Determining Eigenfunction of Operator

Click For Summary

Homework Help Overview

The discussion revolves around determining the constant \( c \) such that the function \( \psi_{c}(x,y,z) = x^{2}+cy^{2} \) is an eigenfunction of the operator \( \hat{L_{z}} \). The operator is defined as \( \hat{L_{z}} = -i \hbar (x\frac{\partial \psi}{\partial y} - y\frac{\partial \psi}{\partial x}) \).

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the application of the operator to the function and the resulting expressions. There are attempts to clarify notation and calculations, with some participants questioning the correctness of the derived expressions and the implications of setting \( \lambda = 0 \).

Discussion Status

The discussion includes various attempts to manipulate the expressions derived from applying the operator. Some participants suggest that if \( \lambda = 0 \), the equation simplifies, leading to a potential value for \( c \). Others explore whether \( c \) can take on multiple values and what that means for the eigenfunction condition.

Contextual Notes

There are indications of confusion regarding the calculations and the role of \( c \) in the eigenvalue equation. Participants are also examining the implications of different values of \( c \) on the eigenfunction status of \( \psi_{c} \).

Hart
Messages
168
Reaction score
0

Homework Statement



Determing the constant c such that [tex]\psi_{c}(x,y,z) = x^{2}+cy^{2}[/tex] is an eigenfunction of [tex]\hat{L_{z}}[/tex]

Homework Equations



[tex]\hat{L_{z}} = -i \hbar (x\frac{\partial \psi}{\partial y} - y\frac{\partial \psi}{\partial x}[/tex]

The Attempt at a Solution



[tex]x\frac{\partial \psi}{\partial y} - y\frac{\partial \psi}{\partial x}) = 2x^{2}-2y^{2}c[/tex]

Therefore:

[tex]\hat{L_{z}} \psi = -i \hbar (2x^{2}-2y^{2}c) = -2i \hbar (x^{2}-y^{2}c)[/tex]

.. and now I'm stuck. :|
 
Physics news on Phys.org
Hart said:

Homework Statement



Determing the constant c such that [tex]\psi_{c}(x,y,z) = x^{2}+cy^{2}[/tex] is an eigenfunction of [tex]\hat{L_{z}}[/tex]

Homework Equations



[tex]\hat{L_{z}} = -i \hbar (x\frac{\partial \psi}{\partial y} - y\frac{\partial \psi}{\partial x})[/tex]

You need to pay more attention to your notation. You can either say,

[tex]\hat{L_{z}}\psi(x,y,z)= -i \hbar \left(x\frac{\partial \psi}{\partial y} - y\frac{\partial \psi}{\partial x}\right)[/tex]

or

[tex]\hat{L_{z}} \longrightarrow -i \hbar \left(x\frac{\partial}{\partial y} - y\frac{\partial}{\partial x}\right)[/tex]

But you can't equate an abstract differential operator to a scalar function like you did above

[tex]x\frac{\partial \psi}{\partial y} - y\frac{\partial \psi}{\partial x} = 2x^{2}-2y^{2}c[/tex]

You need to double check this. :wink:
 
I was meant to state this:

[tex]\hat{L_{z}}\psi(x,y,z)= -i \hbar \left(x\frac{\partial \psi}{\partial y} - y\frac{\partial \psi}{\partial x}\right)= -i \hbar (2x^{2}-2y^{2}c) = -2i \hbar (x^{2}-y^{2}c)[/tex]

[/tex]

I don't know how to rearrange that the find the value of C.
 
Hart said:
I was meant to state this:

[tex]\hat{L_{z}}\psi(x,y,z)= -i \hbar \left(x\frac{\partial \psi}{\partial y} - y\frac{\partial \psi}{\partial x}\right)= -i \hbar (2x^{2}-2y^{2}c) = -2i \hbar (x^{2}-y^{2}c)[/tex]

I don't know how to rearrange that the find the value of C.

[tex]\left(x\frac{\partial \psi}{\partial y} - y\frac{\partial \psi}{\partial x}\right)\neq (2x^{2}-2y^{2}c)[/tex]

Recheck your calculation.
 
I have:

[tex] <br /> (x\frac{\partial \psi}{\partial y}) = x(2cy) = 2cxy<br /> [/tex]

and:

[tex] <br /> (y\frac{\partial \psi}{\partial x}) = y(2x + c) = 2cxy<br /> [/tex]

so:

[tex] <br /> \hat{L_{z}}\psi(x,y,z)<br /> <br /> = -i \hbar \left(x\frac{\partial \psi}{\partial y} - y\frac{\partial \psi}{\partial x}\right)<br /> <br /> = -i \hbar (2cxy - 2cxy)<br /> <br /> = 0<br /> [/tex]

?
 
Hart said:
[tex] <br /> (y\frac{\partial \psi}{\partial x}) = y(2x + c) = 2cxy<br /> [/tex]

Where's the [itex]c[/itex] in this part coming from?

[tex]\frac{\partial\psi}{\partial x}=\frac{\partial}{\partial x}\left(x^2+cy^2\right)=2x[/itex][/tex]
 
It should be:

[tex](y\frac{\partial \psi}{\partial x}) = y(2x + 0) = 2xy[/tex]

then.

Ok, so:

[tex]\hat{L_{z}}\psi(x,y,z)= -i \hbar \left(x\frac{\partial \psi}{\partial y} - y\frac{\partial \psi}{\partial x}\right)= -i \hbar (2cxy - 2xy)= -2i \hbar xy(c-1)[/tex] ??
 
Hart said:
Ok, so:

[tex]\hat{L_{z}}\psi(x,y,z)= -i \hbar \left(x\frac{\partial \psi}{\partial y} - y\frac{\partial \psi}{\partial x}\right)= -i \hbar (2cxy - 2xy)= -2i \hbar xy(c-1)[/tex] ??

Yup, so if [itex]\psi[/itex] is an eigenfunction of [tex]\hat{L}_z[/itex], what equation must be true?[/tex]
 
[tex]\lambda = \frac{-2i \hbar xy(c-1)}{x^{2}+cy^{2}}?[/tex]
 
  • #10
Hart said:
[tex]\lambda = \frac{-2i \hbar xy(c-1)}{x^{2}+cy^{2}}?[/tex]

Sure, but I'd write this as

[tex]\lambda\left(x^2+cy^2\right)=-2i \hbar xy(c-1)[/itex]<br /> <br /> At first, it may not look like there are any values of [itex]c[/itex] that will make this true for all [itex]x[/itex] and [itex]y[/itex], but what if [itex]\lambda=0[/itex]?[/tex]
 
  • #11
[tex]\lambda\left(\psi_{c}\right)=-2i \hbar xy(c-1)[/tex]

It would be true if [tex]\lambda = 0[/tex]?
 
  • #12
Hart said:
[tex]\lambda\left(\psi_{c}\right)=-2i \hbar xy(c-1)[/tex]

It would be true if [tex]\lambda = 0[/tex]?

You tell me...if [itex]\lambda=0[/itex] what does that equation become? Are there any values of [itex]c[/itex] that make that equation true?
 
  • #13
[tex]\lambda\left(\psi_{c}\right)=-2i \hbar x y (c-1) = -2i \hbar x y c + 2i \hbar x y[/tex]

[tex]0 = -2i \hbar x y c + 2i \hbar x y[/tex]

[tex]2i \hbar x y c = 2i \hbar x y[/tex]

[tex]c = 1<br /> [/tex]
 
  • #14
Right, so for c=1, [itex]\psi[/itex] is an eigenfunction of [itex]\hat{L}_z[/itex] with corresponding eigenvalue [itex]\lambda=0[/itex].

If [itex]\lambda\neq 0[/itex] are there any values of [itex]c[/itex] which satisfy the eigenvalue equation for all [itex]x[/itex] and [itex]y[/itex]?
 
  • #15
Um.. c can be any integer value? it's just a scaling value.
 
  • #16
Hart said:
Um.. c can be any integer value? it's just a scaling value.

So, you are telling me that [itex]\lambda\left(x^2+cy^2\right)=-2i \hbar xy(c-1)[/itex] is satisfied for any integer value of [itex]c[/itex]?
 

Similar threads

  • · Replies 10 ·
Replies
10
Views
3K
  • · Replies 5 ·
Replies
5
Views
3K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 19 ·
Replies
19
Views
4K
Replies
24
Views
3K
Replies
2
Views
2K
  • · Replies 3 ·
Replies
3
Views
2K
Replies
11
Views
2K
  • · Replies 13 ·
Replies
13
Views
6K
  • · Replies 1 ·
Replies
1
Views
2K