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.
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.
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 report simulated results of-rapid single flux quantum (SFQ) circuits having driver, receiver, and passive transmission lines for propagating SFQ pulses to investigate the design criteria. We have studied the equivalent input/output resistance of the driver/receiver in various bias conditions and found that the resistance is almost proportional to the bias current of the driver/receiver. Furthermore, we have proposed inserting a series resistor at the end of the superconducting passive transmission line (PTL) for avoiding undesirable flux trapping in the loop and for isolation in regard to the DC current. We also found that the reduction of the bias margin due to the resistance is rather small when the resistance is much smaller than the impedance of the PTL. An operating margin of more than 30% was obtained in the driver/receiver circuits including the PTL and the series resistor.
Superconductive electronics based on Josephson junctions (JJ) is a promising cryogenic alternative technology to complementary metal oxide semiconductor (CMOS) technology for ultra-low energy, high speed stationary applications. For complex superconductive systems, the automated routing process determines the topology and methodology to connect cells while satisfying design constraints. On-chip signal routing has become an issue of growing importance in modern superconductive technologies; particularly, single flux quantum (SFQ) systems. Specialized routing methods for these systems are required. These routing methods include passive transmission lines (PTLs) and Josephson transmission lines (JTLs) behaving as interconnects. A primary issue within a long SFQ interconnect is the effects of resonance due to the imperfect match between the PTLs and Josephson junctions. A repeater insertion methodology to reduce and manage these resonance effects is required for driving long and short interconnect in VLSI complexity SFQ systems. Permissible interconnect lengths are suggested to ensure the reflections do not affect the returning signals. The microwave behavior of the interconnect striplines is also considered to accurately estimate the surface inductance of the lines. A closed-form expression describing the dependence of the surface inductance of a stripline on the line thickness, magnetic field, and current density is discussed. Another primary issue within SFQ circuits is coupling noise between transmission striplines, degrading performance and decreasing margins. Inductive and capacitive coupling noise between the routing layers, for the MIT LL SFQ5ee process, is described. An analysis of inductive and capacitive coupling noise can determine the minimum physical spacing between lines to enhance the automated routing process in large scale systems. The increasing complexity of modern SFQ circuits has also made the issue of flux trapping of growing importance. The use of wide striplines for signal routing has exacerbated this issue. Trapped residual magnetic fields within the striplines damage the operability of superconductive circuits. Area efficient topologies for striplines are introduced to manage flux trapping in large scale SFQ circuits. These topologies are composed of several narrow lines rather than a single wide stripline. The first approach is a narrow parallel line topology in series with small resistors where each narrow line is connected to a single small resistor and via. The resistors in the parallel line topology remove any trapped fluxons and break any loops while requiring additional vias. The second topology is a fingered narrow line topology. The fingered narrow line topology enhances the scalability of SFQ systems while not requiring additional area and vias. These proposed topologies require significantly less area while preventing flux from being trapped within wide superconductive striplines and reducing coupling noise between striplines. These methodologies and techniques are intended as guidelines to enable robust routing with superconductive interconnects. With these and other advances in design methodologies for superconductive electronics, the complexity of SFQ circuits is expected to greatly increase.
Passive transmission lines (PTLs) provide an energy-efficient means of transporting pulsed single flux quantum (SFQ) signals between logic gates and blocks on a chip, or even between chips through a multi-chip module carrier. Although functional up to 70 GHz, our previous designs manifested sharp, length-dependent resonances resulting in diminished operating margins. These are particularly inconvenient since the resonant length is about 1 mm at 40–50 GHz, where most SFQ circuits currently function. To avoid the need to keep the PTLs < 1 mm in length, we have optimized the PTL driver-receiver pairs to sufficiently suppress these resonances; this helps facilitate the use of automated routing tools. We present experimental results, in the 10-70 GHz frequency range, for different driver-receiver pairs designed for PTLs in our dual RSFQ-ERSFQ cell library. This cell library, targeting MIT Lincoln Laboratory's SFQ5ee fabrication process, uses PTLs with two types of ground plane configuration. The first variant has signal in M1 and/or M3 with symmetrical ground planes in M0, M2 and/or M2, M4 respectively. The second variant has signal in M2 and/or M3 with asymmetrical ground planes in M1 and M4. We also present a comparison with wider, 4 Ω, PTLs that are more suitable for transport between distant logic blocks. Next, we present experimental results of PTL lengths ranging from 1.2-12 mm over the same 10-70 GHz frequency range. Finally, we report on the design of circuits for investigating crosstalk between two PTLs and their measurement results.
To enable the use of passive transmission lines (PTLs) for the interconnection of single-flux-quantum (SFQ) circuits, we have implemented a driver and a receiver and have developed a method for designing SFQ circuits with passive interconnections. Basic components and properties of passive interconnections, such as the frequency characteristics of the driver and receiver, the PTL delay, and the crosstalk between PTLs, have been experimentally verified. Our developed components and design method have been applied to actual SFQ circuits, such as a 4 x 4 switch having block-to-block passive interconnections and a 2 x 2 switch having gate-to-gate passive interconnections. We have also shown the advantages of PTLs over Josephson transmission lines (JTLs). We also discuss the prospects of SFO circuits having passive interconnections.
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 parameterβCof the JJ in the design of the PTL's driver and receiver. Furthermore, the accompanying influence from JJ's modifiedβCon 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%.