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104 | 104 | \author[8]{D.~Flores} |
105 | 105 | \author[4]{P.~Freeman} |
106 | 106 | \author[4]{Z.~Galloway} |
107 | | -%\author[4]{Y.~Ghao} |
108 | 107 | \author[9]{A.~Ghassemi} |
109 | 108 | \author[3]{H.~Al Ghoul} |
110 | 109 | \author[1]{L.~Gray} |
111 | 110 | \author[8]{S.~Hidalgo} |
112 | | -%\author[4]{C.~Labitan} |
113 | 111 | \author[9]{S.~Kamada} |
114 | 112 | \author[1]{S.~Los} |
115 | | -%\author[4]{Z.~Luce} |
116 | 113 | \author[5]{M.~Mandurrino} |
117 | 114 | \author[8]{A.~Merlos} |
118 | | -%\author[2]{A.~Mangu} |
119 | | -%\author[4]{F.~Martinez-Mckinney} |
120 | 115 | \author[3]{N.~Minafra} |
121 | | -%\author[1]{A.~Prosser} |
122 | | -%\author[1]{R.~Rivera} |
123 | 116 | \author[1]{A.~Ronzhin} |
124 | 117 | \author[8]{G.~Pellegrini} |
125 | 118 | \author[8]{D.~Quirion} |
|
128 | 121 | \author[4]{A.~Seiden} |
129 | 122 | \author[5]{V.~Sola} |
130 | 123 | \author[2]{M.~Spiropulu} |
131 | | -%\author[4]{E.~Spencer} |
132 | 124 | \author[5]{A.~Staiano} |
133 | 125 | \author[1]{L.~Uplegger} |
134 | 126 | \author[9]{K.~Yamamoto} |
135 | 127 | \author[9]{K.~Yamamura} |
136 | | -%\author[4]{M.~Wilder} |
137 | 128 |
|
138 | 129 | \address[1]{Fermi National Accelerator Laboratory, Batavia, IL, USA} |
139 | 130 | \address[2]{California Institute of Technology, Pasadena, CA, USA} |
@@ -691,9 +682,23 @@ \subsection{Study of the uniformity of the LGAD sensors} |
691 | 682 | An important characteristic is the uniformity of the signal size |
692 | 683 | across the surface of the sensor, which directly impacts on its timing performance. We use the signal amplitude as the metric to characterize the signal |
693 | 684 | size uniformity. The distribution of the LGAD signal amplitudes is fitted to a |
694 | | -Landau distribution. The most probable value (MPV) parameter of the fitted |
| 685 | +Landau distribution. An example of the fit is shown in Fig.~\ref{fig:ExampleLandauFit}. |
| 686 | +The most probable value (MPV) parameter of the fitted |
695 | 687 | Landau distribution is plotted in Fig.~\ref{fig:FNAL_HPK50_MPVXY}. |
696 | 688 | A flat response with a uniform signal size is observed over the whole sensor area. |
| 689 | +As a study of systematic effects, we have also repeated the fit using the convolution |
| 690 | +of a Landau function and a Gaussian function to model the impact of noise and fluctuations |
| 691 | +in the multiplication process. We find that the peak location increases |
| 692 | +systematically by about $5\%$ for all points in a correlated fashion. |
| 693 | +However it does not appear to impact the conclusions drawn on the response uniformity. |
| 694 | + |
| 695 | +\begin{figure}[htbp] |
| 696 | +\centering |
| 697 | +\includegraphics[width=0.49\textwidth]{figs/MPVFitExample_Landau.pdf} |
| 698 | +\caption{The signal amplitude distribution is fitted to a Landau function. |
| 699 | +The data corresponds to one bin of the X-axis scan.} |
| 700 | +\label{fig:ExampleLandauFit} |
| 701 | +\end{figure} |
697 | 702 |
|
698 | 703 | \begin{figure}[htbp] |
699 | 704 | \centering |
|
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