Atom quantom computing

how we could achidve this by junctioni we have two atom first we single one atom and then we did from nucleus to outershells spectrscopy and we differtitate this spectrscopy single electron base to its spin nagure we track single electron spin nature in whole cycle from nuclie to outershells now all electron comes underspectroscopy we convert this in wave lenth of different shells comes under an spectroanyizer or photon beam fecorder of step of single eelectron simultaneously state so its a graph bdcause electron is slining it gives simultandously state we record all stayes after anlyizer then we make 0 1 gap with photn beam recorder by micdoelectron second ahead we drive photon beam recorder to catch the state or inclined the state by stored junctioned photon beam recorder of electron proton nehutron now we could make qubit by photon beam recorder 0and 1 state means by photon bea. recorder inclinatipns and nucleous denstiy mass calculator and electron mass caculator njcleaous mass nucleaus have equal charge but different e.v. and elentront have different e.v. we radio waves to track or u.v. waves to calculate the mass differences then we create gwo form of qubit bh photon beam recorder we use with u.v. jintegral wave bh nucleaus and differtiae wave by electron if it not equal then it means there is quartz of nucleus qubit exists nucleus qubit comes by inclination uv and uv beam recorder with photon beam then we use laser beam and if both oscillation latitude and logitude are equal then it transformation to nucleus quanto. bit so tracks the beam of photon recorder again time stamp with u.v. recorder simjltaneously give us the quantom bit qubit now operatjon over qubit as sane as done hat