A phenomenological approach is presented that allows one to model, and
thereby interpret, photoemission spectra of strongly correlated electron
systems. A simple analytical formula for the self-energy is proposed. This
self-energy describes both coherent and incoherent parts of the spectrum
(quasiparticle and Hubbard peaks, respectively). Free parameters in the
expression are determined by fitting the density of states to experimental
photoemission data. An explicit fitting is presented for the
La1−xSrxTiO3 system with 0.08≤x≤0.38. In general, our
phenomenological approach provides information on the effective mass, the
Hubbard interaction, and the spectral weight distribution in different parts of
the spectrum. Limitations of this approach are also discussed.Comment: 13 pages, 4 figures, IJMPB style (included