Graduate Study Chern-Simons Invariant: Understanding 3-Manifold Measurement

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The Chern-Simons (CS) invariant of a 3-manifold serves as a crucial topological invariant, indicating how the curvature of the manifold deviates from constancy. It is computed as the integral of the Chern-Simons 3-form over the manifold, which is linked to the curvature and defined through a principal G-bundle connection. This invariant is significant because it remains unchanged regardless of the metric or coordinate choices, highlighting its topological nature. The CS invariant provides valuable insights into the topology of 3-manifolds, particularly in relation to the Witten-Reshetikhin-Turaev (WRT) invariant through the volume conjecture. Understanding the CS invariant enhances the study of 3-manifold properties and their geometric characteristics.
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I've been studying the Witten-Reshetikhin-Turaev (WRT) invariant of 3-manifolds but have almost zero background in physics. The WRT of a 3-manifold is closely related to the Chern-Simons (CS) invariant via the volume conjecture. My question is, what does the CS invariant of a 3-manifold measure? I mean, if it's an invariant then it must give you some information about the manifold, right?
 
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The Chern-Simons (CS) invariant of a 3-manifold is an important topological invariant that measures the extent to which the curvature of a given 3-manifold deviates from being constant across the manifold. Specifically, it measures the integral of the "Chern-Simons 3-form" over the 3-manifold. This 3-form is related to the curvature of the 3-manifold and is defined using the connection of a principal G-bundle on the 3-manifold. The CS invariant is interesting in that it is a topological invariant of the 3-manifold, meaning that it is independent of the metric or any other choice of coordinates. This makes it useful for studying the topology of 3-manifolds.
 
Time reversal invariant Hamiltonians must satisfy ##[H,\Theta]=0## where ##\Theta## is time reversal operator. However, in some texts (for example see Many-body Quantum Theory in Condensed Matter Physics an introduction, HENRIK BRUUS and KARSTEN FLENSBERG, Corrected version: 14 January 2016, section 7.1.4) the time reversal invariant condition is introduced as ##H=H^*##. How these two conditions are identical?

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