Adiabatic Quantum-Flux-Parametron (AQFP) logic is a promising emerging device technology with six orders of magnitude lower power than CMOS. However, AQFP is challenged by the fact that every gate must be clocked, where proper data transfer requires connected gates to have shifted but overlapping clocks. As a result, buffers need to be used to balance re-convergent logic paths, a problem that is exacerbated by every multi-node fanout needing a tree of clocked splitters. Recent AQFP circuit design techniques have offered an opportunity to reduce buffer costs by supporting a notion of phase-skipping but the EDA support for these advanced circuits is limited. This paper proposes the first algorithm to optimize buffer and splitter insertion for phase-skipping AQFP circuits and achieves over 31\% savings over existing buffer reduction schemes and up to 74\% savings in buffers and splitter costs over the SOTA non-phase skipping circuits.
Adiabatic Quantum-Flux-Parametron (AQFP) logic is a promising emerging device technology with six orders of magnitude lower power than CMOS. However, AQFP is challenged by the fact that every gate must be clocked, where proper data transfer requires connected gates to have shifted but overlapping clocks. As a result, buffers need to be used to balance re-convergent logic paths, a problem that is exacerbated by every multi-node fanout needing a tree of clocked splitters. Recent AQFP circuit design techniques have offered an opportunity to reduce buffer costs by supporting a notion of phase-skipping but the EDA support for these advanced circuits is limited. This paper proposes the first algorithm to optimize buffer and splitter insertion for phase-skipping AQFP circuits and achieves over 31% savings over existing buffer reduction schemes and up to 74% savings in buffers and splitter costs over the SOTA non-phase skipping circuits.
Josephson Junction (JJ) based superconductor logic families have been proposed and implemented to process analog and digital signals [1] for its low energy dissipation and ultrafast switching speed. Thanks to its construction of resistance-less wires and ultrafast switches, it can operate at clock frequencies of several tens of gigahertz and even hundreds of thousands of times as energy efficient as its CMOS counterparts. It has been perceived to be an important candidate to replace stateof-the-art CMOS due to the superior potential in operation speed and energy efficiency, as recognized by the U.S. IARPA C3 and SuperTools Programs and Japan MEXT-JSPS Project. The design and fabrication of superconducting circuits have already been established [2]-[4]. In addition, a prototype superconducting microprocessor "Core 1" has been demonstrated in 2004 [3], which is able to execute instructions at a high clock frequency of several tens of gigahertz, and with extremely low-power dissipation. These achievements make superconducting electronics highly promising for future high-performance computing applications. As one of the most matured superconducting technology, the Rapid-Single-Flux-Quantum (RSFQ) technology is proposed by K. Likharev, O. Mukhanoc, V. Semenov in 1985 [1]. Despite its capability to be operated at an ultra-high speed of hundreds of GHz while maintaining extremely low switching energy (10^-19 J), it suffers from an increasing static power due to on-chip resistors that are required for constant DC bias supply for the main RSFQ circuit. Numerous methods have been proposed to resolve the static power dissipation problem of RSFQ, including low-voltage RSFQ (LV-RSFQ) [5], reciprocal quantum logic (RQL) [6], LRbiased RSFQ [7] and energy-efficient single-flux quantum (eSFQ) [8]. The Adiabatic Quantum-Flux-Parametron (AQFP) technology, on the other hand, uses AC bias/excitation currents as both multiphase clock signal and power supply [9] to mitigate the power consumption overhead of DC bias while operating at a frequency of few GHz. Consequently, AQFP is remarkably energy efficient compared to RSFQ, albeit operating at a lower frequency. The energy-delay-product (EDP) of the AQFP circuits fabricated using processes such as the AIST standard process 2 (STP2) and the MIT-LL SFQ process [10], [11], is at least 200 times smaller than those of the other energy-efficient superconductor logics and is only three orders of magnitude larger than the quantum limit [9]. Physical testing results of an AQFP 8-bit carry-look-ahead adder and large scale circuits consisting up-to 10,000 AQFP logic gates have demonstrated the AQFP being a promising technology that is robust against circuit parameter variations [12]. Despite the high application potential of AQFP in VLSI circuits, a systematic, automatic synthesis framework for AQFP is imminent. There are two features of AQFP that restrict conventional CMOS synthesis methods being directly applied on AQFP. In spite of And-Or-Inverter(AOI) based representation, which conventional CMOS circuits highly relies on, AQFP circuits prefer majority gates. In fact, its two inputs AND and OR gates are also built with three inputs majority gate with one input being constant. In addition, given its clock-synchronized data propagation nature, AQFP technology requires all inputs to any gate having equal delay. In order to meet this balanced timing requirement, splitters and buffers need to be inserted to the circuit. As a matter of fact, some circuit size can be doubled even with optimum amount of buffers and splitters inserted. The buffer and splitter insertion method can have a huge impact on the overall resource consumption. As the design complexity increases, an unoptimized buffer and splitter insertion method could result in huge amount of unnecessary buffers and splitters added. In addition to a complete synthesis framework, an Integrated Development Environment (IDE) for AQFP design is also lacking. It is imminent to have an IDE for AQFP integrating tools that offer schematic and layout editor, simulation and analysis for better and more efficient AQFP design flow. In this paper, we propose a complete design tool for AQFP design including an Integrated Development Environment (IDE), a complete majority based synthesis framework and a buffer and splitter insertion framework. we propose a majority gates synthesis framework for AQFP circuits that is capable of converting any AOI netlist to its corresponding MAJ netlist by mapping all feasible three-input sub-netlists to corresponding MAJ based implementations. In addition, we also propose an automated buffer and splitter insertion method that is capable of adding the optimum amount of buffers and splitters to any given gate-level netlist. The proposed method can find the minimum amount of buffers and splitters to inserted to achieve equal delay with any library limitation on the size of splitters. Experimental results suggest that the proposed methods can deliver very optimized results. The majority conversion tool can reduce circuit size by an average of 16:47% and delay by 30:21% in average. The buffer and splitter insertion tool only introduces an average of 14:24% overhead in size and 4:70% delay with splitter fanout size limited to 4 compared to an unachievable ideal results with no limitations on splitter fan-out size. Overall, the balanced design in majority gates can be reduced by 23:85% and 29:54% in size and delay compared to its AND/OR/Inverter implemented counterpart.
Abstract Adiabatic quantum-flux-parametron (AQFP) logic is an energy-efficient superconductor logic family. The latency of AQFP circuits is relatively long compared to that of other superconductor logic families and thus such circuits require low-latency clocking schemes. In a previous study, we proposed a low-latency clocking scheme called delay-line clocking, in which the latency for each logic operation is determined by the propagation delay of the excitation current, and demonstrated a simple AQFP buffer chain that adopts delay-line clocking. However, it is unclear whether more complex AQFP circuits can adopt delay-line clocking. In the present study, we demonstrate AQFP logic gates (AND and XOR gates) that use delay-line clocking as a step towards implementing large-scale AQFP circuits with delay-line clocking. AND and XOR gates with a latency of approximately 20 ps per gate are shown to operate at up to 5 and 4 GHz, respectively, in experiments. We also demonstrate that delay-line clocking enables phase skipping operation, in which some of the AQFP buffers for phase synchronization are removed to reduce the junction count and energy dissipation. The results indicate that delay-line clocking can enable low-latency, low-energy, large-scale AQFP circuits.
Abstract Adiabatic quantum-flux-parametron (AQFP) logic is one of the most promising superconductor logic families as a candidate to achieve future energy-efficient high-performance information processing systems. The static power of AQFP logic is zero because of ac flux bias, and the switching energy is ∼zJ at 5 GHz due to adiabatic switching. In this study, we propose a design method using offset buffers to reduce the dimension of AQFP circuits; in particular, we focus on the reduction in the horizontal dimension (which is parallel to excitation current) because in AQFP circuits the horizontal dimension tends to be greater than the vertical dimension (which is perpendicular to excitation current). Offset buffers are buffers with offset input signals. The use of offset buffers enables us to eliminate constant cells (which generate constant 0 s and 1 s) from some logic gates, so that the horizontal dimension of logic gates such as AND and OR gates can be significantly reduced. We designed AND and OR gates with offset buffers, and demonstrated them with wide operating margins. Then, we designed and demonstrated a 4–16 decoder using the AND gate with an offset buffer. We found that the horizontal dimension and area of a 4–16 decoder can be reduced by 33% and 26%, respectively, via the use of offset buffers.
Abstract Adiabatic quantum-flux-parametron (AQFP) logic stands as an energy-efficient superconductor logic family relying on ac excitations. Though a four-phase clocking scheme has been commonly applied to excite and clock AQFP circuits, the cost of multiple sources and long between-stage latency (a quarter clock cycle) remain unsatisfactory. These drawbacks are more severe for sequential logics, where feedback loops require both down-flow and reverse-flow AQFP gates, necessitating extra buffers and imposing a limit on operating depth at the same time. To overcome these restrictions, in this paper, we introduce a novel mixed clocking scheme for low-latency AQFP logic circuits allowing feedback loops. In particular, the down-flow part of the AQFP circuit is excited by an ac current through delay-lines, which can reduce the latency from input to output stages. Meanwhile, the reverse-flow part is clocked by 2 other ac currents with 90° phase difference to reduce the buffering gates. The proposed clocking scheme is first applied to a fundamental logic circuit, confirming correct functionality and low-latency operations for diverse feedback conditions. For experimental validation, we design and fabricate a 3-bit AQFP counter using the proposed clocking scheme based on an on-chip clock splitter. The circuit is examined at 4 GHz under 4.2 K temperature, where we obtain desired operations and wide excitation margins.
An adiabatic quantum flux parametron (AQFP) is a two-terminal superconducting device capable of amplifying or inverting digital input signals at near-kT energy dissipation. This ultra-low power device is desirable for myriad reasons, including high performance accelerator applications as CMOS processors become more and more limited by energy consumption. Promising performance results have been realized on AQFP processors; however, scaling these results to larger computing systems faces engineering challenges due to device density and power distribution. AQFP circuits require a multi-phase activation signal to propagate logic. If data is not properly aligned with the activation phase, it can be dropped or shifted to an incorrect phase and disrupt circuit operation. This work presents design and simulation of an activation phase synchronizer: a simple circuit that will accept data arriving on any phase and re-align it to a known phase of the subsequent cycle. The phase synchronizer can be useful for mitigating clock skew across clock domains or play an important role in asynchronous design where the arrival time of data may be unknown.
Adiabatic quantum-flux-parametron (AQFP) logic is a superconductor logic family that can operate with low switching energy due to adiabatic switching. In a previous study, we proposed a low-latency clocking scheme called delay-line clocking, in which the latency for each logic operation is determined by the propagation delay of the excitation current. We demonstrated several AQFP logic gates with delay-line clocking and demonstrated a phase skipping operation, in which some of the AQFP buffers for phase synchronization are removed to reduce the junction count and energy dissipation. In the present study, we design and demonstrate an AQFP 8-bit ripple carry adder with delay-line clocking to show that delay-line clocking and the phase skipping operation are applicable to large-scale AQFP circuits. The latency of this adder is 960 ps, which is 40% of that for a conventional design. Moreover, due to the phase skipping operation, the junction count is reduced to approximately 70% of that for the conventional design. We find that this adder can operate at up to 4 GHz. The above results indicate that large-scale AQFP circuits can operate with low latency and low junction count by using delay-line clocking and a phase skipping operation.