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Nanomagnetism is a rapidly expanding area of research which appears to be able to provide novel applications. Transmission line does not invalidate the scheme. Moreover, we show that possible noise on the Setting of its parameters demonstrates that fine tuning is not necessary as itĮxists an extended region in the parameters space that corresponds to anĮffective functioning. Thorough analysis of how the overall dynamical system operates depending on the Getting through to a single, localized qubit, and manipulate its state. Qubit, a permanent change in its spin state, thus realizing the possibility of Indeed cause, just passing by the spin-1/2 localized particle embodying the We finally demonstrate that the resulting magnetic pulse can Propose a method for injecting a soliton into the chain by acting just on one We then show that a Heisenberg spin chain can serve as transmission line, and Use, and briefly review the properties that make it apt to represent a signal. We first introduce the specific magnetic soliton of which we will make
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The nearby transit of a magnetic soliton, there conveyed through a transmission Particle, or `qubit', by means of a magnetic signal effectively generated by We propose a method for acting on the spin state of a spin-1/2 localized The robustness of solitons is demonstrated by considering cases where initial states are truncated versions of soliton states and by numerical simulations of the discrete EOM equations when the spins are coupled to a heat bath at finite temperatures.Ī family of wheel-shaped charge-neutral heterometallic (6). It is of special interest that our continuum EOM possesses soliton solutions, and we find that these characteristics are also exhibited by the corresponding solutions of the discrete EOM. The usefulness of the continuum EOM is demonstrated by the fact that the time-evolved numerical solutions of the discrete spin EOM closely track the corresponding time-evolved solutions of the continuum equation. This continuum EOM reduces to the Landau-Lifshitz equation in a particular limiting regime. Our approach is to utilize the solutions of a continuum version of the discrete spin equations of motion (EOM) which we derive by assuming continuous modulations of spin wave solutions of the EOM for discrete spins. We investigate the dynamical behavior of finite rings of classical spin vectors interacting via nearest-neighbor isotropic exchange in an external magnetic field.