frequently interesting to know how a system behaves under some disturbance. These disturbances are typically encoded as operators. f, (æ)Orb(x)dx may be interpreted as the probability of finding the system (x) in the eigenfunction , (x) after being acted on by the disturbance O. Begin with the system in state n =1 and compute the probability that the system is found in some state n + 1 under the action of the operator Qa, where Q is just a constant. In the case of atomic systems, such operators are known as dipole operators and transitions induced by them are called dipole induced transitions. Repeat this problem with the operator e-/L instead.
frequently interesting to know how a system behaves under some disturbance. These disturbances are typically encoded as operators. f, (æ)Orb(x)dx may be interpreted as the probability of finding the system (x) in the eigenfunction , (x) after being acted on by the disturbance O. Begin with the system in state n =1 and compute the probability that the system is found in some state n + 1 under the action of the operator Qa, where Q is just a constant. In the case of atomic systems, such operators are known as dipole operators and transitions induced by them are called dipole induced transitions. Repeat this problem with the operator e-/L instead.
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