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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]   
      
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