# Difference between revisions of "Form Factor:Cylindrical symmetry"

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## Derivation

### Form Factor

Assuming a particle is cylindrically-symmetric:

${\displaystyle \rho (\mathbf {r} )=\rho (r,\phi ,z)=\rho (r)}$

We of course use cylindrical coordinates:

${\displaystyle \mathbf {r} =(x,y,z)=(r\cos \phi ,r\sin \phi ,z)}$

We can take advantage of the cylindrical symmetry by rotating any candidate q-vector into the ${\displaystyle q_{x},q_{z}}$ plane, eliminating the ${\displaystyle q_{y}}$ component:

${\displaystyle \mathbf {q} =(q_{x},0,q_{z})}$
{\displaystyle {\begin{alignedat}{2}\mathbf {q} \cdot \mathbf {r} &=q_{x}x+q_{y}y+q_{z}z\\&=q_{x}r\cos \phi +q_{z}z\\\end{alignedat}}}

The form factor is (note that the integration limits in z define the particle size in that direction):

{\displaystyle {\begin{alignedat}{2}F(\mathbf {q} )&=\int \rho (\mathbf {r} )e^{i\mathbf {q} \cdot \mathbf {r} }\mathrm {d} V\\&=\int \limits _{z=0}^{L}\int \limits _{\phi =0}^{2\pi }\int \limits _{r=0}^{\infty }\rho (r)e^{i\mathbf {q} \cdot \mathbf {r} }r\mathrm {d} r\mathrm {d} \phi \mathrm {d} z\\&=\int \limits _{0}^{L}\int \limits _{0}^{2\pi }\int \limits _{0}^{\infty }\rho (r)e^{i(q_{x}r\cos \phi +q_{z}z)}r\mathrm {d} r\mathrm {d} \phi \mathrm {d} z\\&=\left(\int \limits _{0}^{L}e^{iq_{z}z}\mathrm {d} z\right)\int \limits _{0}^{\infty }r\rho (r)\left(\int \limits _{0}^{2\pi }e^{iq_{x}r\cos \phi }\mathrm {d} \phi \right)\mathrm {d} r\\&=\left(\left[{\frac {1}{iq_{z}}}e^{iq_{z}z}\right]_{z=0}^{L}\right)\int \limits _{0}^{\infty }r\rho (r)\left(\int \limits _{0}^{2\pi }e^{iq_{x}r\cos \phi }\mathrm {d} \phi \right)\mathrm {d} r\\&=\left({\frac {e^{iq_{z}L}-1}{iq_{z}}}\right)\int \limits _{0}^{\infty }r\rho (r)\left(\int \limits _{0}^{2\pi }e^{iq_{x}r\cos \phi }\mathrm {d} \phi \right)\mathrm {d} r\\\end{alignedat}}}