Abstract
It is shown that the two-peak structure of the electron photoemission spectrum of Ce metal and its compounds may arise from two kinds of final states, those with and those without screening by a Ce electron in an impurity state. A comparison between theory and experiment reveals that the phase transition is accompanied by a very slight increase in conduction-electron population.
- Received 3 May 1982
DOI:https://doi.org/10.1103/PhysRevB.26.7052
©1982 American Physical Society