Applying Heisenberg picture to density operator

In summary, the conversation revolves around the application of the Heisenberg picture to the density operator of a particle evolving from point A to point B. The initial state of the particle is represented by the density operator and a selecting operator is used to extract the element of the density operator at a particular point. However, there is a debate over whether the concept of an evolving basis is valid in the Heisenberg picture and it is argued that the quantum state remains constant in this picture.
  • #1
Haorong Wu
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TL;DR Summary
How density operator evolves in the Heisenberg picture?
Suppose that a particle evolves from point A to point B. The state of the particle can be written as $$\rho=\sum \left | m\right >\rho_{mn}\left< n\right | .$$ Because the basis is evolving as the particle travels, I am considering applying the Heisenberg picture to the density operator.

Let the initial state of the particle be $$\rho_0=\sum \left | m,0\right >\rho^0_{mn}\left< n,0\right |,$$ and the selecting operator at ##z## be $$\left |n,z \right > \left <m,z \right | $$. Then the element of ##\rho## at ##z## could be extracted as $$\rho(z)_{mn}=tr(\rho_0 \left |n,z \right > \left <m,z \right |)= \sum_{m'n'}\left <m,z \right | \left | m',0\right >\rho^0_{m'n'}\left< n',0\right | \left |n,z \right > . $$

I am not sure whether this is correct or not. The density operator after all is not a state vector.
 
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  • #2
The Hilbert space does not evolve in either the Schroedinger or Heisenberg pictures. There is no concept of evolving basis. The basis is something you are always free to choose, and is purely a matter of convenience.

The quantum state (ie, the state vector or density operator) is constant in the Heisenberg picture.
 
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  • #3
atyy said:
The Hilbert space does not evolve in either the Schroedinger or Heisenberg pictures. There is no concept of evolving basis. The basis is something you are always free to choose, and is purely a matter of convenience.

The quantum state (ie, the state vector or density operator) is constant in the Heisenberg picture.
Thanks! I will reconsider it.
 

1. How does the Heisenberg picture differ from the Schrödinger picture?

The Heisenberg picture is a different way of looking at quantum mechanics compared to the more commonly known Schrödinger picture. In the Heisenberg picture, the operators are time-independent while the states are time-dependent, whereas in the Schrödinger picture, it is the opposite. This means that in the Heisenberg picture, the operators are the same at all times, making it easier to study the time evolution of a system.

2. What is the purpose of applying the Heisenberg picture to the density operator?

The density operator, also known as the density matrix, is a mathematical tool used to describe the state of a quantum system. By applying the Heisenberg picture to the density operator, we can study the time evolution of the system and make predictions about its future state. This is particularly useful in situations where the system is interacting with its environment and its state is constantly changing.

3. Can the Heisenberg picture be applied to any quantum system?

Yes, the Heisenberg picture can be applied to any quantum system, as long as it is described by a Hamiltonian. The Hamiltonian is a mathematical operator that represents the total energy of the system and is used to calculate the time evolution of the system in the Heisenberg picture.

4. What are the advantages of using the Heisenberg picture?

One of the main advantages of using the Heisenberg picture is that it simplifies the calculations involved in studying the time evolution of a quantum system. This is because the operators are time-independent, making it easier to analyze the system's behavior over time. Additionally, the Heisenberg picture is particularly useful for systems that are constantly changing, such as those interacting with their environment.

5. Are there any limitations to using the Heisenberg picture?

While the Heisenberg picture is a powerful tool for studying quantum systems, it does have some limitations. One of the main limitations is that it only works for systems described by a Hamiltonian. This means that it cannot be applied to systems that are not in equilibrium or are constantly changing, such as systems undergoing phase transitions. Additionally, the Heisenberg picture can only be used for systems that are described by a finite number of degrees of freedom.

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