First, the rate of change of the mean atomic excitation energy is now a function of the distance to the boundary and it dies off in an oscillatory way the boundary is approached.

第一，原子平均激发能量变化率是原子到板的距离的函数，并且当靠近板时以振荡行为消失。

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First, the rate of change of the mean atomic excitation energy is now a function of the distance to the boundary and it dies off in an oscillatory way the boundary is approached.

第一，原子平均激发能量变化率是原子到板的距离的函数，并且当靠近板时以振荡行为消失。

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