Those Pictures (Representations) in QM and the density equations

In summary, the conversation is about the density equation in the Schrödinger picture and the use of different representations for calculating correlations. The speaker is having difficulty understanding these concepts and is seeking clarification. They also mention that expectation values can be converted between different pictures by rearranging the time evolution operator.
  • #1
Robert_G
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Hi there:

I am reading a book (Atom-Photon interaction by Claude Cohen-Tannoudji, Page 448) and the following things gave a big headache.

(1) Is there a density equation in Schrodinger Picture. because I encounter one, like:
##i \hbar \frac{d \sigma}{dt}=[\hat{H}, \sigma]##
and ##\hat{H}## contains the Hamiltonian of the atom, photon, and there interaction. So this is in Schrodinger Representations. right?

(2) The correlation ##\langle \mathscr{L}_+(\tau)\mathscr{L}_-(0)\rangle## is calculated step by step, from the equation in (1). So this is also in Schrodinger Representation. But the "double" correlation ##\langle \mathscr{L}_+(t)\mathscr{L}_+(t+\tau)\mathscr{L}_-(t+\tau)\mathscr{L}_-(t)\rangle## is in Heisenberg Representation, and this is clearly stated in the book, because, as the book said, the operators in that "double" correlation are in Heisenberg Representation. So those two correlations are from different Represetations?

Ps: ##\mathscr{L}_+## is the atomic upper operator, and ##\mathscr{L}_-## is the atomic lower operator.

HELP ME!
 
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  • #2
It's a rough journey to learn this things, oh, my brain.
 
  • #3
(1) Supposing that sigma is the density matrix, yes, you are using the Schrödinger picture

(2) Expectation values don't really specify which picture is being used. You can convert between pictures by rearranging the time evolution operator: <C(t)> = tr{σ C(t)} = tr{σ U(t)+CU(t)} = tr {U(t)σU+(t) C} = tr {σ(t) C} = <C>t
 
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1. What are "those pictures" in QM?

"Those pictures" refer to different mathematical representations or formulations of quantum mechanics, such as the Schrödinger picture, Heisenberg picture, and interaction picture. These pictures use different mathematical formalisms to describe the same physical system.

2. What is the significance of using different pictures in QM?

Each picture offers a different perspective on the same quantum system, making it easier to analyze and solve certain problems. For example, the Schrödinger picture is useful for studying the evolution of quantum states over time, while the Heisenberg picture is better suited for analyzing the time evolution of operators.

3. How do the density equations fit into these pictures?

The density equations, also known as the density matrix equations, are a way of representing the state of a quantum system in terms of probabilities. They can be used in any of the QM pictures, and provide a way to describe the evolution of a system that is not in a pure state.

4. What are the main differences between the pictures in QM?

The main differences between the pictures lie in their mathematical formalism and the quantities that are treated as constants or variables. In the Schrödinger picture, the state of the system is time-dependent, while in the Heisenberg picture, the operators are time-dependent. The interaction picture combines elements of both the Schrödinger and Heisenberg pictures.

5. Which picture is the most popular or widely used in QM?

There is no one "best" picture in QM, as each has its own advantages and applications. The choice of picture depends on the problem at hand and the preferences of the researcher. However, the Schrödinger picture is often used in introductory courses and the Heisenberg picture is commonly used in advanced research.

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