![]() The scattering of photons from charged particles is called Compton scattering after Arthur Compton who was the first to measure photon-electron scattering in 1922. When the incoming photon gives part of its energy to the electron, then the scattered photon has lower energy and according to the Planck relationship has lower frequency and longer wavelength. The wavelength change in such scattering depends only upon the angle of scattering for a given target particle. The constant in the Compton formula above can be written 光子与带电粒子的散射称为康普顿散射,这是以首先在1922年测量光子-电子散射的Arthur Compton命名的。当入射光子将部分能量传递给电子时,散射后的光子能量较低,根据普朗克关系,其频率也较低,波长更长。这种散射中波长的变化仅取决于散射角和目标粒子。上述康普顿公式中的常数可以写成
![]() and is called the Compton wavelength for the electron. The formula presumes that the scattering occurs in the rest frame of the electron. 并且称为电子的康普顿波长。该公式假定散射发生在电子的静止参考系中。
This exploration is designed to accept values for the input wavelength or energy and the angle of scattering. Unspecified parameters will default to the case of molybdenum K-alpha xrays scattering at 90 degrees, one of Compton's historical results. Any of these input values can be changed. 此探索旨在接受输入波长或能量以及散射角度的值。未指定的参数将默认为钼K-alpha X射线在90度散射的情况,这是康普顿历史结果之一。这些输入值中的任何一项都可以进行更改。
以及散射光子的能量是 |
Index Great experiments of physics Reference: Compton 索引 伟大的物理实验 参考:康普顿 | ||||
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