Solution to Show Relation of X, P with Representation of P=-ih/2π*∂/∂x +f(x)

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The discussion focuses on demonstrating the relationship between the position operator X and the momentum operator P, given the commutation relation [X, P] = ih/2π. The user attempts to derive the form of P, represented as P = -ih/2π * ∂/∂x + f(x), by applying the commutation relation to an arbitrary function g(x). They clarify that X is defined as x, and the challenge lies in incorporating the arbitrary function f(x) into their derivation. Ultimately, the goal is to show that P must take the specified form based on the given conditions. The conversation highlights the importance of understanding operator representations in quantum mechanics.
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Homework Statement


given that X(operator) and P (operator) operate on functions,and the relation [X,P]=ih/2π,show that if X(operator)=x ,and P (operator) has the representation P=-ih/2π*∂/∂x +f(x)
where f(x) is an arbitrary function of x


Homework Equations

quantum mechanic by Liboff



The Attempt at a Solution

I wrote the commutator relation of P and x on an arbitrary function like g(x) ,[x,p]g(x) so XP(g(x))-PX(g(x))=ih/2pi(g(x)) because of X=x so I wrote
xP(g(x))-P(xg(x))=xP(g(x))-xP(g(x))-g(x)Px=-g(x)Px=ih/2pi(g(x)) so I can derive just this part of equation-ih/2π*∂/∂x , what can I do for the part of f(x)?
 
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If I'm interpreting the question correctly, your not supposed to derive the commutation relation; it's actually a given. You are also told that X=x.What you don't know is what P is. You're supposed to show that given [X,P]=i \hbar and X=x that P must take the form -i \hbar \frac{d}{dx} +f(x)...to do this, just operate on a function g(x) by [x,P] while leaving P as an unknown operator...what do you get when you do that?
 
thanx now I get it!
 
I think I must derive that P is this form P=-ih/2π*∂/∂x +f(x)
 

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