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Superconducting Technology Assessment - nitrd

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Significant activity in the area of digital superconductive electronics has long existed in the United States, Europe,<br />

and Japan. Over the past 15 years, Nb-based integrated circuit fabrication has achieved a high level of complexity<br />

and maturity, driven largely by the promise of ultra-high-speed and ultra-low-power digital logic circuits. An<br />

advanced process has one (JJ) layer, four superconducting metal layers, three or four dielectric layers, one or more<br />

resistor layers, and a minimum feature size of ~1 µm. Today’s best superconductive integrated circuit processes are<br />

capable of producing digital logic IC chips with 10 5 JJs/cm 2 . Recent advances in process technology have come from<br />

both industrial foundries and university research efforts, resulting in reduced critical current spreads and increased<br />

circuit speed, circuit density, and yield. On-chip clock speeds of 60 GHz for complex digital logic and 750 GHz for<br />

a static divider (toggle flip-flop) have been demonstrated. Large digital IC chips, with JJ counts exceeding 60,000,<br />

have been fabricated with advanced foundry processes. IC chip yield is limited by defect density rather than by<br />

parameter spreads. At present, integration levels are limited by wiring and interconnect density rather than by junction<br />

density, making the addition of more wiring layers key to the future development of this technology.<br />

Recent advances in process technology have come from both<br />

industrial foundries and university research efforts.<br />

Nb-based superconductive IC chip fabrication has advanced at the rate of about one generation, with a doubling<br />

of J c , every two years since 1998. Increasing J c enables increasing digital circuit speed. This is illustrated in Figure<br />

4-3, a plot of static divider speed from several of sources versus J c. Points beyond 8 kA/cm 2 represent single<br />

experimental fabrication runs, not optimized processes. Theoretically, divider speed should approach 1,000 GHz<br />

(1 THz), however, the process and layout must be optimized to reduce self-heating effects in junctions with J c beyond<br />

100 kA/cm 2 . The first generation Nb process discussed in Section 4.6 should be based on 20 kA/cm 2 , 0.8 µm<br />

diameter junctions with six superconducting metal layers. Static dividers fabricated in this process have achieved<br />

speeds of 450 GHz, which should enable complex RSFQ circuits with on-chip clock rates of 50 to 100 GHz.<br />

Figure 4-3. Demonstrations of RSFQ circuit speed with increasing J c<br />

80<br />

f max (GHz)<br />

1000<br />

900<br />

800<br />

700<br />

600<br />

500<br />

400<br />

300<br />

200<br />

1 10<br />

J (kA/cm c<br />

100<br />

2 100<br />

)

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