Expectation Value and Probabilities of Spin Operator Sy

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Homework Help Overview

The discussion revolves around calculating the expectation value and probabilities associated with the spin operator \( S_y \) for a particle in a given spin state. The problem involves understanding the implications of the expectation value being negative and the normalization of the state vector.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants explore the calculation of the expectation value \( \langle S_y \rangle \) and the probabilities of measuring specific eigenvalues of the spin operator. There is discussion about the normalization of the state vector and its impact on the results. Questions are raised regarding the interpretation of a negative expectation value and the necessity of normalization in calculations.

Discussion Status

Participants have provided various calculations and insights into the normalization process, with some expressing confusion about the negative expectation value. There is an acknowledgment that the probabilities should sum to one, and discussions are ongoing about the implications of the results and the normalization of the state vector.

Contextual Notes

Some participants note that the original state vector provided in the problem is not normalized, which affects the calculations of probabilities. There is also mention of a reference example that does not normalize the state vector, leading to further questions about the necessity of normalization in this context.

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Homework Statement



(a) If a particle is in the spin state ## χ = 1/5 \begin{pmatrix}
i \\
3 \\
\end{pmatrix} ## , calculate the expectation value <Sy>(b) If you measured the observable Sy on the particle in spin state given in (a), what values might you get and what is the probability of each?

Homework Equations


(a)
<Sy> = expectation value
<Sy> = < χ | Sy | χ >

## Sy = ħ/2 \begin{pmatrix}
0 & -i \\
i & 0 \\
\end{pmatrix} ##

|χ> = ##1/5 \begin{pmatrix}
i \\
3 \\
\end{pmatrix} ##

< χ | = ##1/5 \begin{pmatrix}
-i & 3\\
\end{pmatrix} ##

(b)
C = < φ | χ >
C*C (where * = complex conjugate) = probability

The Attempt at a Solution


(a) <Sy> =
## 1/5 \begin{pmatrix}
-i & 3\\
\end{pmatrix}
ħ/2 \begin{pmatrix}
0 & -i \\
i & 0 \\
\end{pmatrix} 1/5 \begin{pmatrix}
i \\
3 \\
\end{pmatrix} ##

## = ħ/50 \begin{pmatrix}
-i & 3\\
\end{pmatrix}
\begin{pmatrix}
-3i \\
-1 \\
\end{pmatrix} ##

<Sy> ## = -6ħ/50 = -3ħ/25 ##

If the particle is in the spin state χ (given above) then the expectation value is = -3ħ/25. I don't understand how the expectation value can be negative though?

(b)
The Sy spin operator has two eigenspinors, corrosponding to two eigenvalues of ±ħ/2

i) For the eigenspinor with the positive eigenvalue of ħ/2

## | φ > = 1/√2 \begin{pmatrix}
1 \\
i \\
\end{pmatrix} ##

## < φ | = 1/√2 \begin{pmatrix}
1 & -i \\
\end{pmatrix} ##

C = ## < φ | χ > = 1/√2 \begin{pmatrix}
1 & -i \\
\end{pmatrix} 1/5 \begin{pmatrix}
i\\
3\\
\end{pmatrix} ##

= ## < φ | χ > = 1/5√2 \begin{pmatrix}
1 & i \\
\end{pmatrix} \begin{pmatrix}
i\\
3\\
\end{pmatrix} ##

C = ## < φ | χ > = 1/5√2 \begin{pmatrix}
-2i \\
\end{pmatrix} ##

## C * C = 1/50 (-2i)(2i) = 4/50 = 2/25 ##

The probability of measuring χ for Sy with the eigenvalue ħ/2 = 2/25

ii) For the eigenspinor with the negative eigenvalue of -ħ/2
## | φ > = 1/√2 \begin{pmatrix}
1 \\
-i \\
\end{pmatrix} ##

## < φ | = 1/√2 \begin{pmatrix}
1 & i \\
\end{pmatrix} ##

C = ## < φ | χ > = 1/√2 \begin{pmatrix}
1 & i \\
\end{pmatrix} 1/5 \begin{pmatrix}
i\\
3\\
\end{pmatrix} ##

C = ## < φ | χ > = 1/5√2 \begin{pmatrix}
-4i \\
\end{pmatrix} ##

## C * C = 1/50 (-4i)(4i) = 16/50 = 8/25 ##

The probability of measuring χ for Sy with the eigenvalue -ħ/2 = 8/25

I think I've answered part (b) correctly, it's just the negative expectation value I'm a bit confused about.
 
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says said:
(a) If a particle is in the spin state ## χ = 1/5 \begin{pmatrix}
i \\
3 \\
\end{pmatrix} ## , calculate the expectation value <Sy>
Is this state vector normalized? Do your results for the probabilities in part (b) add to 1? Should they?

I don't understand how the expectation value can be negative though?
Why does this bother you?

Your work looks good, but you are not getting the correct numerical values due to using a state vector that is not normalized.
 
The results for the probabilities don't add to 1, which I thought they should. I'm guessing they will add to one once I normalise χ.

I'm not entirely sure how to normalise χ though?
 
What does it mean for a state vector to be normalized?
 
## [ 1 / |A| ] * A ##

|A| = √(i2+32) = √ 8
|A| = √(-1+9) = √8

1/(5√8) ## \begin{pmatrix}
i \\
3 \\
\end{pmatrix} ##

Sorry, I posted that before I'd finished writing. I believe that is the normalised state vector though.
 
You need to replace the factor of 1/5 in the state |χ> by some other number, A, that normalizes the state. So, write the state as
|χ> = A ## \begin{pmatrix}
i \\
3 \\
\end{pmatrix} ##
where you need to determine a value of A that normalizes the state (<χ|χ> = 1). You can take A to be a real number.

Be careful in forming <χ|. What happens to the entry ##i## in going from |χ> to <χ|?
 
< χ | = A ## \begin{pmatrix}
- i & 3 \\
\end{pmatrix} ##

| χ > = A ## \begin{pmatrix}
i\\
3 \\
\end{pmatrix} ##

< χ | χ > = 1 ⇒ A=1/10
 
says said:
< χ | = A ## \begin{pmatrix}
- i & 3 \\
\end{pmatrix} ##
Yes, taking A to be real.

< χ | χ > = 1 ⇒ A=1/10
Almost. Note that A occurs in both < χ | and | χ >. Check your work.
 
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opps!

A= √(1/10)
 
  • #10
Right.
 
  • #11
C = < φ | ψ>
C*C

Ok, I re-calculated with the normalised state vector and got:

4/20 for the eigenspinor with the positive eigenvalue of ħ/2
16/20 for the eigenspinor with the negative eigenvalue of -ħ/2

*I haven't put in my working here just to save on formatting time

4/20 + 16/20 = 1

Question though relating to part (a)
1) why don't I have to use the normalised state vector to get the expectation value?
2) And how can the expectation value be negative? I thought we would always at the very least expect the value to be a positive integer
 
  • #12
says said:
4/20 for the eigenspinor with the positive eigenvalue of ħ/2
16/20 for the eigenspinor with the negative eigenvalue of -ħ/2
Looks right. Of course you can reduce these fractions.

Question though relating to part (a)
1) why don't I have to use the normalised state vector to get the expectation value?
You do need to used the normalized state. Or, you could use the more general formula for non-normalized states: ##\langle S_y \rangle = \frac {\langle \chi |S_y| \chi \rangle}{\langle \chi | \chi \rangle}##

2) And how can the expectation value be negative? I thought we would always at the very least expect the value to be a positive integer
Note that you have found that the probability of measuring ##-\hbar/2## is four times greater than the probability of getting ##+\hbar/2##. What does "expectation value" mean in terms of the probabilites?
 
  • #13
Ok, so I've re-calculated the expectation value with the normalised state vector.

## 1/√10 \begin{pmatrix}
-i & 3 \\
\end{pmatrix} *
ħ/2 \begin{pmatrix}
0 & -i \\
i & 0 \\
\end{pmatrix} *
1/√10 \begin{pmatrix}
i \\
3 \\
\end{pmatrix}
##

## = -6ħ/20 = -3ħ/10 ##

So that is the expectation value. Expectation value is the mean / average of all the results we would get. The probability in part (b) is four times greater for -ħ/2 and thus the expectation value should be more skewed towards being a negative number?
 
  • #14
I was following this Griffiths example to do this question. He doesn't normalise the state vector, which confuses me a bit in relation to my problem
 

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  • #15
The wavevector in Griffiths example is already normalized with the factor of 1/√6. It is a little odd that the vector that you are given in your problem has a factor of 1/5 (unless it is meant to test you on the idea of normalization :oldsmile:).
 
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  • #16
ok. Thanks for your help @TSny
 

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