human skeleton as a kinematic chain allows positioning using forward and inverse kinematics. In mechanical engineering , a kinematic chain is an assembly of rigid bodies connected by joints to provide constrained motion that is the mathematical model for a mechanical system . [ 1 ]
In condensed matter physics, an AKLT model, also known as an Affleck-Kennedy-Lieb-Tasaki model is an extension of the one-dimensional quantum Heisenberg spin model.The proposal and exact solution of this model by Ian Affleck, Elliott H. Lieb, Tom Kennedy and Hal Tasaki [] [1] provided crucial insight into the physics of the spin-1 Heisenberg chain.
Linkages may be constructed from open chains, closed chains, or a combination of open and closed chains. Each link in a chain is connected by a joint to one or more other links. Thus, a kinematic chain can be modeled as a graph in which the links are paths and the joints are vertices, which is called a linkage graph.
The six-vertex model can be solved using the algebraic Bethe ansatz for the Heisenberg spin chain (Baxter 1982). The half-filled Hubbard model in the limit of strong repulsive interactions can be mapped onto a Heisenberg model with J < 0 {\displaystyle J<0} representing the strength of the superexchange interaction.