Solving for $\hat{A}\psi(x)=\psi(x+b)$

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Homework Help Overview

The discussion revolves around the operator \(\hat{A} = \exp\left(b \frac{d}{dx}\right)\) and its application to a function \(\psi(x)\), specifically showing that \(\hat{A}\psi(x) = \psi(x+b)\). The subject area includes differential operators and series expansions in calculus.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the meaning of the operator and its exponential notation, with one participant expressing confusion about the operator's definition. Suggestions include considering an infinitesimal change to understand the operator's effect better.

Discussion Status

The discussion is ongoing, with participants providing insights into the series expansion of operators and the implications for the function \(\psi(x)\). There is an acknowledgment of the complexity of operator notation, and some participants are beginning to grasp the connection between the operator and the resulting function transformation.

Contextual Notes

One participant notes difficulty with the operator basics and notation, indicating a potential gap in foundational understanding that may affect their ability to engage with the problem fully.

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Homework Statement



Given operator [tex]\hat{A}=exp({b}\frac{d}{dx})[/tex] where b is a constant, show that:

[tex]\hat{A}\psi(x)=\psi(x+b)[/tex]

Homework Equations


The Attempt at a Solution



I have no idea with this one. If I understand correctly the operator, A, says take the derivative of (something) with respect to x, multiply the result by b, and then exponentiate it. A pointer would be much appreciated here.
 
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It's usually a good idea to consider an infinitesimal change first and then deduce the result for a finite change.
 
You haven't quite gotten the meaning of the exponential notation correct, which is why you're confused :wink: A function of an operator is defined by its series expansion,
[tex]f(\hat{D}) = f_0 + f_1 \hat{D} + f_2 \hat{D}^2 + \cdots[/tex]
Typically the function f is one that can be expanded in a Maclaurin series (Taylor series around 0), so in that case the coefficients [itex]f_n[/itex] are just the same coefficients that appear in the Maclaurin series:
[tex]f_n = \frac{1}{n!}f^{(n)}(0)[/tex]
For the exponential function, the series is
[tex]e^x = 1 + x + \frac{x^2}{2} + \cdots[/tex]
so the operator [tex]e^{\hat{D}}[/tex] is defined as
[tex]e^{\hat{D}} = 1 + \hat{D} + \frac{\hat{D}^2}{2} + \cdots[/tex]
In your case, [itex]\hat{D}[/itex] is multiplication by a constant composed with the derivative operator [itex]\mathrm{d}/\mathrm{d}x[/itex], so the notation [itex]\hat{D}^n[/itex] is effectively telling you to take the n'th derivative and then multiply by [itex]b^n[/itex]. This would of course be applied to whatever the operator is acting on - for example, in
[tex]e^{b\mathrm{d}/\mathrm{d}x}\psi(x)[/tex]
each term would be produced by differentiating ψ(x) some number of times and then multiplying by b that many times.
 
Oh I see! Thank you both for responding. Interesting that it yields the series expansion for psi of (x+b). Learning operator basics and notation is turning out harder than I expected.
 

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