I. Introduction
Time-to-digital converter (TDC) is the core device in time measurement, which is widely used in high-energy physics [1], [2], light detection and ranging (LiDAR) systems [3], [4], medical imaging [5], [6], digital phase-locked loop (DPLL) [7], [8], and analog-to-digital converter (ADC) [9], [10]. At the Super Tau-Charm Facility (STCF) in China, the endcap region particle identification (PID) system detects the internally reflected Cherenkov light (DIRC) and measures its time-of-flight (TOF) to identify charged particles produced by the collision of electrons and positrons. As shown in Fig. 1, TDC in the DIRC-like TOF (DTOF) detector is responsible for the quantization of the time of arrival (TOA) and time-over-threshold (TOT) of the photon signal. For excellent PID capability, the DTOF detector is required to have a single-photon time resolution of better than 50 ps [11], which needs the timing uncertainty of the readout part to be no more than 43 ps. After deducting the contributions from the photosensor (32 ps), amplifier and discriminator (20 ps), and clock synchronization (15 ps), the time measurement precision of TDC should be better than 15 ps. In addition, the TDC has to reach a sample rate of several megahertz, a large measurement dynamic range, and relatively low power consumption to fulfill the operation and integration requirements of STCF.
Illustration of the DTOF detector at STCF.