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SEMICONDUCTOR PHOTONICS LAB., HANYANG UNIV 3.1 Photons 3.1.3 Compton Scattering Scattering of an x-ray photon by a free electron in a conductor When the kinetic energy of electron is determined From the conservation of linear momentum law As if it were particle, we need to consider its energy and momentum
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SEMICONDUCTOR PHOTONICS LAB., HANYANG UNIV Simplified schematic diagram of the Compton experiment Result of Compton experiment
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SEMICONDUCTOR PHOTONICS LAB., HANYANG UNIV Momentum conservation along y-axis Momentum conservation along x-axis From above, unmeasurable angle Ф must be eliminated For X-ray photon energy
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SEMICONDUCTOR PHOTONICS LAB., HANYANG UNIV But ’ is only slightly greater than so that ’ is slight smaller than unity and ’ is slightly larger than unity.
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SEMICONDUCTOR PHOTONICS LAB., HANYANG UNIV 3.1.4 Black Body Radiation Small hole acts as black bodyInserting cannot escape to outside
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SEMICONDUCTOR PHOTONICS LAB., HANYANG UNIV Classical physics Probability of distribution Average E in black body Quantum physics Average E in black body (Density of E = Degree of freedom · average E)
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