Maximum position expectation value for 1D harmonic oscillator

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Homework Help Overview

The discussion revolves around maximizing the expectation value of position \(\langle x \rangle\) for a one-dimensional harmonic oscillator by determining a linear combination of the states \(|0\rangle\) and \(|1\rangle\). Participants are exploring the implications of their calculations and the methods available for optimization.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the calculation of \(\langle \alpha | x | \alpha \rangle\) and question the correctness of their expressions. The use of the Lagrange multiplier method is suggested for maximizing the expectation value. There are inquiries about the implications of different sets of coefficients and how to determine which is appropriate.

Discussion Status

The conversation is active, with participants providing corrections and suggestions for further exploration. Some have shared their own attempts and results, while others are questioning the validity of their approaches. There is no explicit consensus on the best method, but various lines of reasoning are being examined.

Contextual Notes

Participants are constrained by homework rules that limit the use of wave functions and require adherence to normalization conditions. The discussion also reflects a variety of interpretations regarding the maximization problem and the nature of the solutions derived.

AwesomeTrains
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Hey, I'm stuck halfway through the solution it seems. I could use some tips on how to continue.

1. Homework Statement

I have to determine a linear combination of the states |0\rangle, |1\rangle, of a one dimensional harmonic oscillator, so that the expectation value \langle x \rangle is a maximum.

Homework Equations


x=\sqrt{\frac{\hbar}{2m\omega}}(a+a^\dagger)

The Attempt at a Solution


I set |\alpha \rangle\equiv c_1|1\rangle + c_2|0\rangle
Then I calculate \langle \alpha | x | \alpha \rangle = \sqrt{\frac{\hbar}{2m\omega}} (c_1^*\langle1| + c_2^*\langle 0|)(a+a^\dagger)(c_1|1\rangle + c_2|0\rangle)=\sqrt{\frac{\hbar}{2m\omega}}[c_1^*(c_1+c_2)+c_2^*c_2] = \sqrt{\frac{\hbar}{2m\omega}}[1+c_1^*c_2]
I get the last equation because of the normalization condition:
c_1^*c_1+c_2^*c_2=1
This is where I don't know how to continue. Is this even the right approach?
(I'm not allowed to use the wave functions.)

Anything is appreciated.

Kind regards
Alex
 
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You should recheck your calculation of ##\langle \alpha \lvert x \rvert \alpha \rangle##. The ##c_i^*c_i## terms shouldn't be there.
 
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As for the maximization problem, the Lagrange multiplier method may be helpful.
 
Thanks for the fast reply.
I've corrected my calculation, is this right?:
First I calculate (a+a^\dagger)|\alpha\rangle
a(c_1|1\rangle+c_2|0\rangle)=c_1|0\rangle+0c_2|0\rangle=c_1|0\rangle
and
a^\dagger(c_1|1\rangle+c_2|0\rangle)=c_1\sqrt{2}|2\rangle+c_2|1\rangle

Then because |\alpha\rangle^\dagger = c_1^*\langle1|+c_2^*\langle0|
\langle\alpha|(a+a^\dagger)|\alpha\rangle=c_1^*\langle1|(c_1\sqrt{2}|2\rangle+c_2|1\rangle+c_1|0\rangle)+c_2^*\langle0|(c_1\sqrt{2}|2\rangle+c_2|1\rangle+c_1|0\rangle)= c_1^*c_2+c_2^*c_1
Do I use the lagrange multiplier method here? Or how do I continue?
 
The Lagrange multiplier is used for finding the maximum value of <x>.
 
So It's like a function of 4 variables f(c_1,c_1^*, c_2,c_2^*)=c_1^*c_2+c_2^*c_1 which I have to maximize under the condition c_1^*c_1+c_2^*c_2=1
Or is there an easier solution?
 
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Hello! I Have the same exercise in my homework. Using the Lagrange multiplier I get ##c_{1}=c_{2}=1/\sqrt{2}##. Is that right?
 
AwesomeTrains said:
So It's like a function of 4 variables f(c_1,c_1^*, c_2,c_2^*)=c_1^*c_2+c_2^*c_1 which I have to maximize under the condition c_1^*c_1+c_2^*c_2=1
Or is there an easier solution?
Yes, it is.
Mikhail_MR said:
Hello! I Have the same exercise in my homework. Using the Lagrange multiplier I get ##c_{1}=c_{2}=1/\sqrt{2}##. Is that right?
Whether it's true or not, you can do some kind of examination. For example, you can write ##\langle \hat{x} \rangle \propto |c_1||c_2| \cos{(\phi_1-\phi_2)}## where the ##\phi##'s are the angle of each coefficients, since we want to maximize our expectation value, it's necessary that ##\phi_1=\phi_2##.
 
Last edited:
Thanks for advise, blue_leaf77. I have made my calculation new.
I get 4 different sets of values.
##c_{1}=c_{2} = i/\sqrt{2}##
##c_{1}=c_{2} = -i/\sqrt{2}##
##c_{1}=i/\sqrt{2}; c_{2} = -i/\sqrt{2}##
##c_{1}=-i/\sqrt{2}; c_{2} = i/\sqrt{2}##

Using your advise how to examine solutions only the first and the second solutions are of interest. I can get this result on another way just inserting values in ##f## and finding a maximum. My question is: how i decide which set is right (the first or the second)?
 
  • #10
Mikhail_MR said:
Thanks for advise, blue_leaf77. I have made my calculation new.
I get 4 different sets of values.
##c_{1}=c_{2} = i/\sqrt{2}##
##c_{1}=c_{2} = -i/\sqrt{2}##
##c_{1}=i/\sqrt{2}; c_{2} = -i/\sqrt{2}##
##c_{1}=-i/\sqrt{2}; c_{2} = i/\sqrt{2}##
Well as long as ##\phi_1 = \phi_2## is satisfied, any ##\phi_1## is possible.
Mikhail_MR said:
how i decide which set is right (the first or the second)?
In the original question posted by the OP, he is asked to calculate the maximum of ##\langle \hat{x} \rangle##. In your case, I don't know what you are asked to do in your own homework.
 
  • #11
I have to calculate the maximum of ##\langle \hat{x} \rangle## too
 
  • #12
blue_leaf77 said:
Well as long as ##\phi_1 = \phi_2## is satisfied, any ##\phi_1## is possible.
You have this freedom.
 
  • #13
Mikhail_MR said:
Thanks for advise, blue_leaf77. I have made my calculation new.
I get 4 different sets of values.
##c_{1}=c_{2} = i/\sqrt{2}##
##c_{1}=c_{2} = -i/\sqrt{2}##

Using your advise how to examine solutions only the first and the second solutions are of interest. I can get this result on another way just inserting values in ##f## and finding a maximum. My question is: how i decide which set is right (the first or the second)?
Your first solution corresponds to the state
$$\lvert \alpha_1 \rangle = i\left(\frac {1}{\sqrt{2}} \lvert 0 \rangle + \frac{1}{\sqrt{2}} \lvert 1 \rangle\right) = e^{i\frac {\pi}{2}}\left(\frac {1}{\sqrt{2}} \lvert 0 \rangle + \frac{1}{\sqrt{2}} \lvert 1 \rangle\right),$$ and your second solution to
$$\lvert \alpha_2 \rangle = -i\left(\frac {1}{\sqrt{2}} \lvert 0 \rangle + \frac{1}{\sqrt{2}} \lvert 1 \rangle\right) = e^{-i\frac {\pi}{2}}\left(\frac {1}{\sqrt{2}} \lvert 0 \rangle + \frac{1}{\sqrt{2}} \lvert 1 \rangle\right).$$ The two states differ only by an overall phase factor, so…
 
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