Are These Hermitian Conjugates Also Hermitian Operators?

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Homework Help Overview

The discussion revolves around determining the hermitian conjugates of specific operators in quantum mechanics, specifically the position operator (x) and momentum operator (p). The original poster presents three cases: xp, the commutator [x, p], and the sum xp + px, and seeks to establish whether these operators are hermitian.

Discussion Character

  • Conceptual clarification, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants explore the application of the hermitian condition and the use of integration by parts to manipulate operators. Questions arise regarding the correct method to bring operators into the appropriate form for analysis, particularly concerning the product rule and the implications of complex conjugation.

Discussion Status

Some participants express confusion about the requirements for demonstrating whether an operator is hermitian, leading to a variety of interpretations and approaches. There is acknowledgment that the operator xp is not hermitian, while others suggest that the sum xp + px is hermitian based on properties of operator products.

Contextual Notes

Participants note the complexity of handling the position and momentum operators, particularly in relation to their definitions and the implications of their non-commutativity. The discussion reflects an ongoing exploration of the mathematical properties of these operators without reaching a definitive conclusion.

xicor
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Homework Statement



Find the following hermitian conjugates and show if they are hermitian operators:

i) xp
ii) [x , p]
iii) xp + px

Where x is the position operator and p is the momentum operator.

Homework Equations



<f|Qg> = <Q^{t}f|g>
Q = Q^{t} Hermitian operator
p = -ih(d/dx)

The Attempt at a Solution



For the first case I have applied the condition of hermitian operators where I get <f|-ihx(dg(x)/dx)> and then get the form <f|-ih(dxg(x)/dx)>which leads to the integral ∫f*(-ih(d/dx)(xg(x)dx but am not sure how you bring the operator to f*. Do you just do the product rule and bring the product or to f* or do you need to do integration by part?

For the case of [x , p] you get [x, p] = -xih(d/dx) +ih(dx/dx) and find I apply this to the hermitian conjugate I get <-ihf|g> but was told something was wrong since I got it from <-xih(dg*/dx)+ih(g +x(dg/dx)>. For the third part I'm not getting anything that make sense when I apply -(xih(d/dx) + ih(dx/dx)) and got ∫f*(ih(g + 2x(dg/dx))dx but according to my notes xp + px should be hermitian.

Thanks to anybody that helps.
 
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Sorry, but I think I'm confused on what you have to even do for the hermitian conjugate. Do you even need to apply the <f|Qg) = <Q*f|g> to show the hermitian conjugate or do you just need to do the complex conjugate of the operator and if it isn't hermtian it will be something different when you apply <f|Qg) = <Q*f|g>?

For example, in the case of xp if I apply the complex conjugate I will get ihx(d/dx) instead of -ihx(d/dx) meaning it isn't a hermitian operator. When I applied the condition for hermitian conjugates and get <f|(-ihx(dg/dx)>, I then bring the brak-ket notation to the integral form ∫f*(-ihx(dg/dx)dx where -ihx can be brough to f in the form ∫(ihxf)*(dg/dx)dx where integration by parts is the process to bring the derivative to f. The problem I have here is with x since you then need to do the product rule for (ihxf)* where I get the result -∫(ihf - ihx(df/dx))gdx which can be changed into form -<ih(f - x(df/dx))|g> which is obviously not the same as the original form. Is this correct and the answer like that was produced under the brak-ket notation because xp isn't hermitian?
 
xicor said:
Sorry, but I think I'm confused on what you have to even do for the hermitian conjugate. Do you even need to apply the <f|Qg) = <Q*f|g> to show the hermitian conjugate or do you just need to do the complex conjugate of the operator and if it isn't hermtian it will be something different when you apply <f|Qg) = <Q*f|g>?

For example, in the case of xp if I apply the complex conjugate I will get ihx(d/dx) instead of -ihx(d/dx) meaning it isn't a hermitian operator. When I applied the condition for hermitian conjugates and get <f|(-ihx(dg/dx)>, I then bring the brak-ket notation to the integral form ∫f*(-ihx(dg/dx)dx where -ihx can be brough to f in the form ∫(ihxf)*(dg/dx)dx where integration by parts is the process to bring the derivative to f. The problem I have here is with x since you then need to do the product rule for (ihxf)* where I get the result -∫(ihf - ihx(df/dx))gdx which can be changed into form -<ih(f - x(df/dx))|g> which is obviously not the same as the original form. Is this correct and the answer like that was produced under the brak-ket notation because xp isn't hermitian?

Yes, xp isn't Hermitian. You use integration by parts to move the derivatives around and the x factor will block that. [x,p] should be easier, it's a constant but it's pure imaginary. For xp+px you can just deal on the abstract level with the operators. AB+BA is always hermitian no matter what the hermitian operators A and B are. Can you tell me why?
 
Last edited:
Alright, I think I understand now. If I apply a function to [x, p] I then find that [x, p]f = ihf so [x, p] = ih. When I apply this to the hermitian condition I get negative sign produced when I bring the i to the other function so [x, p] isn't hermitian.

For the case of xp +px if I consider it to be in form AB + BA, I can then use (AB)^{t} = B^{t}A^{t} meaning that (AB + BA)^{t} = B^{t}A^{t} + A^{t}B^{t} = BA + AB = BA +AB. This means that (xp + px)^{t} = (xp + px) so xp + px is a hermitian operator.
 
xicor said:
Alright, I think I understand now. If I apply a function to [x, p] I then find that [x, p]f = ihf so [x, p] = ih. When I apply this to the hermitian condition I get negative sign produced when I bring the i to the other function so [x, p] isn't hermitian.

For the case of xp +px if I consider it to be in form AB + BA, I can then use (AB)^{t} = B^{t}A^{t} meaning that (AB + BA)^{t} = B^{t}A^{t} + A^{t}B^{t} = BA + AB = BA +AB. This means that (xp + px)^{t} = (xp + px) so xp + px is a hermitian operator.

Yeah, that's it exactly.
 

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