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Applied Physics Letters

Study on the optical input interface for Nb single-flux-quantum logic circuits

M. Inoue, Takashi Nishitani, Akira Fujimaki, Takahiro Yamada, Koji Sawaki, Iwao Kawayama, Masayoshi Tonouchi

Published Dec 18, 2006• 0 citations
Publisher

Abstract

The authors have studied the optical input interface for Nb single-flux-quantum (SFQ) circuits and demonstrated its operation using photomixing technique. Two tunable lasers of C band were used for photomixing. We adopted a multistage toggle flip-flop (TFF) circuit as the main part of the test circuit. As the first trial, we used lasers with wavelength difference of 0.044nm at around 1550nm, which corresponds to the laser beat frequency of 5.5GHz. The output signals from the 13- and 14-stage TFFs were observed and it showed the input SFQ frequency of 5.5GHz. Thus, the authors demonstrated the conversion of the optical signal to SFQ signal and succeeded in driving the SFQ circuit.

DOI
10.1063/1.2410216

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The authors have studied the optical input interface for Nb single-flux-quantum (SFQ) circuits and demonstrated its operation using photomixing technique. Two tunable lasers of C band were used for photomixing. We adopted a multistage toggle flip-flop (TFF) circuit as the main part of the test circuit. As the first trial, we used lasers with wavelength difference of 0.044nm at around 1550nm, which corresponds to the laser beat frequency of 5.5GHz. The output signals from the 13- and 14-stage TFFs were observed and it showed the input SFQ frequency of 5.5GHz. Thus, the authors demonstrated the conversion of the optical signal to SFQ signal and succeeded in driving the SFQ circuit.
We investigated interface circuits between a single-flux-quantum (SFQ) circuit and an adiabatic quantum-flux-parametron (AQFP) for their hybrid system. The target frequency of interface circuits is several GHz. The interface circuit that transmits a signal from the SFQ circuit to the AQFP gate (SFQ/AQFP) is realized by combining an SFQ toggle flip-flop (TFF) with the AQFP buffer. The bias margin of the SFQ TFF and the excitation current margin of the SFQ/AQFP interface are 2.47 mV ±24.7% and 1.36 mA ±8.82%, respectively. The interface circuit that transmits a signal from the AQFP to the SFQ circuit (AQFP/SFQ) was designed by using a high-sensitive mutually coupled dc/SFQ converter (MC-dc/SFQ) to detect magnetic flux signal output from the AQFP. The bias margin of the high-sensitive MC-dc/SFQ and the excitation current margin of the AQFP/SFQ are 2.88 mV ±13% and 1.6 mA ±18.8%, respectively. These interface circuits also allow us to use long-distance interconnection based on SFQ passive transmission lines between AQFP gates.
We report on the functionality of a Nb-based superconducting single flux quantum (SFQ) toggle flip-flop (TFF) circuit, comprising a complementary superconductor–ferromagnet–superconductor (SFS) Josephson π-junction. The SFS junction was used as a phase shifting element inserted in the storage loop of the TFF. The fabricated circuits demonstrated correct functionality with the operation parameter ranges of ± 20%. The application of SFS π-junctions makes the SFQ circuits very compact, may substantially improve their stability, and may also be suitable for integration with Josephson quantum circuits (qubits).
We investigated interface circuits between rapid single-flux-quantum (RSFQ) circuits and adiabatic quantum-flux-parametron (AQFP) circuits for a high-speed and low-power hybrid computing system. In addition, the interface circuits allow us to use long-distance interconnections based on single-flux-quantum (SFQ) passive transmission lines between AQFP gates. The target frequency of interface circuits is several gigahertz. There are two types of interface circuits. The RSFQ/AQFP interface circuit, which transmits a signal from RSFQ circuits to AQFP gates, was realized by coupling an RSFQ toggle flip-flop (TFF) to an AQFP buffer gate. The simulated bias margins of the RSFQ TFF and the excitation current margin of the RSFQ/AQFP interface were 2.22 mA ± 24.7% and 1.71 mA ± 25.0%, respectively. The AQFP/RSFQ interface circuit, which transmits a signal from AQFP gates to RSFQ circuits, was designed by using a high-sensitive magnetically coupled dc/SFQ converter (MC-dc/SFQ) to detect an output current of an AQFP buffer gate. The simulated bias margins of the MC-dc/SFQ and the excitation current margin of the AQFP/RSFQ interface were 0.558 mA ± 20.5% and 1.95 mA ± 36.1%, respectively. We also fabricated and measured the interface circuits.
A single flux quantum (SFQ) logic cell library has been developed for the 10kA/cm2 Nb multi-layer fabrication process to efficiently design large-scale SFQ digital circuits. In the new cell library, the critical current density of Josephson junctions is increased from 2.5kA/cm2 to 10kA/cm2 compared to our conventional cell library, and the McCumber-Stwart parameter of each Josephson junction is increased to 2 in order to increase the circuit operation speed. More than 300 cells have been designed, including fundamental logic cells and wiring cells for passive interconnects. We have measured all cells and confirmed they stably operate with wide operating margins. On-chip high-speed test of the toggle flip-flop (TFF) cell has been performed by measuring the input and output voltages. The TFF cell at the input frequency of up to 400GHz was confirmed to operate correctly. Also, several fundamental digital circuits, a 4-bit concurrent-flow shift register and a bit-serial adder have been designed using the new cell library, and the correct operations of the circuits have been demonstrated at high clock frequencies of more than 100GHz.
High-speed logic operation of an output interface circuit for a single-flux-quantum (SFQ) system was demonstrated at a data rate of 5 Gb/s. Using NEC's 2.5-kA/cm/sup 2/ Nb junction process, we designed, fabricated, and tested the interface circuit consisting of a 2-b SFQ demultiplexer and two Josephson latching drivers. We verified the proper operation of the demultiplexer. The interface can convert 5-Gb/s SFQ-pulse data into two-channel 2.5-Gb/s return-to-zero data with an amplitude of approximately 6 mV.
A new generation of the Josephson digital circuits-rapid single flux quantum (RSFQ) devices-based on overdamped externally shunted high quality Nb-AlO x -Nb tunnel junctions have been designed, fabricated and experimentally investigated. All-refractory material 11-layer 5 mu m integrated technology has been successfully employed for the preparation of the RSFQ microcircuits. The T flip-flop has been demonstrated to operate properly up to clock frequencies of 100 GHz at 25% margins. The proper operation of the buffer stage for a one-directional SFQ pulse transmission at clock frequencies up to 125 GHz has been achieved. The possibilities to convert the information from the usual DC form to SFQ and vice versa have been demonstrated. An output signal in an SFQ/DC converter as high as 220 mu V has been measured. A new counter type A/D converter which includes a comparator and reversible binary counter with DC outputs has been fabricated and tested. The proposed ADC seems to be very promising for high-accuracy measurement of medium-bandwidth signals. The possibilities of creating a number of SFQ devices with outstanding parameters are discussed.