A binary counter using bistable dc SQUID's as flip flop circuits is demonstrated. All of the functions: LOAD, COUNT, STORE, READ, and CLEAR can be performed. The use of single flux quantum logic results in high sensitivity (10-18J input pulse energy), high speed (100 GHz count rate) and low power (10-7W at 100 GHz count rate).
A Josephson binary counter using single-flux quanta transitions of DC SQUIDs (superconducting quantum interference devices) has been fabricated using an eight-level NbN-based process. High-speed binary division has been demonstrated at 4.2 K, with single-cell counting observed at 60 GHz using the Josephson voltage-to-frequency relationship. Count rate was primarily limited by conservative process and design rules. The counter was designed for operation at 4.2 K. At 8-10 K, the beta /sub L/ of the SQUIDs would not allow operation, though the junction characteristics were good.>
Adiabatic quantum-flux-parametron (AQFP) logic is an energy-efficient superconductor logic family. In this article, we design binary counters, namely an up counter, a down counter, and an up/down counter, based on AQFP logic. These binary counters are T-flip-flop-based and count logic 1s in the input signal that is synchronized with excitation currents, which clock the counters. The internal state of a T flip-flop changes when the internal state of the previous T flip-flop changes from logic 1 to 0 and from logic 0 to 1 for the count-up and count-down operations, respectively. Each internal state of a T flip-flop is read out serially by a buffer chain coupled to the T flip-flops. We fabricate 4-bit up, down, and up/down counters using the AIST 10 kA/cm2Nb high-speed standard process and demonstrate their correct operation at low frequency. This is the first demonstration of binary counters based on AQFP logic.
This paper presents a study on the merits of single flux quantum (SFQ) logic in superconducting digital electronics. With no requirements for an external RF clock source, the speed of SFQ logic circuits can exceed 100 GHz, orders of magnitude higher than latching logic circuits. Use of overdamped junctions in SFQ circuits makes this logic available for already developed high-Tc junctions. Simulations show the operation of SFQ circuits at above 10 GHz with the junctions having characteristics similar to those of YBa2Cu3O7-x/Au/YBa2Cu3O7-x planar junctions. A similar concept is applied to NbN circuits operable above 10 K. A flip-flop counter using NbN junctions with Vm (1.5 mV)=3 mV and Delta =1.9 mV to model 12 K operation has been successfully simulated up to 5 GHz. Operating margins of only 26% on MVTL shift register were obtained by simulations, which is comparable to the margins for SFQ logic circuits. A counting SFQ analogue-to-digital converter can be improved by using an output buffered quantizer.
A superconductive analog-to-digital converter which uses a DC SQUID as a quantizer and a flip-flop counter as a digitizer has been designed, fabricated, and tested. The circuit was fabricated using a ten-level niobium process. Tests at 4.2 K demonstrated counting to the full 12-b accuracy of the design, monotonic A/D conversion with linearity to less than 1 LSB over the more than 9-b range of conversion, read-on-the-fly operation with counter overflow, and counter operation with a gate current bus.
High speed, single flux quantum (SFQ) binary scalers are important components in superconducting analog-to-digital converters (ADC). This paper reviews the concept for a SQUID ADC and the design of an SFQ binary ripple counter, and reports the simulation of key components, and fabrication and performance of non-latching SQUID scalers and SFQ binary ripple counters. The SQUIDs were fabricated with Nb/Nb2O5/PbIn junctions and interconnected by monolithic-superconducting transmission lines and isolation resistors. Each SQUID functioned as a bistable flip-flop with the input connected to the center of the device and the output across one junction. All junctions were critically damped to optimize the pulse response. Operation was verified by observing the do I-V curves of successive SQUIDs driven by a cw pulse train generated on the same chip. Each SQUID exhibited constant-voltage current steps at 1/2 the voltage of the preceding device as expected from the Josephson voltage-to-frequency relation. Steps were observed only for the same voltage polarity of successive devices and for proper phase bias of the SQUID. Binary frequency division was recorded up to 40GHz for devices designed to operate to 28GHz.