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Superconducting Technology Assessment - nitrd

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If technology, power, or cost limitations of superconductive clock speed optical technologies prove to be problematic,<br />

one possible option which should be held open would be to go to half clock rate transmission speeds. While this<br />

necessitates 2 bit buffer stages on the superconductive chip, this should not present any serious circuit design<br />

issues. If this approach were taken, 20-25 Gbps opto-electronic components could be used, which should be much<br />

more readily achievable within the target time frame of 2010 for a demonstration system.<br />

It is assumed throughout this chapter that the word width is 64 bits; the use of a 72 bit wide word so that error<br />

correction lines can be included in the data transmission is not an issue.<br />

3.2 ISSUES OF USING OPTICS AT 4K<br />

Given the use of very low power consumption of superconductive processors, the total power expended by the<br />

inter-level communications becomes a major issue in the system. With the power efficiency of refrigeration systems<br />

at 4K at 0.2%, because of the power demands, placing transmitting optics at 4K does not appear to be feasible,<br />

given the options considered below.<br />

218<br />

a) Placing optical sources at 4K is very power consuming. This is not only due to the power needed<br />

to drive one laser/line (x64 lines wide) but also for the wide bandwidth analog amplifiers required<br />

to raise the voltage levels from the (typically) 3 mV characteristic of Josephson Junction (JJ) technology<br />

to the 1.5 -2 volts required to drive the lasers. There are good fundamental reasons to expect that<br />

this will not change in the near future. The power goals of the current DARPA efforts are in the<br />

3-10 mW/Gbps range for 10-20 Gbps devices.<br />

b) Another option is to generate CW laser light at room temperature and transmit it by fiber into the 4K<br />

environment where it would be modulated by the data on each line and then transmitted on to the<br />

next level, located at room temperature. This would be a very attractive option if an optical modulator<br />

capable of operating at 50 Gbps, with a drive voltage (3-5 mV) consistent with superconductive technology<br />

existed. Currently available devices at 40 GHz require drive voltages in the range of 6 volts p-p, with rf<br />

drive powers of 700 mW into a 50 ohm line. Furthermore this would also require the use of high gain,<br />

large bandwidth amplifiers, not consistent with very low power consumption. There are modulator devices<br />

being considered which might have the desired properties. These include the coupling of micro-ring<br />

resonators to standard Mach-Zender modulators to reduce the modulation voltages required to less<br />

than one volt, and the development of micro-disk electro-absorption modulators operating at 40 Gbps.<br />

A third possibility is the use of VCSELs as modulators. In this case they act as injection locked lasers which<br />

have a higher modulation frequency capability than normal directly modulated lasers. The longer term<br />

possibilities include the use of organic glasses or polymers as either amplitude or phase modulators, which<br />

have much lower drive power requirements. or the use of magneto-optic modulators directly driven by<br />

the superconductive circuitry which would eliminate the need for any amplifiers. All of these alternatives<br />

are in a very early stage of research, and may not be available in time to meet the needs of the STA,<br />

with the currently planned funding rate. These options should be evaluated as they develop.<br />

c) Even if the desirable modulators discussed in section 3.2(b) were available, they may solve only half the<br />

problem. An optical receiver would also have to be placed at 4K to capture the data flow into the<br />

processor. Reasonable detected optical powers (200µw) would generate adequate voltage (100-160 mV)<br />

to drive the superconductive circuitry directly if a 100 ohm load and appropriate thresholding can be done.<br />

d) A simpler and more elegant solution is the use of amplifierless receivers. This is being explored for<br />

use in Si-CMOS devices by U.Texas at Austin. Since superconductive circuits are current driven, the<br />

superconductive logic could be driven directly with the detected current (100-160 µA) from the<br />

photodiodes. If this is achievable, it may be very advantageous to have the 300K to 4K interconnect<br />

be all optical, even if the reverse path is not. However, if any electronic amplification were required,<br />

the amplifier power would likely become a major thermal problem. This issue must be closely examined.

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