1–6 Oct 2023
Geremeas, Sardinia, Italy
Europe/Zurich timezone

Design and characterization of sub-10ps TDC ASIC in 28nm CMOS technology for future 4D trackers

3 Oct 2023, 11:40
20m
Mistral Room

Mistral Room

Oral ASIC ASIC

Speaker

Larry Lou Jr Ruckman (SLAC National Accelerator Laboratory (US))

Description

4D tracking with ~10ps timing is crucial for reducing the combinatorial challenge of track reconstruction at high pileup densities, it offers completely new handles to detect and trigger on LLP and enables particle-ID capabilities at low transverse momentum. At the Muon Collider, the timing information will be essential for reduction of BIB. A high-precision TDC is a critical block necessary for enabling 4D tracking. We present the design and characterization of a 4-channel sub-10ps TDC ASIC in 28nm CMOS technology. The developed TDC is based on a novel 2D Vernier ring-oscillator structure with embedded sliding-scale technique for conversion linearity improvement.

Summary (500 words)

4D trackers with ~10ps timing will be transformative at future collider experiments. Timing is crucial for reducing the combinatorial challenge of track reconstruction at extremely high pileup densities, it offers completely new handles to detect and trigger on long-lived particles (LLP), expands the reach to search for new phenomena, and enables particle-ID capabilities at low transverse momentum. At the Muon Collider, the timing information will be essential for reduction of the beam-induced background (BIB).
CERN’s EP-R&D-WP5 survey has promoted the selection of 28nm CMOS node as the next step in microelectronics scaling for HEP designs. As one of the critical blocks necessary to enable 4D operation in trackers, we present the design and characterization of a 4-channel sub-10ps Time-to-Digital Converter (TDC) ASIC in the 28nm node. The developed TDC is based on a novel 2D Vernier ring-oscillator structure with embedded sliding-scale technique for conversion linearity improvement that will simplify calibration of the TDCs, especially useful in high-channel count implementations such as 4D trackers.
The core of the TDC architecture is composed of differential voltage-controlled delay cells set at 50ps propagation delay and assembled in a 4-cell ring-oscillator with enable/disable function with programmable starting state. The ring-oscillator, enabled with a START trigger, coupled with a counter and a series of flip-flops that sample the oscillator's state at a STOP-trigger, is capable of performing time-interval quantization with 50ps time-steps and a range of 1.6ns. The feature of having the oscillator starting condition programmable, coupled with pseudo-random selection of the starting point at each measurement cycle, performs the sliding-scale function thus improving the conversion linearity beyond the limits set by mismatches between the delay cells of the ring-oscillator. To reach a sub-10ps resolution, the 50ps time-step of the previous structure is interpolated by a factor of 8 using a second ring-oscillator with delay cells set to 56.25ps propagation delay and enabled by a second STOP signal. Each step of the first ring-oscillator is sampled in correspondence of both rising and falling edges of the second ring-oscillator by a 2D array of flip-flops. This 2D Vernier structure reaches a resolution equal to the difference of propagation delays of cells in the two oscillators, i.e. 6.25ps. Compared to a traditional Vernier TDC, the 2D configuration allows faster conversion times and longer measurement range. Both ring-oscillators implement the programmable starting state, i.e. sliding-scale, thus improving the linearity of the overall conversion.
The schematic and layout of a TDC channel is shown in Fig. 1. Each channel receives one START and two STOP signals, simultaneously performing a 6.25ps and a 50ps measurements of the two time-intervals, for example a time-of-arrival (TOA) and a time-over-threshold (TOT) measurement. The 1.6ns measurement range of the prototype can easily be extended in future iterations by simple addition of a flip-flop to the counter. The 4-channel ASIC is shown in Fig. 2. The ASIC was submitted at the end of January and the characterization is expected to start in May. Both the design and characterization will be presented at the workshop.

Authors

Aldo Pena Perez (SLAC National Accelerator Laboratory) Angelo Dragone (SLAC National Accelerator Laboratory (US)) Ariel Gustavo Schwartzman (SLAC National Accelerator Laboratory (US)) Bojan Markovic (SLAC National Accelerator Laboratory (US)) Caterina Vernieri (SLAC National Accelerator Laboratory (US)) Dong Su (SLAC National Accelerator Laboratory (US)) Larry Lou Jr Ruckman (SLAC National Accelerator Laboratory (US)) Lorenzo Rota Valentina Cairo (CERN) aseemg Gupta

Presentation materials