A What is the Vector Manipulation Formula for Elastic Scattering Angle?

JD_PM
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I was reading *Introduction to Nuclear Physics* by Krane and stumbled on the following (page 47):

In Elastic scattering, the initial electron wave function is of the form ##e^{i k_i r}## (free particle of momentum ##p_i = \hbar k_i##). The scattered electron can also be regarded as a free particle of momentum ##p_f = \hbar k_f## and wave function ##e^{i k_f r}##.

The interaction ##V(r)## converts the initial wave into the scattered wave; the probability for the transition will be proportional to the square of the following quantity:

$$F(q) = \int V(r) e^{iqr}dv$$

Plugging both Coulomb's potential and charge-per-unit-volume into ##F(q)##:

$$F(q) = \int e^{iqr'} \rho(r') dv'$$

Normalizing and knowing that ##\rho(r')## just depends on ##r'## (and not on ##\theta'## nor ##\phi'##) we get:

$$F(q) = \frac{4\pi}{q}\int r' sin (qr') \rho(r') dr'$$

Where ##q = k_i - k_f##. The scattering is elastic, so momentum is conserved (##p_i = p_f##) and ##q## is merely a function of the scattering angle ##\alpha## between ##p_i## and ##p_f##.

**Now a bit of vector manipulation shows:**

$$q = \frac{2p}{\hbar}sin(\frac{\alpha}{2})$$

**I do not know how to get the last expression**
 
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Using ##| \mathbf{k}_i | = |\mathbf{k}_f| = k##, calculate ##q^2##:
$$
\begin{align*}
q^2 &= (\mathbf{k}_i - \mathbf{k}_f)^2 \\
&= k^2 - 2 \mathbf{k}_i \cdot \mathbf{k}_f - k^2 \\
&= 2 k^2 (1 - \cos \alpha) \\
&= 4 k^2 \sin^2 (\alpha /2 )
\end{align*}
$$
Taking the square root and using ##p = \hbar k## will give you your equation.
 
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DrClaude said:
Using ##| \mathbf{k}_i | = |\mathbf{k}_f| = k##, calculate ##q^2##:
$$
\begin{align*}
q^2 &= (\mathbf{k}_i - \mathbf{k}_f)^2 \\
&= k^2 - 2 \mathbf{k}_i \cdot \mathbf{k}_f - k^2 \\
&= 2 k^2 (1 - \cos \alpha) \\
&= 4 k^2 \sin^2 (\alpha /2 )
\end{align*}
$$
Taking the square root and using ##p = \hbar k## will give you your equation.

In your third line; I do not see how you get the ##-2k^2 cos \alpha## term
 
JD_PM said:
In your third line; I do not see how you get the ##-2k^2 cos \alpha## term
$$
\begin{align*}
\mathbf{k}_i \cdot \mathbf{k}_f &= | \mathbf{k}_i | |\mathbf{k}_f| \cos \alpha \\
&= k^2 \cos \alpha
\end{align*}
$$
where ##\alpha## is the angle between ##\mathbf{k}_i## and ##\mathbf{k}_f## (or ##\mathbf{p}_i## and ##\mathbf{p}_f##).
 
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DrClaude said:
$$
\begin{align*}
\mathbf{k}_i \cdot \mathbf{k}_f &= | \mathbf{k}_i | |\mathbf{k}_f| \cos \alpha \\
&= k^2 \cos \alpha
\end{align*}
$$
where ##\alpha## is the angle between ##\mathbf{k}_i## and ##\mathbf{k}_f## (or ##\mathbf{p}_i## and ##\mathbf{p}_f##).
It is the dot product definition! My bad, thanks DrClaude.
 
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