摘要
In quantum mechanics, the ability to simultaneously pre- dict the precise outcomes of two conjugate observables, such as the position and momentmn, for a particle is re- stricted by the uncertainty principle [1]. For example, the more precisely the location of the particle is determined, the less accurate the momentum determination will be. Originally given by Heisenberg, the uncertainty principle is best known as the Heisenberg-Robertson [2] commu- tation ARAS ≥1/2（[R,S]）I, with AR（AS） representing the standard deviation of the corresponding variable R （S）.
In quantum mechanics, the ability to simultaneously pre- dict the precise outcomes of two conjugate observables, such as the position and momentmn, for a particle is re- stricted by the uncertainty principle [1]. For example, the more precisely the location of the particle is determined, the less accurate the momentum determination will be. Originally given by Heisenberg, the uncertainty principle is best known as the Heisenberg-Robertson [2] commu- tation ARAS ≥1/2（[R,S]）I, with AR（AS） representing the standard deviation of the corresponding variable R （S）.
