We have observed magnetic-field-induced charged excitonic transitions from one-side-modulation-doped Al x Ga 1−x As/ GaAs asymmetric double quantum wells ͑ADQWs͒ where two low-energy conduction subbands e1 and e2 are coupled strongly, whereas the heavy-hole ground state hh1 is localized mostly in a quantum well.In the presence of a magnetic field applied parallel to the growth axis, the photoluminescence spectrum of the e1-hh1 transition develops into a Landau fan for filling factors of Ͼ 2. However, at Ͻ 2, the lowest Landaulevel ͑LL͒ transition reveals the charged-exciton behavior with an abrupt changeover in the field dependence of the transition energy, whereas the intensities of other LL transitions in the same Landau fan diminish. When the density of free electrons in the ADQWs is about 1.4ϫ 10 11 cm −2 , a new charged excitonic e2-hh1 transition also appears in the + polarization at Ͻ 2.The many-body interaction of a two-dimensional electron gas ͑2DEG͒ in modulation-doped quantum wells ͑QWs͒ has been the subject of extensive investigations in the past years. 1-9 The photoluminescence ͑PL͒ spectroscopy is a useful tool in studying the many-body effect on interband optical transitions in QWs. In particular, a number of PL investigations 10-13 have observed that at a filling factor ͑=n e h / eB͒ of 2 ͑here n e , h, and B denote the electron density, the Planck constant, and the magnetic field, respectively͒, there is an abrupt change in the slope of the energy of the lowest Landau-level ͑LL͒ transition with line narrowing, indicating the formation of 2DEG-hole complexes. The transformation from a LL behavior to an excitonic one for Ͻ 2 has been explained by two different interpretations.According to an interpretation in terms of the screening effect, 4 the transition of electron-hole ͑e-h͒ plasma into exciton, the so-called exciton-Mott transition, occurs when the density of plasma is decreased below a critical value. A similar transition can occur in QWs containing 2DEG and a photogenerated hole when the density of electrons is decreased. At a high electron density of n e ജ 1/a B 2 ͑here, a B is the Bohr radius of exciton in the QW͒, the e-h Coulomb interaction is screened effectively by free carriers, resulting in the prohibition of exciton formation. The critical electron density for the transition of electron-plasma into exciton increases in the presence of a magnetic field. Since the magnetic field shrinks the wave function of an electronic bound state, the screening effect on the e-h Coulomb interaction is reduced, allowing the formation of many-electrons-hole complexes such as X − the negatively charged exciton. 14,15 According to this mechanism, there is no difference between symmetric and asymmetric QWs in the changeover from a LL behavior to an excitonic behavior.On the other hand, a rather recent theory explains the abrupt changeover from LL behaviors to excitonic behaviors in both energy and linewidth as a consequence of hidden symmetry 11 ͑HS͒ inherent in a symmetric 2DEG system in strong magneti...