Show Lx is Hermitian: Homework Equation Integration

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In summary, the conversation discusses the task of showing that Lx (angular momentum) is Hermitian in 3-d space. The homework equations and attempt at a solution are provided, with the suggestion to use integration by parts. The conversation then focuses on determining what v is in the integration by parts process. Ultimately, the conclusion is reached that Lx is e.s.a. and its closure is s.a., making it a Hermitian operator.
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Homework Statement



I have to show that in 3-d, Lx (angular momentum) is Hermitian.

Homework Equations



In order to be Hermitian: Integral (f Lx g) = Integral (g Lx* f)
Where Lx=(hbar)/i (y d/dz - z d/dy)
and f and g are both well behaved functions: f(x,y,z) and g(x,y,z)

The Attempt at a Solution



I know to do this I have to do integration by parts. I got to the point where I had to figure out, using integration by parts,: Integral [f(x,y,z) y (dg(x,y,z)/dz) dx]

And I cannot figure this out :(

I set:
u=f(x,y,z) y
dv=(dg(x,y,z)/dz) dx

So then I get: du=[df(x,y,z)/dx]y + f(x,y,z)
But what is v then?? Unless I'm completely off-track already, in which case, help would be great!
 
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  • #2
You need to multiply by dx dy dz, and integrate over all three, not just dx. This should make the integration by parts much easier.
 
  • #3
As in...

u=f(x,y,z)y
dv=(dg(x,y,z)/dz) dxdydz

So that...

du = (df/dx)y + (df/dx)y + f + (df/dz)y
v=...?

Still not sure :(
 
  • #4
Focus on the z integral (because the derivative is with respect to z). So du = (df/dz)y.
 
  • #5
oh, and then v is just g(x,y,z)...
 
  • #6
Yep!
 
  • #7
great, thanks!
 
  • #8
Since L_{x} (or rather its closure in the strong topology of L^{2}(R^3)) generates a uniparametric subgroup of the group of unitary operators which represent a rotation (around an arbitrary axis) in a Hilbert space, then, by Stone's theorem, L_{x} is e.s.a. and its closure is s.a. But all e.s.a. operators are hermitian/symmetric. QED
 
  • #9
Yeah, that's what I *meant* to say ...
 

FAQ: Show Lx is Hermitian: Homework Equation Integration

What is a Hermitian operator?

A Hermitian operator is a type of linear operator in quantum mechanics that satisfies the property of being self-adjoint, which means that the operator is equal to its own adjoint. In other words, the operator and its adjoint have the same mathematical form.

How do you show that Lx is Hermitian?

To show that Lx is Hermitian, we need to prove that Lx is equal to its own adjoint, which is denoted as Lx†. This can be done by taking the integral of the inner product of Lx and a test function, and then showing that it is equal to the integral of the inner product of the adjoint of Lx and the same test function. If these two integrals are equal, then Lx is Hermitian.

What is the importance of Lx being Hermitian?

The fact that Lx is Hermitian is important because it guarantees that the eigenvalues of Lx are real numbers. This is a fundamental property of Hermitian operators and is crucial in many areas of physics, including quantum mechanics.

What is the significance of the Homework Equation in Lx being Hermitian?

The Homework Equation, also known as the Fundamental Theorem of Calculus, is used in the proof of Lx being Hermitian. It allows us to take the derivative of an integral, which is crucial in showing that the integral of the inner product of Lx and a test function is equal to the integral of the inner product of the adjoint of Lx and the same test function.

Can you provide an example of a Hermitian operator in quantum mechanics?

One example of a Hermitian operator in quantum mechanics is the position operator, which is denoted as x. This operator acts on a wavefunction to give the position of a particle in space. It is Hermitian because it satisfies the property of being self-adjoint, meaning x is equal to its own adjoint x†.

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