Can someone explain what a propagator is and does?

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A propagator is a mathematical tool used in quantum mechanics to describe the evolution of quantum states over time, specifically from an initial time t1 to a final time t2. It allows for the calculation of the probability amplitude of finding a system in a particular state at a later time. The discussion references Shankar's book and suggests that Sakurai's text provides clear explanations of the non-relativistic propagator. The propagator can be expressed in various equivalent forms, emphasizing its role in unitary evolution within the framework of Hilbert space. Understanding the propagator is essential for grasping the dynamics of quantum systems.
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So, Shankar in his famous book started to use the propagator a bunch of times in his Simple Problems in One Dimension chapter, and I have been confused to what it is and does.
 
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zheng89120 said:
So, Shankar in his famous book started to use the propagator a bunch of times in his Simple Problems in One Dimension chapter, and I have been confused to what it is and does.

A propagator propagates :biggrin:, for instance a quantum state from time t1 to time t2.
 
I recommend Sakurai's book for some nice descriptive views on the non-relativistic propagator.

Starting from the abstract Hilbert space formalism, it may be helpful to write down a few equivalent expressions for the propagator: <x'|U(t2-t1)|x> = <x'|U+(t2)U(t1)|x> = <ψ'(t2)|ψ(t1)>

So you take a state |x>, let it evolve unitarily from initial time t1 to final time t2 and ask "what's the probability (amplitude) to find it in state |x'>".
 
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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