Relay-Version: version B 2.10 5/3/83; site utzoo.UUCP Path: utzoo!mnetor!seismo!rutgers!sri-unix!ctnews!pyramid!oliveb!intelca!mipos3!cpocd2!howard From: howard@cpocd2.UUCP (Howard A. Landman) Newsgroups: comp.arch,comp.lsi Subject: Re: Josephson Junction computers Message-ID: <504@cpocd2.UUCP> Date: Mon, 16-Mar-87 14:21:31 EST Article-I.D.: cpocd2.504 Posted: Mon Mar 16 14:21:31 1987 Date-Received: Wed, 18-Mar-87 06:38:55 EST References: <8702240351.AA00239@angband.s1.gov> <7718@utzoo.UUCP> <492@cpocd2.UUCP> <1486@vice.TEK.COM> Reply-To: howard@cpocd2.UUCP (Howard A. Landman) Organization: Intel Corp. ASIC Services Organization, Chandler AZ Lines: 40 Xref: mnetor comp.arch:594 comp.lsi:63 In article <1486@vice.TEK.COM> keithl@vice.TEK.COM (Keith Lofstrom) writes: >Advantages: > JJ's prime advantage is their very low power, allowing them to be placed >closely together. With proper design, you can design JJ gates with switch >energies of just a few kT. JJ gates can be made to match transmission lines > - hard to do at low power with semiconductor circuits requiring >100mV >logic swings. One problem I failed to mention in my previous posting is data storage. While JJ gates are very low power, the standard way to store a bit in a JJ circuit is to put a current into a superconducting loop. There's a really interesting feature to this current, which is that it is equivalent to some "trapped" magnetic flux through the loop. Now, this flux is governed by the simple Bohr-Sommerfeld quantization that most of you first heard about in the Bohr model of the hydrogen atom: there are discrete energy levels that can be trapped. Thus the minimum you can switch is a single flux quantum; and there exist JJ circuits that do just that! However, the quantization levels depend on the size of the loop, and increase as the loop gets smaller (remember "particle in a box"?). This is all freshman physics, but the implication is that the amount of energy required to store one bit of information goes *UP* as JJ circuits get smaller, and hence the power consumption goes up, and the power density (power per area) goes *WAY* up. Hence JJ cicuits will not scale gracefully to smaller sizes. They are already "quantum limited". This same effect, taken the other way to large loops (say 1 meter across), is what makes JJ flux detectors so extremely sensitive. >Imagine what superconducting transmission lines can do for you here (Note: >superconducting wires are still dispersive - at a Terahertz or so). As I mentioned before, not much. It's easy to get transmission speeds of .5 to .8 the speed of light using non-superconducting wires. Try teflon twin-ax driven by ECL, for example, as used in large Amdahl and Fujitsu machines. Not even superconductors can get > 1.0. -- Howard A. Landman ...!intelca!mipos3!cpocd2!howard