TIMING RESOLUTION OF ACTIVE GANGING OF 48 SiPMs ESTEBAN CRISTALDO - PowerPoint PPT Presentation

TIMING RESOLUTION OF ACTIVE GANGING OF 48 SiPMs ESTEBAN CRISTALDO JORGE MOLINA Laboratorio de Mecánica y Energía (LME) Facultad de Ingeniería de la Universidad Nacional de Asunción (FIUNA)

Brief description ◦ I will present the preliminary results of the simulations of timing resolution of the amplified signals of 48 SiPMs by the transimpedance active ganging configuration. ◦ I will try to establish a relationship between the signal’s dynamic characteristics and the arrival time separation of photons hitting the detector in order to distinguish individual photon hits at the output.

Active Ganging scheme Output Transimpedance Hamamatsu S13360-6050

Simulation outline

t bf Dynamic characteristics of the simulated signal: Rise Time (t r ) : 97 ns Fall Time (t f ) : 619.5 ns Time to begin Fall (t bf ) : ~200ns The time to begin the fall is measured from t(V p10% ) at the rising edge to t(V p90% ) at the falling edge. t f t r

3 PE Simulated event where 10 photon hit the detector with exponential distribution of arrival time. The first peak is the fast component with τ = 6 ns followed by photons arriving with τ = 1,6 us. 1 PE

3 PE 1 PE

Peaks below 200 ns of time separation start mergin in each other and blend as a fast arriving photon. Single photon peaks can be clearly seen with a time separation of 300 ns and above 200 ns. The signal peak is distinguishable because it has time to fall 𝑢 𝑡 > 𝑢 𝑐𝑔 𝑢 𝑡 ~260 ns ~300 ns

Two photons arriving with a separation of 110 ns produce a single double peak. The signal peak merge as one because: 𝑢 𝑡 < 𝑢 𝑐𝑔 𝑢 𝑡 ~110 ns

Increasing the number of hits in one detector to 100 illustrates the limits of the timing resolution of the active ganging amplifier.

Increasing the number of hits in one detector to 100 illustrates the limits of the timing resolution of the active ganging amplifier.

Multiple photons arriving under the time resolution Multiple photon hits blending in one peak. are packed in one peak.

◦ Apparently, the time resolution of this configuration is around 200 ns, meaning it cannot distinguish photons arriving less than 200 ns apart. ◦ To have a better view of the time resolution, photon hits can be simulated arriving at fixed time rate of: ◦ 300 ns ◦ 200 ns ◦ 150 ns ◦ 100 ns

With 300 ns arrival time, the peaks are clearly distinguishable.

With 200 ns arrival time, the peaks are still clearly distinguishable, but single photon peaks arriving nearly can be missed.

With 150 ns arrival time, peak amplitude is nearly completely attenuated for single photon hits.

With 100 ns arrival time, the peaks are completely undistinguishable.

Conclusions ◦ Based on observations of this simulations, I conclude that for a signal with a rise time of 97 ns it may be posible to distinguish photons arriving 200 ns appart, down to 150 ns if good SNR is achieved. ◦ By extrapolation, to be able to obtain a timing resolution of 100 ns the rise time of the signal must be 60 ns or less and a time to begin the fall of ~ 100 ns . ◦ Statistical data on based on this kind of simulation can be produced to determine the signal parameters more accurately.

Thanks for your attention.