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I would really appreciate if someone could help me about computing the form factor $$F(q^2)=\int_0^{\infty}\rho(r)e^{-iq\cdot r}d^3r \quad, $$ when $$\rho (r)=\begin{cases}\rho_0& r<R\\0& r>R\end{cases}\quad . $$ The answer is $$F(q^2)=\frac{3(\sin (qr)-qr\cos(qr))}{(qr)^3},$$ where $r=|\overset{\to}{r}|$, $q=|\overset{\to}{q}|$, $\overset{\to}{q}$, and $\overset{\to}{r}$ are three dimensional vectors, but I don't know how to obtain it. Thanks in advance.

What I've tried: Using spherical coordinates, we have $d^3 r=dxdydz=r^2dr\sin \theta d\theta d\phi$, where $0\leq r\leq R$, $0\leq \theta \leq \pi$, and $0\leq \phi \leq 2\pi$. Then $$\int_{0}^{\infty}e^{-i\overset{\to}{q}\cdot \overset{\to}{r}}d^3 r=\int\int\int e^{-irq\cos\theta}r^2dr\sin \theta d\theta d\phi$$ $$=2\pi \int\int e^{-irq\cos\theta}r^2dr\sin \theta d\theta .$$ Now how can I compute the last integral?

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    $\begingroup$ Transform to spherical coordinates, picking up a $|r|^2\sin{\theta}$ Jacobian factor and a cosine in the exponential from the definition of the inner product, with integration range $0<|r|<R$, $0<\theta<\pi$, and $0<\phi<2\pi$. The resultant integrals are known. $\endgroup$ Commented Jun 18, 2023 at 13:03
  • $\begingroup$ @QuantumFieldMedalist Thanks very much for the hint. Based on your comment, I've just added my try. I'd appreciate if you could help me about computing the last integral. $\endgroup$
    – Mahtab
    Commented Jun 18, 2023 at 13:56
  • $\begingroup$ The integral over $\theta$ can be computed by a trig-substitution, namely $x:= \cos \theta$, yielding $2 \frac{\sin{qr}}{q r}$. The remaining $r$ integral may be computed by integration by parts. $\endgroup$ Commented Jun 18, 2023 at 14:01
  • $\begingroup$ @QuantumFieldMedalist As you said, $\int e^{-irq\cos\theta}\sin \theta d\theta=2\frac{\sin qr}{qr}$. But the remaining $r$ integral is $\rho_0 2\pi (\frac{2}{q})(-\frac{r}{q}\cos qr+\frac{1}{q^2}\sin qr)$ which is different from the answer. Can you help me about this? $\endgroup$
    – Mahtab
    Commented Jun 18, 2023 at 14:39
  • $\begingroup$ After plugging in your $\theta$ integral, there is still a factor of $r^2$. Thus, the remaining integral is basically $\int_{0}^{R} dr \frac{r}{q} \sin{ q r} = \frac{(\sin{qr} - q R \cos{qr})}{q^{3}}$. Using the fact that $\rho_{0} = \frac{3}{4 \pi R^{3}}$ gives the right answer. $\endgroup$ Commented Jun 18, 2023 at 15:10

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You can use the fact $$ \int e^{-iqr \cos\theta} \sin \theta d\theta = -\int e^{-iqr c} dc $$ where $c$ is the integration variable that replaced $\cos\theta$. The integral is now elementary. The form factors for spheres (this case), rods and slabs are reported in, e.g., this paper (see equation 42). For more details, see also Scattering from homogeneous objects and this answer.

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  • $\begingroup$ Thank you very much for your help and the nice comments. $\endgroup$
    – Mahtab
    Commented Jun 18, 2023 at 15:15

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