Commit 2a1c0843 authored by Simon Spannagel's avatar Simon Spannagel
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Add reference to transient paper

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@@ -1022,3 +1022,14 @@ keywords = {Gallium nitride, Low-field mobility}
  url = {https://www.sciencedirect.com/science/article/pii/S0010465520301181},
  author = {Andy Buckley and Philip Ilten and Dmitri Konstantinov and Leif Lönnblad and James Monk and Witold Pokorski and Tomasz Przedzinski and Andrii Verbytskyi},
}

@article{apsq_transient,
  title = {Transient Monte Carlo simulations for the optimisation and characterisation of monolithic silicon sensors},
  journal = {Nucl. Instr. Meth. A},
  volume = {1031},
  pages = {166491},
  year = {2022},
  issn = {0168-9002},
  doi = {10.1016/j.nima.2022.166491},
  author = {R. Ballabriga and J. Braach and E. Buschmann and M. Campbell and D. Dannheim and K. Dort and L. Huth and I. Kremastiotis and J. Kröger and L. Linssen and M. Munker and P. Schütze and W. Snoeys and S. Spannagel and T. Vanat},
}
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@@ -125,7 +125,8 @@ Q_n^{ind} = \int_{t_0}^{t_1} I_n^{ind} \textrm{d}t = q \left[ \phi (\vec{x}_1)

assuming discrete time steps.
Here, $`q`$ is the charge of the carrier, $`\phi(\vec{x})`$ the weighting potential at position $`\vec{x}`$ and
$`I_n^{ind}`$ the induced current in the particular time step.
$`I_n^{ind}`$ the induced current in the particular time step. A detailed description of the procedure is provided in
\[[@apsq_transient]\] along with examples of application.

Since this procedure requires a realignment of the weighting potential for every pixel or electrode in question, the 
`SENSOR` mapping geometry is not a viable option. The weighting potential map needs to be centered around the electrode
@@ -168,3 +169,4 @@ the pixel in question os by definition zero.*
[@shockley]: http://dx.doi.org/10.1063/1.1710367
[@ramo]: http://dx.doi.org/10.1109/JRPROC.1939.228757
[@planecondenser]: http://dx.doi.org/10.1016/j.nima.2014.08.044
[@apsq_transient]: https://doi.org/10.1016/j.nima.2022.166491
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