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|    sci.chem    |    Chemistry and related sciences    |    55,615 messages    |
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|    Message 54,990 of 55,615    |
|    Treon Verdery to All    |
|    Making large quantities of muons for muo    |
|    14 Aug 22 01:53:35    |
      From: treon3verdery@gmail.com              Muon atoms are 200 times smaller than electron atoms, thus in few-atom       transistors like carbon nanotube and fullerene transistors each muonic atom,       like a carbon atom, is 200 times smaller, providing about seven halving of       transistor sizes with one        technology, muonic semiconductors. At a different muonic semiconductor, a       multi 3d/2d charge shape field effect transistor muons can give the FET 2^200       different analog like shapings of the charge in the transistor due to muon       atoms being 200 times        smaller, thus if the analog field shape of an FET can be read it can contain       more separate bits of information in one transistor than the largest 2020AD       CPU. To do muonic semiconductors a source of muons, produced in large       quantities as cheaply as        possible is to use a laser striking a foil machines, but with new foil       replacements. Metal hydrides like palladium hydride store hundreds of times       their own volume in hydrogen atoms, fully filling palladium hydride with       hydrogen gas then using it to        receive laser-on-foil shock energy delivers laser shock energy to hundreds of       times more nuclei this way, which generates particles (kaons and pions) that       turn into directionally motioned muons. To create the highest laser on foil       shockwave energy at        published femtosecond laser pulse duration muon generators it is possible       overlapping nodal waves can be used. At 2D a central laser dot inside a 6       laser dot perimeter could create a laser shock overlapping pulse 7 additive       peak amplitudes stacked high.        This much larger amount of energy per foil atom could cause a variety of       effects like more muons generated from more nuclei fused, to higher velocity       muons, to some preferred ratio between muons and some other particle or       radiation being generated to        make high capacity laser foil muon generators physiologically harmless. 3D       laser on foil shockwave amplitude stacking is also possible. Right after the 7       laser spot hologram could, various hundreds or thousands deeper in the foil       could be another        location for a second focused laser beam, whether a half-cup parabolic shape       with its shockwave focus pointed towards the 7 stack central beam high       amplitude shockwave area, or a kind of multihundred laser spot lace doily with       all the beams converging on        the central beam of the seven spot. Along with human designs for shockwave       concentrators genetic algorithms running physics software could find variously       the most intense combined laser foil shock, the most kaon/pion/muon generating       laser foil shock, the        most physiologically harmless high muon production shock. Engineers would       design and contribute growthful GA seeds like facing the foil with a metal       transparency grating, or its opposite highest absorption morphology. Noting       sequential layers of        electroplating or electroless plating to build up the foil gratings,       refractors, and reflectors, and even negative refractive index superlenses       could be plated as layers to make a laser percussing foil. It is possible that       flinging nuclei together to        collide them first uses energy sufficient to neutralize crystal lattice and       electron orbital energy. Making the surface of the laser foil be liquid metal       at STP obviates that energy. To make palladium hydride or other metal hydride       liquid at STP,        alloying with eutectic gallium indium could be possible. Another approach is       simply to use a second broad beam laser to physically warm say the topmost 40       micrometers of hydrogen saturated palladium to be at unalloyed liquid metal       temperatures. Another        possibility is completely liquefying the palladium or other metal hydride and       have it coat a thicker rigid easy to handle zirconium or beryllium oxide base       foil/support. Zirconium is transparent to neutrons so it might omit       interacting with muon        generating kaons and pions. After a stream of muons is generated, possibly       three orders of magnitude more from the three orders of magnitude more of       palladium hosted hydrogen atoms, whose muon production could double again if       two nucleon deuterium is        hosted by the metal hydride, and, multiplied by 14 with the 2D center hexagon       overlap, or multiplied by 28 with a 3D depthy half cup reflector, or       multiplied by 280 with saggital depth muliple half cup reflectors and doilies,       doubled from using        metamaterials at the foil, and raised 1/3 from genetic algorithm optimization       then each million muons generated at a previous unenhanced foil would now make       1.4*10^6 times more muons or 1.4 trillion muons.              To make even more muons change the pulse length from 7 published femtoseconds       to 1 femtosecond, and at a 3 cm diameter foil percuss using 1024 nm frequency       beams .5 micrometers apart to make it so 3 micrometers wide hosts 2 beams, and       the 2 million        separate beams at the diameter makes a total complete parallel beam count near       3.14 trillion laser spots. 1 quadrillion laser percusses per second (1       femtosecond each) makes the 1.4 trillion * 1 quadrillion pulses per second       create 1.4 *10^25 muons in a        directional stream, about 1100-1400 farads of muons. If instead of 100% duty       cycle the laser only pulses 1% as often to keep long lived and cool then 11-14       farads of muons are produced, sufficient for many large multibillion or       trillion element        semiconductor chips that utilize the muon's 200 times smaller size to do       computations              Some other muon generating technologies are: cone or windsock shaped foil,       this uses the same diameter beam entrance as a flat laser foil disk but easily       exposes 14-16 times as much foil surface to lasers, and laser numbers could be       multiplied with 16 to        make lots more muons.              Well known to muon producers and published is how superdense hydrogen exists       and can be used as a laser foil. My metal hydride hosting hydrogen gas is       hundreds of times less dense than a superdense hydrogen foil. C24 rolled up       ball deuterium instead of        hydrogen alkane wax is another hydrogen dense possible foil that is unfussy at       STP                     [continued in next message]              --- SoupGate-Win32 v1.05        * Origin: you cannot sedate... all the things you hate (1:229/2)    |
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