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IEEE Transactions on Applied Superconductivity

Timing Evaluation of Passive Transmission Line by RSFQ Ring Oscillator

Xi Gao, Huanli Liu, Xiaoping Gao, Xue Zhang, Jie Ren

Published Feb 5, 2024• 1 citation
Publisher

Abstract

Passive transmission line (PTL) has been widely applied in rapid single flux quantum (RSFQ) circuits, especially as the first choice of long-distance transmission in large-scale integrated circuits such as arithmetic and logic unit (ALU) and central processing unit (CPU). With the increasing demand of timing regulation, general bias margin is not enough to evaluate the performance of PTL circuits. Timing accuracy including propagation delay of the micro stripe line (MSL) and its delay skew is more critical for clock routine and signal transmission when employing PTL circuits. However, the related reports about the timing information of PTL circuits is limited in the single-value verification of the theoretical MSL's delay. More factors such as bias current, transmission length and system noise should be considered into the evaluation of the PTL circuits. This work focuses on the timing extraction of the designed PTL circuits through different control groups, and evaluates the timing discrepancy between the measurement and simulation. We adopt the method of time accumulation by increasing different lengths of MSL in the loop of the ring oscillator (RO) and subtract each other to evaluate the MSL's propagation delay. We analyzed MSLs of two layers (MSL1 and MSL2). The measured propagation delay of 1${\bm{mm}}$MSL is 8.20${\bm{ps}}/{\bm{mm}}\ $for MSL1 and 7.66${\bm{ps}}/{\bm{mm}}$for MSL2, which has a delay skew of 0.30${\bm{ps}}$and 0.57${\bm{ps}}$from the simulated value (8.23${\bm{ps}}$). Within MSL transmission length of 5${\bm{mm}}$, a maximum deviation of 1.2${\bm{ps}}$is adopted as time redundancy of PTL circuits applied in ALU and CPU design.

DOI
10.1109/tasc.2024.3360014

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Passive transmission line (PTL) has been widely applied in rapid single flux quantum (RSFQ) circuits, especially as the first choice of long-distance transmission in large-scale integrated circuits such as arithmetic and logic unit (ALU) and central processing unit (CPU). With the increasing demand of timing regulation, general bias margin is not enough to evaluate the performance of PTL circuits. Timing accuracy including propagation delay of the micro stripe line (MSL) and its delay skew is more critical for clock routine and signal transmission when employing PTL circuits. However, the related reports about the timing information of PTL circuits is limited in the single-value verification of the theoretical MSL's delay. More factors such as bias current, transmission length and system noise should be considered into the evaluation of the PTL circuits. This work focuses on the timing extraction of the designed PTL circuits through different control groups, and evaluates the timing discrepancy between the measurement and simulation. We adopt the method of time accumulation by increasing different lengths of MSL in the loop of the ring oscillator (RO) and subtract each other to evaluate the MSL's propagation delay. We analyzed MSLs of two layers (MSL1 and MSL2). The measured propagation delay of 1mm{\bm{mm}}mmMSL is 8.20ps/mm {\bm{ps}}/{\bm{mm}}\ ps/mm for MSL1 and 7.66ps/mm{\bm{ps}}/{\bm{mm}}ps/mmfor MSL2, which has a delay skew of 0.30ps{\bm{ps}}psand 0.57ps{\bm{ps}}psfrom the simulated value (8.23ps{\bm{ps}}ps). Within MSL transmission length of 5mm{\bm{mm}}mm, a maximum deviation of 1.2ps{\bm{ps}}psis adopted as time redundancy of PTL circuits applied in ALU and CPU design.
Along with the improvement of integration and the requirement of high-speed operation, the passive transmission line (PTL) plays a significant role in superconducting integrated circuits due to its intrinsic advantage of extremely low propagation delay and low signal loss in long-distance transmission. Good impedance matching is critical to reduce the signal reflection in the transmission line and maximize the power transferred. Based on the PTL wiring layer selection under SIMIT-Nb03 process, we studied the equivalent input/output impedance for Josephson junction (JJ) at the IO port and explored a method of impedance matching in rapid-single-flux-quantum circuits by adjusting the Stewart McCumber parameterβC{\beta }_{\bm{C}}βC​of the JJ in the design of the PTL's driver and receiver. Furthermore, the accompanying influence from JJ's modifiedβC{\beta }_{\bm{C}}βC​on the performance of the driver and receiver is evaluated to maximize the profit of the functional circuits. The common-used serial resistor is removed to obtain a balanced bias margin for the PTL circuits. The proposed PTL has been designed and tested based on SIMIT-Nb03 fabrication process. In total,$ \pm $30% bias margin for the PTL is achieved at low frequency and high frequency (40 GHz) contrast tests, including operation speed and transmission length as test vector. Additionally, a frequency sweep for 1 mm PTL is performed by the designed ring oscillator on the chip. The maximum working frequency is up to 129 GHz, with a margin duration of 8%.
The increasing complexity of modern rapid single flux quantum (RSFQ) circuits has made on-chip signal routing, an issue of growing importance. In this paper, several methods for routing large-scale RSFQ circuits are described, and a process is presented for determining when to use passive microstrip transmission lines (PTL) and active Josephson transmission lines (JTL). The effect of the size of the JTL inductor and Josephson junctions on the length of a JTL chain for a target delay is also discussed. The dependence of the JTL inductance on the physical layout is evaluated, and the effects of the primary PTL parameters on delay are characterized. A novel PTL driver and receiver configuration is also proposed. Tradeoffs among the number of JJs, inductance, and length of a PTL stripline in the receiver and driver circuits are reported. The energy dissipation is evaluated for two different interconnects. A tradeoff between the proposed PTL circuits and an optimized JTL in terms of energy dissipation and delay is discussed. Guidelines for choosing the optimal element values are determined, and a simulated bias margin of ±29% for the bias current of the proposed receiver operating at 20 GHz in a 10 kA/cm2technology for a 1-mm transmission line is achieved. Summarizing, guidelines and design tradeoffs appropriate for automated layout and synthesis are provided for driving long interconnect in SFQ VLSI circuits.
We have designed ring oscillators to test rapid single flux quantum (RSFQ) circuits with passive transmission lines at high frequencies. To reduce the width of the transmission line, design methods for increasing the characteristic impedance of the transmission line have been investigated and then we designed a 5-stage of Josephson transmission line (JTL) receiver which can transform the impedance from 1 to 4 /spl Omega/ by changing the critical current and the inductance. The receiver, driver, and micro-strip line were inserted in a ring oscillator. The ring oscillator fabricated with the Nb/AlOx/Nb junction process was successfully operated at frequencies ranging from 6 to 10 GHz for line lengths of 0.6, 3, 6, and 9 mm. The usefulness of the impedance transformation was then confirmed experimentally. A propagation delay per unit length of 8.4 ps/mm was also obtained.
Superconductive passive transmission lines (PTL) are widely used for signal routing in large-scale rapid single flux quantum (RSFQ) circuits. Due to the imperfect matching of the transmission lines between the driver and receiver, single flux quantum (SFQ) pulses are partially reflected. The round trip propagation time of these reflections can coincide with the following SFQ pulse, resulting in a decrease in bias margins or incorrect circuit behavior. This resonant effect depends upon the length of the PTL and the clock frequency of the signal. A methodology to reduce and manage this effect is the focus of this article. A closed-form expression describing the dependence of the resonance frequency on the length of the PTL is presented. This expression describes a set of forbidden lengths for PTL interconnect segments in RSFQ circuits. The proposed methodology and algorithm insert active PTL-based repeaters into long superconductive interconnect while ensuring the length of the line segment is outside the forbidden region and increasing bias margins.
As the complexity of superconductor circuits grows, we envision a dense network of passive transmission lines (PTLs) being used to interconnect cells in rapid-single-flux-quantum (RSFQ) circuits. In our library approach, each cell has dedicated tracks as place holders for routing PTLs. Higher impedance PTLs are desirable due to their narrower width. However, at higher impedance, the margins for the PTL receiver degrade rapidly. We have designed, fabricated, tested, and simulated passive transmission lines (PTLs) for high-speed interconnects in the MIT-LL SFQ5ee 10 kA/cm2process. For the symmetric dual ground planes case, PTLs are in the M1 layer with M0 and M2 ground planes, or in the M3 layer with M2 and M4 ground planes. For the asymmetrical dual ground planes case, PTLs are in M2 or M3 layers with M1 and M4 ground planes. We report ±30% margins for these PTLs. We investigate the receiver margins for these PTLs and report impact of margins as a function of corners, interlayer transitions, variants of drivers, and receivers. We demonstrate 100 GHz PTL operation in ring oscillator measurements. We have also adopted multi-layer multi-conductor transmission line models for PTL simulation. We observe good model-to-hardware correlation for low- and high-frequency operation.
We have studied single-flux-quantum (SFQ) propagation properties in passive transmission lines (PTLs) based on a 10-Nb-layer device structure (ADP2). In ADP2, we can use the PTLs with a line width about 5 mum, one seventh of conventional line width by adopting a strip line (SL) structure and increasing the characteristic impedance. The evaluation has been conducted on the PTL length and the via-hole structure by using ring oscillators. We found that the decrease in the operating region was larger for longer PTL, compared with that in a conventional device structure (STD2). The results would be caused by the increase in the surface resistance. The via-holes connecting the PTLs on different layers have more complicated structure than those of STD2. We have designed the via-hole structure using the electromagnetic wave simulator HFSS. As a result, we have demonstrated sufficiently large operating margins at any data rates up to 80 Gb/s even for the ring oscillator with 30 via-holes.