In this work, the proposed ULVTSCR devices are processed in a 65-nm CMOS logic technology. The layout of the basic ULVTSCR is shown in Fig. 3, where the width of its internal SCR (WSCR) is 50 µm. The ENMOSs-string is set nearby the internal SCR and the distance between them is 8 µm (the minimum distance of the design rule). The width of each ENMOS (WN) is 10 µm. To avoid the parasitic effects associated with the substrate, two P-type guard rings are employed around the ENMOSs-string and the internal SCR, respectively. The quasi-static I-V characteristics of the proposed devices are measured using Hanwa TED-T5000 transmission line pulsing (TLP) tester with 10 ns rise time and 100 ns pulse width.
Four ULVTSCR devices containing different numbers (N = 3, 4, 5, 6) of ENMOSs are named ULVTSCR1, ULVTSCR2, ULVTSCR3, and ULVTSCR4, respectively. Measured TLP I-V characteristics of four ULVTSCRs are compared in Fig. 4, as their specification and measurement results are listed in Table I. As expected, all devices operate with much low trigger voltages (Vt1) as well as high enough failure currents (It2). There are two trigger stages observed in turn-on processes of all devices. In ULVTSCR1, the first stage starts at ~ 1.92V due to the INMOS turned on driven by the trigger point (seen in Fig. 1.(a)), and the second stage is at ~ 5.65V due to the internal SCR triggering. Then, the voltage of ULVTSCR1 snap back to ~ 2.42V because of the positive feedback effect between Q1 and Q2. Subsequently, the SCR path dominants the ESD current conduction with a low resistance and achieves It2 of ~ 2.72A. When increases N from 3 to 6, the total Vth of the ENMOSs tends to be doubled. On the one hand, the Vt1 has a decrease from ~ 5.65V to ~ 5.47V due to more current urged to the SCR path with the increased resistance of the ENMOSs-string. Notice that the Vh and It2 of these devices basically keep the same. On the other hand, the Von of ULVTSCR2, ULVTSCR3 and ULVTSCR4 accordingly has been improved to ~ 2.80V, ~ 3.44V, and ~ 4.05V, respectively. Therefore, the proposed ULVTSCR structure is expected to provide effective ESD protections for different applications by adjust the number of its ENMOSs.
The leakage currents of four ULVTSCRs were measured by sweeping DC voltage from 0 to 1.8V at room temperature, as shown in Fig. 5. The results indicate that all ULVTSCRs possess acceptable nA-level leakage when biased DC voltage below 0.6A. As the the number of ENMOS increased, the leakage characteristic will be optimized. For 1.8V applications, the ULVTSCR4 with 6 external NMOSs can be used. For 1.2V operations, The NMOS strings with 5 NMOSs is more suitable. More importantly, the leakage clamp capability might be further improved by increasing the number of the external NMOSs. But the number of ENMOSs needs special consideration with a trade-off between the area and leakage according to various applications.
In nanoscale CMOS processes, the epitaxy thickness is goes to thinner as the feature size scaling down, which will lead a higher sheet resistance for NWELL and PWELL. Therefore, increasing the distance (D1) from N + active region to P + active region in NWELL/PWELL can effectively enlarge the resistance of NWELL (PWELL). Figure 6 shows the measured TLP I-V characteristic of ULVTSCRs with four different D1. When increasing D1 from 0.5 µm to 4.0 µm, the Vt1 decreases by about 23% from ~ 6.92V to ~ 5.03V, and the trigger current is reduced from ~ 892 mA to ~ 467 mA. Moreover, the It2 also has an increase from ~ 2.72A to ~ 2.97A. These phenomenon can be attributed to more current branching into the SCR path as the INMOS path and N+/NWELL/PWELL/P + diode path weakened by the enlarged RNWELL and RPWELL.
Figure 7 illustrates that a larger length of the INMOS’s gate D2 will lead to a significant increase in Vh (from 2.42V to 3.69V) and an enhancement in holding current. This is because the increased base length of the Q2 will cause a decrease in the SCR current gain. Besides, the increased INMOS channel resistance will restrain current through the INOMS path, however, prompt more current to flow into the SCR path, which alleviates the so-called current concentration effect on INMOS, and further result in an improved It2 from 2.72A to 2.85A.