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IEEE Transactions on Applied Superconductivity

CMOS-to-SFQ Interface Circuits for RZ and NRZ Coded Signals Transformation

Siqi Li, Xiaoping Gao, Huanli Liu, Minghui Niu, Hui Zhang, Xue Zhang, Jie Ren

Published Mar 18, 2024• 3 citations
Publisher

Abstract

A hybrid computing system employing the superconductor central processing unit and semiconductor memory is a prospective strategy to boost speed and power performance. Aiming to convert coded signals at room temperature to single-flux-quantum (SFQ) logic signals in a cryogenic environment, this article presents two types of CMOS-to-SFQ interface circuits for return-to-zero (RZ) and nonreturn-to-zero (NRZ) coded signals transformation. One can double the data rate (DDR) of bipolar RZ signals, and the other can decode unipolar and polar NRZ signals. In the simulation using parameters of the SIMIT Nb03 process, both the interface circuits have up to 20 GHz sampling frequency, more than ±30% bias current margin, and tolerance toward 20 dB SNR white noise. The DDR interface circuit can generate SFQ pulses at both edges of 1.4–2.6 mA bipolar RZ signal, and the decoding interface circuit can interpret 0.2–0.6 mA unipolar and polar NRZ signal into SFQ pulses. The test circuits have been fabricated under the SIMIT Nb03 6 kA/cm2process. In low-frequency measurement, the DDR interface circuit can convert 1.4–2.4 mA bipolar RZ signal, and the decoding interface circuit can convert 0.25–0.5 mA unipolar and polar NRZ signal with more than ±30% bias current margin. In high-frequency measurement, the DDR interface circuit shows an ability to convert a 3.33 GHz input signal.

DOI
10.1109/tasc.2024.3376983

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A hybrid computing system employing the superconductor central processing unit and semiconductor memory is a prospective strategy to boost speed and power performance. Aiming to convert coded signals at room temperature to single-flux-quantum (SFQ) logic signals in a cryogenic environment, this article presents two types of CMOS-to-SFQ interface circuits for return-to-zero (RZ) and nonreturn-to-zero (NRZ) coded signals transformation. One can double the data rate (DDR) of bipolar RZ signals, and the other can decode unipolar and polar NRZ signals. In the simulation using parameters of the SIMIT Nb03 process, both the interface circuits have up to 20 GHz sampling frequency, more than ±30% bias current margin, and tolerance toward 20 dB SNR white noise. The DDR interface circuit can generate SFQ pulses at both edges of 1.4–2.6 mA bipolar RZ signal, and the decoding interface circuit can interpret 0.2–0.6 mA unipolar and polar NRZ signal into SFQ pulses. The test circuits have been fabricated under the SIMIT Nb03 6 kA/cm2process. In low-frequency measurement, the DDR interface circuit can convert 1.4–2.4 mA bipolar RZ signal, and the decoding interface circuit can convert 0.25–0.5 mA unipolar and polar NRZ signal with more than ±30% bias current margin. In high-frequency measurement, the DDR interface circuit shows an ability to convert a 3.33 GHz input signal.
Interfaces between RSFQ circuits in the Return-to-Zero (RZ) and semiconductor circuits in the Non-Return-to-Zero (NRZ) mode are developed for data transmission at about 10 GHz clock frequencies reducing the errors owing to a finite sampling jitter of conventional room temperature equipment. A prototype of a NRZ output interface with the Nb-Al/sub 2/O/sub 3/-Nb technology has been simulated, implemented and successfully tested at 100 MHz. The interface can easily be combined with a superconducting pulse amplifier for NRZ output signals in the range of several mV. Corresponding simulations and a layout of the amplifier are presented.
Superconducting computers can be realized using a Josephson-CMOS hybrid structure, combining the high speed and low power of single-flux quantum (SFQ) logic with the high integration density of CMOS technology. However, reliable interconnection between SFQ and CMOS circuits at cryogenic temperatures remains challenging due to low signal-to-noise ratio (SNR) and interference. To address these challenges, we propose a DC-biased SiGe BiCMOS interface that converts the 0.2 mV output of the SFQ/DC converter (Q2D) to 1.2 V for CMOS memory. A high-impedance voltage amplifier (VA) and a low-impedance transimpedance amplifier (TIA) were designed to optimize signal matching with the Q2D. The interfaces were simulated, fabricated, and tested at 4.2 K to evaluate their performance. Both analytical and experimental results demonstrate that the TIA significantly improves the SNR and enhances noise immunity during static random-access memory (SRAM) read/write operations, making it more effective than the VA for signal matching between the Q2D and CMOS circuits. This work presents a practcal solution for SFQ-CMOS interconnection, effectively addressing SNR and interference challenges and contributing to the development of scalable superconducting computing systems.
The high-speed operation of a one-channel output interface for a single-flux quantum (SFQ) system has been demonstrated. The interface consisted of a Josephson latching driver, a room-temperature semiconductor amplifier, and a decision circuit module. The Josephson latching driver was fabricated by using a 2.5-kA/cm/sup 2/ standard Nb junction process and used to amplify an SFQ pulse into a 5.5-mV level signal at 10 Gb/s. The interface converted the SFQ pulse signal into a nonreturn-to-zero signal having an amplitude of 1 V at 10 Gb/s.
Abstract Conventional interfaces for a Josephson-CMOS hybrid system typically rely on Josephson latching drivers (JLDs) or SQUID (Superconducting Quantum InterferenceDevice) stacks to convert weak signals, which are then connected to additional amplifiers providing outputs of 1.2 V or 1.8 V. JLDs output tens of millivolts but require AC bias and precise clock alignment. SQUID stacks reach frequencies of tens of GHz but output few millivolts voltages and occupy large area. To address these challenges, an interface based on SiGe BiCMOS(Silicon-Germanium Bipolar Complementary Metal-Oxide-Semiconductor) has been designed, fabricated, and tested. Fabricated using the 130 nm SiGe BiCMOS process, the interface converts 200 μV voltage signals to 1.2 V and consumes only 386 μW per channel at 4.2 K. In low-frequency measurement, the hybrid system supports 21-channel signals conversion without requiring additional CMOS amplifiers, simplifying cryogenic system design. Advantages include eliminating the need for AC bias and clock alignment, while drawbacks like limited speed are also discussed. This technology facilitates the practical application of multichannel superconducting computers and other applications that require efficient signal conversion, making it one of the most promising interface solutions for the hybrid system.
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.
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.