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физически наблюдаемого проявления волновой природы квантовых систем являются интерференционные пики электронного пучка в эксперименте с двумя щелями. Картина очень похожа на полученную дифракцией классических волн.

      F (x) может быть постоянной величиной от времени для волновой функции стационарного уравнения Шредингера. Для эволюции волновой функции ψ (n,m,t) во времени t, требование постоянства во времени F (x) вполне справедливо для выбранной суперпозиции исследуемого квантового процесса. С вопросами суперпозиции мы ознакомимся ниже.

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