Calculating Probability of Energy Measurement in Quantum Systems

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Homework Help Overview

The discussion revolves around calculating the probability of measuring a specific energy level, E_{1}, in a quantum system represented by the state |\psi\rangle. The original poster presents the state as a superposition of two normalized stationary states, |1\rangle and |2\rangle, and seeks guidance on how to approach the problem of normalization and probability calculation.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants discuss the need for normalization of the state |\psi\rangle and question how to derive the normalized form from the given superposition. There are attempts to express the normalization condition and calculate the probability of measuring E_{1} based on the squared magnitudes of the components of |\psi\rangle.

Discussion Status

The discussion is ongoing, with participants exploring different interpretations of normalization and its implications for calculating probabilities. Some guidance has been offered regarding the normalization of states, but there is no clear consensus on the correct approach or final expression for the probability.

Contextual Notes

Participants note the importance of normalization in quantum mechanics and express uncertainty about the proper application of this concept to the problem at hand. There is an indication that foundational knowledge may be lacking, as one participant suggests reviewing basic textbook material on the topic.

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Homework Statement



Quantum system in state |\psi\rangle. Energy of state measured at time t: Calculate probability that measurement will be E_{1}.

Homework Equations



|\psi\rangle=|1\rangle+i|2\rangle

|1\rangle is normalised stationary state with energy E_{1}. Similarly with 2.

The Attempt at a Solution



I have the time-dep Schrödinger equation for \psi as:

i \hbar \frac{\partial}{\partial t}|\psi \rangle = \hat{H}|\psi\rangle=E_{\psi}|\psi\rangle

.. but that's it.

I really don't know where to start with this :frown:
 
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First of all: To calculate probabilities you always need to normalize the states. While |1> and |2> are normalized by assumptions, what about |\psi>?
 
For normalisation of |\psi\rangle I calculated:

| |\psi\rangle |^{2}=\left(|1\rangle+i|2\rangle\right)\left(|1\rangle-i|2\rangle\right)=|1\rangle^{2}+|2\rangle^{2}
 
But what will be the normalized psi?
 
|\psi\rangle=E_{1}^{2}+E_{2}^{2} ?
 
I've still not understood this :frown:
 
You wrote:
1)
<br /> | |\psi\rangle |^{2}=\left(|1\rangle+i|2\rangle\right)\left(|1\rangle-i|2\rangle\right)=|1\rangle^{2}+|2\rangle^{2}<br />But before that:

2) |1> is normalised stationary state with ... Similarly with 2.

What can you do with 1) knowing 2)?
 
that..

| |\psi\rangle |^{2}=E_{1}^{2}+E_{2}^{2}

?
 
.. so

P(E_{1})=\frac{E_{1}^{2}}{E_{1}^{2}+E_{2}^{2}}

? or something like that
 
  • #10
So you did not read about normalization of states. And you should! That's bad!

Which is your basic textbook?
 

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