Quantum Formulation of X-Ray Interactions with Matter
摘要
This chapter introduces the quantum theoretical formulation of photon-matter interactions, constituting the first of five chapters in Vol. II. The quantum approach has its roots in a foundational paper by Kramers and Heisenberg in 1925 [1], written just before the formulation of quantum theory. Two years later Dirac quantized the EM field and used first order perturbation theory to derive the quantum mechanical expression for x-ray absorption and emission [2], later called by Fermi “Golden rule number 2” [3]. Shortly thereafter Dirac re-derived the Kramers–Heisenberg formula in the second order quantum formulation [4]. We shall here use this modern quantum version of the theory and, giving credit to its architects, refer to it as the Kramers–Heisenberg–Dirac (KHD) theory.