Answering "How to Understand Approximation in QM

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Homework Help Overview

The discussion revolves around understanding an approximation in quantum mechanics, specifically related to the harmonic oscillator as presented in Griffiths' . The original poster seeks clarification on the meaning of an approximation in a series expansion that leads to the expression for the exponential function.

Discussion Character

  • Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants explore the relationship between the series expansion and the exponential function, questioning the nature of the approximation. Some participants attempt to clarify the exactness of the series when summed from zero to infinity, while others discuss the implications of Taylor series and their derivatives.

Discussion Status

The discussion is active, with participants providing insights into the Taylor series and its application to the problem. Some have expressed satisfaction in resolving their initial confusion regarding the equality of the series and the exponential function, while others continue to explore the implications of the approximation.

Contextual Notes

There is a focus on the Taylor series and its terms, with participants noting the significance of zero terms in the expansion. The original poster's desire to avoid approximations indicates a constraint in their understanding that is being addressed through the discussion.

Tspirit
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Homework Statement


In the Griffiths book <Introduction to QM>, Section 2.3.2: Analytic method (for The harmonic oscillator), there is an equation (##\xi## is very large)
$$h(\xi)\approx C\sum\frac{1}{(j/2)!}\xi^{j}\approx C\sum\frac{1}{(j)!}\xi^{2j}\approx Ce^{\xi^{2}}.$$
How to understand the meaning of the third approximately equal sign?

Homework Equations


I know the Taylor series
$$e^{x}=\frac{x^{n}}{n!}$$

The Attempt at a Solution


If take place of ##\xi## with ##2\xi##, the equation may hold. However, can it be like this? What is the series of ##e^{\xi^{2}}## in real? I don't want the approximation. Thank you.
 
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If the sum runs from j=0 to infinity, it is not an approximation, it is exact. It is the Taylor series of ##e^x## with ##x=\xi^2##.

Note that ##\xi^{2j} = (\xi^2)^j##.
 
mfb said:
If the sum runs from j=0 to infinity, it is not an approximation, it is exact. It is the Taylor series of ##e^x## with ##x=\xi^2##.

Note that ##\xi^{2j} = (\xi^2)^j##.
Thank you! I have found the problem I met. In fact, I want to prove the following equation $$e^{x^{2}}=\sum\frac{x^{2n}}{n!},$$ but didn't succeed at first. Now I can. This is the process.
Adopting the Taylor expansion of the left, with the derivertives
$$ (e^{x^{2}})^{(0)}=e^{x^{2}},(e^{x^{2}})^{(1)}=e^{x^{2}}2x,(e^{x^{2}})^{(2)}=e^{x^{2}}(4x^{2}+2),(e^{x^{2}})^{(3)}=e^{x^{2}}(8x^{3}+12x),(e^{x^{2}})^{(4)}=e^{x^{2}}(16x^{4}+48x^{2}+12) ...,$$
$$e^{x^{2}}=1+0+2x^{2}/{2!}+0+12x^{4}/{4!}+...,$$ which is exactly equal to the right expression $$1+x^2/(1!)+x^4/(2!).$$
Actually, the zero terms in the Taylor expansion stopped me from calculating continuously in the beginning, making me think they are not equal.
 
That is more complicated, but it works as well.
 
Tspirit said:
Thank you! I have found the problem I met. In fact, I want to prove the following equation $$e^{x^{2}}=\sum\frac{x^{2n}}{n!},$$ but didn't succeed at first. Now I can. This is the process.
Adopting the Taylor expansion of the left, with the derivertives
$$ (e^{x^{2}})^{(0)}=e^{x^{2}},(e^{x^{2}})^{(1)}=e^{x^{2}}2x,(e^{x^{2}})^{(2)}=e^{x^{2}}(4x^{2}+2),(e^{x^{2}})^{(3)}=e^{x^{2}}(8x^{3}+12x),(e^{x^{2}})^{(4)}=e^{x^{2}}(16x^{4}+48x^{2}+12) ...,$$
$$e^{x^{2}}=1+0+2x^{2}/{2!}+0+12x^{4}/{4!}+...,$$ which is exactly equal to the right expression $$1+x^2/(1!)+x^4/(2!).$$
Actually, the zero terms in the Taylor expansion stopped me from calculating continuously in the beginning, making me think they are not equal.

You could simply let ##y = x^2##, then:

##e^y = \sum\frac{y^{n}}{n!}##

And

##e^{x^2} = \sum\frac{(x^2)^{n}}{n!} = \sum\frac{x^{2n}}{n!}##

In fact, you don't really need to introduce the intermediate variable ##y##. You can simply write down this last equation directly.
 
PeroK said:
You could simply let ##y = x^2##, then:

##e^y = \sum\frac{y^{n}}{n!}##

And

##e^{x^2} = \sum\frac{(x^2)^{n}}{n!} = \sum\frac{x^{2n}}{n!}##

In fact, you don't really need to introduce the intermediate variable ##y##. You can simply write down this last equation directly.
Indeed, it's a simpler method.
 

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