45 T. This reveals a filling-factor-dependent, multicomponent anticrossing structure of the
Raman G peak, resulting from magnetophonon resonances between magnetoexcitons and
E 2 g phonons. This is explained with a model of Raman scattering taking into account the
effects of spatially inhomogeneous carrier densities and strain. Random fluctuations of strain-
induced pseudomagnetic fields lead to increased scattering intensity inside the anticrossing …