Superconducting Technology Assessment - nitrd
Superconducting Technology Assessment - nitrd
Superconducting Technology Assessment - nitrd
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Superconductor Integrated Circuit<br />
Fabrication <strong>Technology</strong><br />
LYNN A. ABELSON AND GEORGE L. KERBER, MEMBER, IEEE<br />
Invited Paper<br />
Today’s superconductor integrated circuit processes are capable<br />
of fabricating large digital logic chips with more than 10<br />
K gates/cm P . Recent advances in process technology have come<br />
from a variety of industrial foundries and university research<br />
efforts. These advances in processing have reduced critical current<br />
spreads and increased circuit speed, density, and yield. On-chip<br />
clock speeds of 60 GHz for complex digital logic and 750 GHz for<br />
a static divider (toggle flip-flop) have been demonstrated. Large<br />
digital logic circuits, with Josephson junction counts greater than<br />
60 k, have also been fabricated using advanced foundry processes.<br />
Circuit yield is limited by defect density, not by parameter spreads.<br />
The present level of integration is limited largely by wiring and<br />
interconnect density and not by junction density. The addition<br />
of more wiring layers is key to the future development of this<br />
technology. We describe the process technologies and fabrication<br />
methodologies for digital superconductor integrated circuits and<br />
discuss the key developments required for the next generation of<br />
100-GHz logic circuits.<br />
Keywords—Anodization, critical current, flip-flop, foundry, interlevel<br />
dielectric, Josephson junction, niobium, niobium nitride,<br />
100-GHz digital logic, photolithography, planarization, quantum<br />
computing, qubit, rapid single-flux quantum (RSFQ), reactive ion<br />
etch, resistor, SiOP, superconductor integrated circuit, trilayer.<br />
I. INTRODUCTION<br />
In the past ten years, low-temperature superconductor<br />
(LTS) integrated circuit fabrication has achieved a high level<br />
of complexity and maturity, driven in part by the promise<br />
of ultrahigh speed and ultralow power digital logic circuits.<br />
The typical superconductor integrated circuit has one<br />
Josephson junction layer, three or four metal layers, three<br />
or four dielectric layers, one or more resistor layers, and a<br />
minimum feature size of 1 m. Niobium, whose transition<br />
temperature is 9 K, has been the preferred superconductor<br />
Manuscript received December 3, 2003; revised April 16, 2004.<br />
L. A. Abelson is with Northrop Grumman Space <strong>Technology</strong>, Redondo<br />
Beach, CA 90278 (e-mail: lynn.abelson@ngc.com).<br />
G. L. Kerber was with Northrop Grumman Space <strong>Technology</strong>, Redondo<br />
Beach, CA 90278 USA. He is now in San Diego, CA 92117 USA (e-mail:<br />
george.kerber@glkinst.com).<br />
Digital Object Identifier 10.1109/JPROC.2004.833652<br />
0018-9219/04$20.00 © 2004 IEEE<br />
due to its stable material and electrical properties, and ease<br />
of thin-film processing. The Josephson junction, which is<br />
the active device or switch, consists of two superconducting<br />
electrodes (niobium) separated by a thin ( 1 nm thick)<br />
tunneling barrier (aluminum oxide). Josephson junctions,<br />
fabricated in niobium technology, exhibit remarkable electrical<br />
quality and stability. Although the physical structure<br />
of the Josephson junction is simple, advanced fabrication<br />
techniques have been developed to realize a high level of<br />
integration, electrical uniformity, and low defects. Today,<br />
niobium-based VLSI superconductor digital logic circuits<br />
operating at 100 GHz are a near-term reality and could have<br />
a significant impact on the performance of future electronic<br />
systems and instrumentation if the rate of innovation and<br />
progress in advanced fabrication continues at a rapid pace.<br />
The promise of ultrahigh speed and ultralow power<br />
superconductor digital logic began in the mid-1970s with<br />
the development of Josephson junction-based single-flux<br />
quantum (SFQ) circuits. In 1991, Likharev and Semenov<br />
published the complete SFQ-based logic family that they<br />
called rapid SFQ (RSFQ) logic [1]. In 1999, researchers<br />
demonstrated a simple RSFQ T flip-flop frequency divider<br />
(divide-by-two) circuit operating above 750 GHz in niobium<br />
technology [2]. In terms of raw speed, RSFQ logic is the<br />
fastest digital technology in existence [3]. RSFQ logic gates<br />
operate at very low voltages on the order of 1 mV and require<br />
only about 1 W for even the fastest logic gates. As a result,<br />
on-chip RSFQ logic gate density can be very high even for<br />
100-GHz clock frequencies. RSFQ logic is considered to be<br />
the prime candidate for the core logic in the next generation<br />
of high-performance computers [4]–[7] and is recognized<br />
as an emerging technology in the Semiconductor Industries<br />
Association roadmap for CMOS [8]. Recently a prototype<br />
of an 8-b, RSFQ microprocessor, fabricated in the SRL<br />
(formerly NEC) 2.5-kA/cm process (see Table 1), demonstrated<br />
full functionally at a clock frequency of 15.2 GHz<br />
with power consumption of 1.6 mW [9]. Even smaller scale<br />
applications, such as ultrawide band digital communication<br />
PROCEEDINGS OF THE IEEE, VOL. 92, NO. 10, OCTOBER 2004 1517