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⊥_values and indicated some anisotropy in the relaxation with respect to 〈110〉 directions. The largest relaxation anisotropy has been measured for sample Modu102 where R=11% and 23% for two orthogonal directions. The average relaxation has been used for the analysis of the optical data.
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The exciton binding energies can be calculated by the variational approach [Ref. 23]. In the simple hydrogenic model, light- and heavy-hole excitons would have energies of 0.7 meV and 1.4 meV, respectively, in bulk InAs. These values are respectively 4.2 meV and 6.2 meV in bulk InP and lie in between for the InAsP alloys. For finite quantum wells, the exciton energies should lie somewhere between the bulk values and the infinite well limit for which the two-dimensional (2D) Rydberg is four times the three-dimensionnal (3D) Rydberg. For example, in the GaAs/AlGaAs system, one finds an effective Rydberg of about 1.5 times the bulk value for wells less than 10 nm in thickness [Ref. 23]. This is in excellent agreement with our findings (Table I) and justifies our use of the less rigourous treatment which still preserves all of the essential physics.
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