In this article, we are going to address the issue of Topological entropy in physics from different perspectives with the aim of offering a comprehensive and complete vision of this matter. We will explore its history, its implications in today's society, the advances and challenges that have arisen around it, as well as the opinions of experts and opinion leaders on the subject. Topological entropy in physics is a topic that has generated great interest and debate in different areas, so it is crucial to delve into its understanding and analysis to have a broader and enriching vision of it. Through this article, we intend to offer a detailed and rigorous approach to Topological entropy in physics, with the intention of contributing to knowledge and reflection on this topic.
The topological entanglement entropy[1][2][3] or topological entropy, usually denoted by , is a number characterizing many-body states that possess topological order.
A non-zero topological entanglement entropy reflects the presence of long range quantum entanglements in a many-body quantum state. So the topological entanglement entropy links topological order with pattern of long range quantum entanglements.
Given a topologically ordered state, the topological entropy can be extracted from the asymptotic behavior of the Von Neumann entropy measuring the quantum entanglement between a spatial block and the rest of the system. The entanglement entropy of a simply connected region of boundary length L, within an infinite two-dimensional topologically ordered state, has the following form for large L:
where is the topological entanglement entropy.
The topological entanglement entropy is equal to the logarithm of the total quantum dimension of the quasiparticle excitations of the state.
For example, the simplest fractional quantum Hall states, the Laughlin states at filling fraction 1/m, have γ = ½log(m). The Z2 fractionalized states, such as topologically ordered states of Z2 spin-liquid, quantum dimer models on non-bipartite lattices, and Kitaev's toric code state, are characterized γ = log(2).