mapa mental quantica, Esquemas de Mecânica Quântica

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Interpretetion of wave function >robubly dencitity(in sense) of Finding a partie, so it should be rermalizea left cds fires-orde time ceritive Sehencinger Non-relaivir e fermal are represertarin, time [E Etr Rem crange tre normaize cond Expectation Cêsevoráie ia the averece of correaponding Ensemble everaga but time averege. Mechanical Quant lincertainty brinciple >enduer of the s>ancera denatian cf position ané momenrum s gerater tran half of hear Hillbert space, state vector, =conjugate a times b Commute Two operators share same eigenstate(degnerate ? ) mer product Hermitian Operator 1. enginvalues are real 2. enginstates are orthanoal 3. enginstates are completeness. (cannot prove in infintite dimension space) ED. ssa mermo if you measure Q(x, p) for a particle in the state Psi(x,t), The resul must be a eigenvalue q. n of the operator Q(x, p), corresponding probablity is [Cn| 2 or |Cz|"2dz Hisenberg's equation In Hisenberg picture, the state vector are time-independent The observable satisífies dajdt = ilhbar [H,A(t)]+partal A(t)partial t Uncertainty pri sigma a*sigma b = ( = mihtar. Le2 o teZeiyrzetera Spin Des des che quantum numbers mentioned above, There exist Spin 1/2 to mora interral freedom cf degree which may caused Two eng nstotes uz and down physical effect. | Addition cf angular momentum