ELECTRON COMPUTING

WE KNOW THAT electron criuclating and protn repletion but if we consider repelction zero then electron needs bar heres we consider that there is extenal force is working and electron electron 2 ,6,8,18 so here we have to consider a constant force is working that called grvaity we consider grvaity is working between electron to mange them sleves in one cycle to naoteh cycle atom grvaiyt is working 2 pie r.g f=2 pie r.ga sin theta f=2pie r.ga cos theta f(-)=-2pie r.ga sin theta f(-)=-2pie r.ga cos theta interelatve force is working then here is working then thoughs so two electron force is working between then that called in (cos theta sin theta) (-sin theta -cos theta) -(cos squre theta + sin squqre theta) = -1 so heres with 2 electron -1*-1 =1 (bit got from heres) 6 -1*-1*-1*-1*-1*-1=1 so electron here is shape that eletcron living in two repletion one is zero and another is 1 and thirs state is -1 levae the class of theris so two electron ga(0g 0g)interaction with each other of elctron under gravity (1g 1g) or (0g 1g) firts equation (1g 0g) then heres is working because 1 is coming by -1 multilication it also come by 1 multipciation so here is eelctron third state is getting multiplicaitve so we cosndier in place of -1 there is plus 1 so six electron (0g 1g) (0g 1g 0g 1g 0g 1g) (1g 0g) (1g 0g 1g 0g 1g 0g) (0g 1g) or (1g 0g) (0g 1g) (1g 0g) then we get the bit this is the next bit of six electron in cirnuclations soa gates will work same ly row to columns ways (0g 1g 0 0 0 0) 2 elctron bit six electron bit (0g 1g 0g 1g 0g 1g) (1g 0g 0 0 0 0) row to column and operator (1g 0g 1g 0g 1g 0g) then answer will come of them

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