WebFeb 5, 2009 · Based on arbitrary short-range (e.g. nearest neighbor) integrable spin chains, it allows us to construct an infinite set of conserved long-range charges. We explain the moduli space of deformation parameters by different classes of generating operators. WebSpin chains in solid state materials are quintessential quantum systems with potential applications in spin-based logic, memory, quantum communication, and computation. A critical challenge is the experimental determination of spin lifetimes with the ultimate goal of …
[1812.11609] Spin chains for two-qubit teleportation
WebMar 1, 2024 · The spin-1/2 Heisenberg chain was the first quantum many-body Hamiltonian to be solved exactly by H. Bethe in 1931 [].This pioneer work led to the development of the Bethe ansatz for integrable one-dimensional models, of which the spin-1/2 Heisenberg model and its anisotropic extension, the XXZ chain, are notable examples [].In addition to … WebOct 10, 2016 · Spin chains are paradigmatic systems for the studies of quantum phases and phase transitions, and for quantum information applications, including quantum … how many calories is in totino\u0027s pizza
[2111.07927] Entanglement entropy in critical quantum spin …
WebMay 15, 1989 · Abstract. One-dimensional antiferromagnets have exotic disordered ground states. As was first argued by Haldane (1983), there is an excitation gap for integer, but not half-integer, spin. The authors review the arguments for this behaviour based on field-theory mappings, the Lieb-Schultz-Mattis theorem, exactly solvable models, finite-chain ... WebWe investigate dynamical stability of the ground state against a time-periodic and spatially-inhomogeneous magnetic field for finite quantum XXZ spin chains. We use the survival probability as a measure of stability and demonstrate that it decays as P ( t ) ∝ t −1/2 under a certain condition. The dynamical properties should also be related to the level statistics … WebNov 1, 2007 · First, let's take just one spin. There are two possible basis states, "up" and "down". Let the "up" state be represented by the column vector , and the "down" state by . Then the operators for that spin are Now, with two spins, the basis states are up-up, up-down, down-up, and down-down. high risk high reward investments reddit