Understanding Quantum State Preparation: The Significance of |u> and |d> Vectors

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The discussion explains the preparation of quantum states, specifically focusing on the spin states represented by the ket-vectors |u> and |d>. When a measurement apparatus oriented along the z-axis registers +1, it indicates that the system is in the state |u>. This means that subsequent measurements will treat the system as if it is definitively in the |u> state. The preparation of the state |u> implies a consistent outcome for future observations. Understanding this concept is crucial for grasping quantum state preparation and measurement implications.
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"Let’s begin by labeling the possible spin states along the three coordinate axes. If A is oriented along the z axis, the two possible states that can be prepared correspond to σz= ±1. Let’s call them up and down and denote them by ket-vectors |u> and |d> . Thus, when the apparatus is oriented along the z axis and registers +1, the state |u> has been prepared. " says in The Theoritical Minimum

what it means ? In particular "the state |u> has been prepared" Actually I am asking just this part
 
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It means that the system is in state |u>,
$$
| \psi \rangle = | \mathrm{u} \rangle
$$
 
By saying that the state |u\rangle is prepared, one can assume that all subsequent measurements of that same system will be as though the system is in state |u\rangle.
 
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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