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Superconducting Technology Assessment - nitrd

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Single flux quantum is the latest generation of superconductor devices and circuits. The I-V curve for SFQ operation<br />

is single-valued and the devices are DC powered. A fundamental property of JJs in the voltage state is that the junction<br />

produces precisely reproducible SFQ pulses at a frequency proportional to the voltage:<br />

(2)<br />

where Φ 0 = 2.07 mV-ps is the magnetic flux quantum. Each pulse represents one quantum of magnetic flux, 2.07<br />

x10 -15 Webers, passing through the junction. At 100 µV, the SFQ frequency is 50 GHz. Thus, invisible in the DC<br />

characteristics, the junction DC voltage is the result of generating identical SFQ pulses according to Eq. (2). A 2 ps<br />

pulse is approximately 1 mV. In SFQ circuits, each switching junction is associated with a small inductor L that can<br />

compress and store a flux quantum. A parameter β L~ 1 defines the relation between β L and I C,<br />

(3)<br />

Switching time is a critical factor for digital applications; the minimum pulse width and maximum frequency are<br />

limited by parameters J C,I C, C’, and R, where C’ is the specific capacitance of the junction and R is generally an<br />

external shunt resistance. SFQ junctions are designed for optimal speed (i.e., near critical damping). An external<br />

shunt resistor is used to insure that β C ~ 1. Then, the SFQ pulse width is:<br />

(4)<br />

Thus, the maximum operating frequency scales as J C 1/2 . Figure 3 shows that the measured speed of asynchronous<br />

flip-flops, the simplest SFQ logic circuit, follows this rule.<br />

Figure 3. Measured speed of static dividers varies as J C 1/2 .<br />

f max (GHz)<br />

1000<br />

900<br />

800<br />

700<br />

600<br />

500<br />

400<br />

300<br />

200<br />

100<br />

1 10 100<br />

J c (kA/cm 2 )<br />

149

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