Is the Coth Approximation Correct for Large x in a QM Textbook?

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The discussion centers on the validity of the coth approximation for large x in quantum mechanics, specifically referencing an expression from a textbook by Newton. The approximation states that coth(x) is approximately equal to 1 + 2e^{-2x} for large x. The derivation involves rewriting coth(x) in terms of e^{-2x} and performing a power series expansion. The participants confirm that the approximation holds true under the conditions specified, particularly at low temperatures where the weighing factor is (1/E). The conclusion affirms the correctness of the approximation for large x in the context provided.
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In a QM textbook (Newton), I found the below expression for large x:

<br /> coth(x)\cong 1+2e^{-2x}<br />

I tried

<br /> coth(x)=\frac{e^{x}+e^{-x}}{e^{x}-e^{-x}}=\frac{1+e^{-2x}}{1-e^{-2x}}<br />
 
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Write z = e^{-2x}, so that z is small when x is large. Then,

\coth x = \left(1+z\right)\left(1-z\right)^{-1}.

Do a power series expansion of of this, or do a power series expansion of just \left(1-z\right)^{-1}.
 
Is it correct to do like this:
for large x; ex=1+ex.
So on mere substitution into the eqn.
<br /> coth(x)=\frac{e^{x}+e^{-x}}{e^{x}-e^{-x}}=\frac{1+e^{-2x}}{1-e^{-2x}}<br />
one will get
<br /> coth(x)\cong 1+2e^{-2x}<br />
at low temperature the weighing factor is (1/E).
<br /> x=E/(2k_{\rm B}T)<br />.
 
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