Difference between expectation value and eigenvalue

In summary: The expectation value is the average that we would find if we were to make perform our measurement on a large number of systems, all prepared in the same way.
  • #1
Sara Kennedy
18
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There is another topic for this but I didn't quite see it and I don't know how I've gone so far through my course not asking this simple question. So what's the difference?

My thought process for hydrogen. I know it can have quantised values of energy, the energy values are the Eigen values of the wave state. There can be multiple Eigen values, E, with a corresponding wave states, Ψ.
Which can be of the form HΨ=EΨ.

If I want to find the expectation value, <H> this will give me the value of E that is most likely to be found every time I repeat a measurement on the system? The value I get for <H> will not change, but the value of E in the other equation can change.

Is my thought process correct?
 
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  • #2
The expectation value is the average that we would find if we were to make perform our measurement on a large number of systems, all prepared in the same way. That is not the same thing as the value we are most likely to find and it is not necessarily an eigenvalue; the average family has 2.5 children, but you will never ever find a family with 2.5 children - the number of children will always be some integer.

Suppose the quantum state is ##\Psi=\alpha\psi_1+\beta\psi_2##. Here ##\psi_1## and ##\psi_2## are eigenfunctions of ##H## with the eigenvalues ##E_1## and ##E_2##, meaning that they are solutions of the time-independent Schrodinger equation ##H\psi=E\psi##: ##H\psi_1=E_1\psi_1## and ##H\psi_2=E_2\psi_2##.

##\Psi## is a solution of the time-dependent Schrodinger equation (which, strictly speaking, is the real Schrodinger equation) ##H\psi=E\psi## where ##E## is the energy operator ##i\hbar\frac{\partial}{\partial{t}}##. If we measure the energy of this system, we will get one of two answers: ##E_1## with probability ##|\alpha|^2## and ##E_2## with probability ##|\beta|^2##.

Now if we prepare a large number of systems in the state ##\Psi## and perform an energy measurement on each one, the average of all our measurements will come out to ##E_1|\alpha|^2+E_2|\beta|^2## - that's the expectation value.
 
  • #3
I read that a few times. Still clueless
 
  • #4
Sara Kennedy said:
My thought process for hydrogen. I know it can have quantised values of energy, the energy values are the Eigen values of the wave state. There can be multiple Eigen values, E, with a corresponding wave states, Ψ.
Which can be of the form HΨ=EΨ.

You must think about the wave function of the physical system which are solutions of the Schrodinger equation -
H operating on wave function giving E times the wave function -
In general the wave function is/can be expanded in a complete orthonormal set of possible eigen functions and expectation value is the result of a measurement which can be any state of the system
having any of the possible eigen state -not a particular one - each particular value has finite probability of its occurrence.
 
  • #5
Nugatory said:
Suppose the quantum state is ##\Psi=\alpha\psi_1+\beta\psi_2##. Here ##\psi_1## and ##\psi_2## are eigenfunctions of ##H## with the eigenvalues ##E_1## and ##E_2##, meaning that they are solutions of the time-independent Schrodinger equation ##H\psi=E\psi##: ##H\psi_1=E_1\psi_1## and ##H\psi_2=E_2\psi_2##.

##\Psi## is a solution of the time-dependent Schrodinger equation (which, strictly speaking, is the real Schrodinger equation) ##H\psi=E\psi## where ##E## is the energy operator ##i\hbar\frac{\partial}{\partial{t}}##. If we measure the energy of this system, we will get one of two answers: ##E_1## with probability ##|\alpha|^2## and ##E_2## with probability ##|\beta|^2##.

Now if we prepare a large number of systems in the state ##\Psi## and perform an energy measurement on each one, the average of all our measurements will come out to ##E_1|\alpha|^2+E_2|\beta|^2## - that's the expectation value.
Okay I see what you are saying now.

##E_1|\alpha|^2+E_2|\beta|^2##

So the expectation value is not actually going to be one of the values of E... say E1 or E2, but as you said... maybe 2.5 children. Its not the mode but the mean?
 
  • #6
Sara Kennedy said:
So the expectation value is not actually going to be one of the values of E... say E1 or E2, but as you said... maybe 2.5 children. Its not the mode but the mean?

Pretty much, yes.
 

1. What is an expectation value?

An expectation value is a mathematical concept in quantum mechanics that represents the average value of a physical quantity in a given state. It is calculated by taking the product of the probability of obtaining a certain measurement and the corresponding measurement itself, and then summing these values for all possible measurements.

2. What is an eigenvalue?

An eigenvalue is a value that represents the possible outcomes of a measurement for a specific physical quantity in a given state. It is a characteristic of the state and is determined by solving the Schrödinger equation. The corresponding eigenvector represents the state in which the measurement will result in that eigenvalue with certainty.

3. What is the difference between expectation value and eigenvalue?

The expectation value represents the average value of a physical quantity in a given state, while the eigenvalue represents the possible outcomes of a measurement for that physical quantity in the same state. In other words, the expectation value is a statistical concept while the eigenvalue is a specific measurement value.

4. Can the expectation value and eigenvalue be the same?

Yes, the expectation value and eigenvalue can be the same if the state is an eigenstate, meaning that the measurement of the physical quantity will always give the same result. In this case, the eigenvalue will also be the expectation value.

5. How are expectation value and eigenvalue used in quantum mechanics?

Expectation value and eigenvalue are used to describe the behavior of quantum systems and make predictions about the outcomes of measurements. They are essential in understanding the probabilistic nature of quantum mechanics and are used in various calculations and equations, such as the time evolution of a state and the uncertainty principle.

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