Hi George, A question right up my alley! When you dope a semiconductor you are just providing more free electrons or holes, dependant on the dopant, to reduce the resistivity. This is illustrated by the increases the drift current through the material., At some point the doping becomes degenerate, at which time the material is less silicon and more dopant. Basically increasing the doping of a semiconductor makes it behave more like a metal, to the point of degeneracy then it changes back.. This method of degenerate doping can also be used to create an insolating layer in a silicon substrate for isolation. There are a very limited number of pure metals that are superconductors, Niobium the most commonly used and the one with the highest transition temperature, 4K. Others are Aluminum and Tin. The transition temperature is the temperature at which a material becomes superconducting. If you look at a resistivity versus temperature plot of most materials and extrapolate to 0 K the resistivity does not go to zero at 0 K, even superconductors above Tc. A superconductor will look like a normal metal then transition, in a step wise fashion(the transition region), to 0 resistance, at Tc, under DC conditions. Since we use the interconnects of a chip, package, or system at frequencies other than DC there is also another interesting behavior. Superconductors actually have measurable loss at frequencies above DC. These losses become significant and then pass those of cooled Copper or Aluminum at about 100GHz for temperature of 77K (Liquid Nitrogen). So the interesting thing is that cryo-cooled normal metals actually perform better at high frequencies than high temperature or low temperature superconductors. Ramo, Whinnery and VanDuzer, 3rd edition, have an excellent plot of this on page 152 figure 3.16b. BTW, this was one of the areas of my research. Hope this helps. Regards ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ NORTH EAST SYSTEMS ASSOCIATES, INC ------------------------------------- "High Performance Engineering & Design" ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ Dr. Edward Sayre 3rd e-mail: esayre3@xxxxxxxx NESA, Inc. http://www.nesa.com/ 5 Lan Drive, Suite 200 Tel +1.978.392-8787 x 218 Westford, MA 01886 USA Fax +1.978.392-8686 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ At 03:30 PM 3/21/2003 +1100, you wrote: > Hi all, > If doping increases the conductivity of Silicon , why cant we > attain superconductivity with heavy doping of a material? Whats the > phenomenon that limits the conductivity if we actually do increase > carriers by doping? > >Thanks and regards, >George. > > > >_____________________________________________________________ >Get 25MB, POP3, Spam Filtering with LYCOS MAIL PLUS for $19.95/year. >http://login.mail.lycos.com/brandPage.shtml?pageId=plus&ref=lmtplus >------------------------------------------------------------------ >To unsubscribe from si-list: >si-list-request@xxxxxxxxxxxxx with 'unsubscribe' in the Subject field > >or to administer your membership from a web page, go to: >//www.freelists.org/webpage/si-list > >For help: >si-list-request@xxxxxxxxxxxxx with 'help' in the Subject field > >List archives are viewable at: > //www.freelists.org/archives/si-list >or at our remote archives: > http://groups.yahoo.com/group/si-list/messages >Old (prior to June 6, 2001) list archives are viewable at: > http://www.qsl.net/wb6tpu > ------------------------------------------------------------------ To unsubscribe from si-list: si-list-request@xxxxxxxxxxxxx with 'unsubscribe' in the Subject field or to administer your membership from a web page, go to: //www.freelists.org/webpage/si-list For help: si-list-request@xxxxxxxxxxxxx with 'help' in the Subject field List archives are viewable at: //www.freelists.org/archives/si-list or at our remote archives: http://groups.yahoo.com/group/si-list/messages Old (prior to June 6, 2001) list archives are viewable at: http://www.qsl.net/wb6tpu