Prove that any Hermitian operator is linear

In summary, the student is struggling with trying to solve a homework equation. They are at a loss as to how to even get started. They have been given a definition of a hermitian operator, but do not know how to get from the equation int(f*A*g*dx)=int(g*A*f*dx) to the final step where A[f+g]=Af+Ag. They explain that if they can prove that A(f+g)-(Af+Ag) = 0 for all functions f and g and all scalars c, they will have completed the task. They state that they can do this by expanding the left-hand side and using the fact that A is her
  • #1
Pchemaaah
15
0

Homework Statement


Simply--Prove that any Hermitian operator is linear

Homework Equations


Hermitian operator defined by: int(f(x)*A*g(x)dx)=int(g(x)*A*f(x)dx)

Linear operator defined by: A[f(x)+g(x)]=Af(x)+Ag(x)

Where A is an operator

The Attempt at a Solution



I am at a complete loss of how to even start this. I know I need to get from int(f(x)*A*g(x)dx)=int(g(x)*A*f(x)dx) to A[f(x)+g(x)]=Af(x)+Ag(x) where A is the Hermitian operator, but I don't know how/what to manipulate to get here...
 
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  • #2
For future reference, it's helpful if you actually post the definitions you're given. Usually the word "operator" means a linear operator, so a Hermitian operator would be linear by definition. From what you posted, I take it when you say A is Hermitian, then you mean A is defined on some space of functions, and [itex]\int f \overline{(Ag)} = \int (Af) \overline{g}[/itex], where the bar denotes complex conjugation and the integral presumably will always make sense.

Anyway, define <f,g> to be [itex]\int f\overline{g}[/itex]. So we have that <Af,g>=<f,Ag>. Consider

[tex]\langle A(f+\lambda g) - (Af + \lambda Ag), A(f+\lambda g) - (Af + \lambda Ag) \rangle.[/tex]
 
  • #3
morphism said:
For future reference, it's helpful if you actually post the definitions you're given. Usually the word "operator" means a linear operator, so a Hermitian operator would be linear by definition. From what you posted, I take it when you say A is Hermitian, then you mean A is defined on some space of functions, and [itex]\int f \overline{(Ag)} = \int (Af) \overline{g}[/itex], where the bar denotes complex conjugation and the integral presumably will always make sense.

Anyway, define <f,g> to be [itex]\int f\overline{g}[/itex]. So we have that <Af,g>=<f,Ag>. Consider

[tex]\langle A(f+\lambda g) - (Af + \lambda Ag), A(f+\lambda g) - (Af + \lambda Ag) \rangle.[/tex]

Thank you for the response and sorry I did not explicity post the definitions.

I understand that you defined A to be hermitian as demonstrated by your first set where <Af,g>=<f,Ag>, but I have no idea what the second part means. What is lambda? Why is the same thing on both sides and why did you choose to subtract (Af + \lambda Ag)?
 
  • #4
Lambda is just some scalar. We want to prove that A(f + cg) = Af+cAg, or written differently, A(f+cg) - (Af+cAg) = 0, for all functions f and g and all scalars c.

If you're familiar with inner/dot products you'll know why I did what I did: if <v,v>=0 then v=0.
 
  • #5
My class isn't using dot products or anything like that to do anything. We have just been mired in calculus with little to no instruction on how to use it.

Why do you want to involve a scalar? Is it possible to show this without using dot products/other 3D tools?
 
  • #6
I didn't read the whole thing, but it looks like lambda is just an arbitrary complex number. When you see someone put the same thing on both sides of the scalar product, it's usually because they want to use that [itex]\langle f|f\rangle \geq 0[/itex] for arbtrary non-zero f.

Edit: Much too slow :frown:
 
  • #7
We want to involve a scalar because we want to prove that A is linear - remember, this means that A(cg) = cAg for all scalars c, as well as A(f+g)=Af+Ag.

And you don't really need any 3D tools - I was just using them to guide my intuition.

For now let's ignore the scalar and focus on proving that A(f+g)-(Af+Ag)=0.

If we can prove that

[tex]\int (A(f+g)-(Af+Ag)) \overline{(A(f+g)-(Af+Ag))} = \int |A(f+g)-(Af+Ag)|^2 = 0[/itex]

then this will do the job (why?). To accomplish this, expand the left-hand side, and use the fact that A is Hermitian.
 
  • #8
I guess what I mean is that seems really arbitrary to pick what you did and I do not understand why/how you would come to pick that since my class has solely been working with integrals etc and hasnt even touched vectors/dot products.

Edit--I am sorry but my level of understanding is really low. How did you synthesize that integral?

And I also apologize but with my level of math I am unsure with what to do to the left side. I know it looks like I am begging for an answer, but I literally am lost in this class since it assumes we know a level of math that wasnt required to take it. How does the complex conjugate effect how it expands it and how can that be simplified any further?
 
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  • #9
Yes, I guess it does look like I'm pulling a rabbit out of a hat if you don't know what dot products are. It's strange that your class is discussing Hermitian operators without mentioning anything about dot products.
 
  • #10
Pchemaaah said:
Linear operator defined by: A[f(x)+g(x)]=Af(x)+Ag(x)
This is wrong, or at least incomplete. It should be A[af+bg]=aAf+bAg, where a and b are arbitrary complex numbers and f and g are arbitrary functions. (I'm in a nitpicking mood, so I'll also point out that it's wrong to write f(x) instead of f here, since f(x) is a number and f is a function).

Pchemaaah said:
Hermitian operator defined by: int(f(x)*A*g(x)dx)=int(g(x)*A*f(x)dx)
I would write it as <f,Ag>=<A*f,g>, where <f,g> is defined as [itex]\int f(x)^*g(x)dx[/itex], but you can keep expressing it as an integral if you want to.
 
  • #11
Fredrik said:
This is wrong, or at least incomplete. It should be A[af+bg]=aAf+bAg, where a and b are arbitrary complex numbers and f and g are arbitrary functions. (I'm in a nitpicking mood, so I'll also point out that it's wrong to write f(x) instead of f here, since f(x) is a number and f is a function).


I would write it as <f,Ag>=<A*f,g>, where <f,g> is defined as [itex]\int f(x)^*g(x)dx[/itex], but you can keep expressing it as an integral if you want to.

Like I said, we haven't addressed how this applies to space, only in paper/calculus form so I don't know any better. And I am pretty far removed from the realm of proper math expression (over 3 yrs since I took any math class) so forgive me for these technical errors.
 
  • #12
morphism said:
We want to involve a scalar because we want to prove that A is linear - remember, this means that A(cg) = cAg for all scalars c, as well as A(f+g)=Af+Ag.

And you don't really need any 3D tools - I was just using them to guide my intuition.

For now let's ignore the scalar and focus on proving that A(f+g)-(Af+Ag)=0.

If we can prove that

[tex]\int (A(f+g)-(Af+Ag)) \overline{(A(f+g)-(Af+Ag))} = \int |A(f+g)-(Af+Ag)|^2 = 0[/itex]

then this will do the job (why?). To accomplish this, expand the left-hand side, and use the fact that A is Hermitian.

So does that mean that [tex]\int (A(f+g)-(Af+Ag)) \overline{(A(f+g)-(Af+Ag))} = \int |A(f+g)-(Af+Ag)|^2 = 0[/itex] becomes [tex]\int (A(f+g)-(Af+Ag)) \overline{(A(f+g)-(A(f+g)} = \int |A(f+g)-(Af+Ag)|^2 = 0[/itex]
[tex]\int (A(f+g)-(Af+Ag)) \overline{(0))} = \int |A(f+g)-(Af+Ag)|^2 = 0[/itex]

Since if A is linear it follows that Af+Ag=A(f+g)? Isnt this approaching the question backwards though, because now I assuming it is linear and showing it is Hermitian instead of the other way around.
 
  • #13
You're not supposed to use the linearity. You're supposed to show that the left hand side (or the right-hand side, since it's the same thing) is =0 without using the linearity. This would prove that A(f+g)=Af+Ag.

The calculation is a bit awkward when we have to manipulate the integrals instead of abstract scalar products. I'm going to show you how I would prove the linearity using the abstract notation and the properties of a scalar product. Mostly because I'm really bored right now. This isn't a complete solution to your homework problem, since if you do it this way, you would have to prove that the "scalar product" defined using the integrals really is a scalar product, and do a few more things to have a complete proof.

[tex]\langle f,A(ag+bh)\rangle =\langle A^*f,ag+bh\rangle =a\langle A^*f,g\rangle+b\langle A^*f,h\rangle[/tex]

[tex]=a\langle f,Ag\rangle+b\langle f,Ah\rangle =\langle f,aAg+bAh\rangle[/tex]

This proves the linearity if the following is true: If <x,y>=<x,z> for all x, then y=z. You can prove that as an excercise if you want. If you don't feel like doing it this way, don't worry about it. The method that morphism suggested is fine too.
 
  • #14
Hmm without using that linearity equation then I would look for something to expand or factor to see if I can get some sort of cancellation, but since we are working with operators that strategy doesn't work out. I think there might be some way to split the left side integral apart based on the Hermiticty of A, but I don't see how/where since A is always near both f and g and they can't seem to separate.
 
  • #15
The idea is to use the Hermiticity of the operator to rewrite the expression so that you can use the linearity of the integral (or scalar product). Example:

[tex]\int\overline{A(f+g)}A(f+g) =\int\overline{A^*A(f+g)}(f+g) =\int\overline{A^*A(f+g)}f+\int\overline{A^*A(f+g)}g[/tex]

[tex]=\int\overline{A(f+g)}Af+\int\overline{A(f+g)}Ag =\int\overline{A(f+g)}(Af+Ag)[/tex]

Now rewrite this as

[tex]=\overline{\int\overline{(Af+Ag)}A(f+g)}[/tex]

and repeat the same procedure to get

[tex]\cdots=\overline{\int\overline{(Af+Ag)}(Af+Ag)} =\int\overline{(Af+Ag)}(Af+Ag)[/tex]

The calculation is pretty long. One of the reasons is that this method proves that <A(f+g),A(f+g)>=0 instead of separately proving that <h,A(f+g)>=<h,Af+Ag> for all h and that this implies that A(f+g)=Af+Ag. Morphism came up with a trick to do it all at once, but it makes the calculations longer. So you might want to stick with the method I used in #13 and just figure out how to express it using integrals.
 

Related to Prove that any Hermitian operator is linear

1. What is a Hermitian operator?

A Hermitian operator is a type of linear operator that is commonly used in quantum mechanics. It is a mathematical object that represents an observable quantity, such as energy or position, in a quantum system. It is named after the mathematician Charles Hermite.

2. How do you prove that a Hermitian operator is linear?

To prove that a Hermitian operator is linear, you must show that it satisfies the properties of linearity. This means that it must satisfy the conditions of additivity, homogeneity, and the preservation of scalar multiplication. These properties ensure that the operator behaves consistently and predictably when applied to different inputs.

3. What is the significance of proving that a Hermitian operator is linear?

Proving that a Hermitian operator is linear is important because it allows us to use mathematical techniques and tools, such as linear algebra, to analyze and understand quantum systems. It also allows us to make predictions about the behavior of these systems and make calculations that can be experimentally tested.

4. Can you give an example of a Hermitian operator?

One example of a Hermitian operator is the position operator, which represents the position of a particle in space. Another example is the energy operator, which represents the energy of a quantum system. These operators are used in the Schrödinger equation, one of the fundamental equations of quantum mechanics.

5. Are all Hermitian operators linear?

Yes, all Hermitian operators are linear. This is because the definition of a Hermitian operator includes the requirement that it must be a linear operator. Therefore, any operator that is not linear cannot be considered a Hermitian operator.

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