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TWO-DIMENSIONAL ELECTRON GAS 2009Interfer<strong>en</strong>ce of fractional microwave induced resistance oscillations withmagneto-intersubband oscillations in a bilayer systemMicrowave induced resistance oscillations (MIRO) whichevolve into “zero resistance states” (ZRS) in high mobilitysamples and for a suffici<strong>en</strong>tly high microwave power arecurr<strong>en</strong>tly both under experim<strong>en</strong>tal and theoretical investigation.They are governed by the ratio of the radiation frequ<strong>en</strong>cyω to the cyclotron frequ<strong>en</strong>cy ω c = eB/m ∗ , wherem ∗ is the effective mass of the electrons. With increasingmicrowave (MW) power, fractional MIROs (FMIROs)are observed which can be <strong>des</strong>cribed by ε = ω/ω c = n/mwith integer n and m and m ≥2. If a double quantum well(DQW) is exposed to microwave irradiation, photoresistancediffers from the single-subband case because of additionalintersubband scattering. MIS oscillations are increased/decreasedor show an inversion (peak flip) for lowfrequ<strong>en</strong>cies. The oscillating magnetoresistance is caused byan interfer<strong>en</strong>ce of the physical mechanisms responsible forthe MIS oscillations and conv<strong>en</strong>tional MIRO, strongly correlatedwith microwave frequ<strong>en</strong>cy. It has also be<strong>en</strong> foundthat the inelastic mechanism explains photoresistance measurem<strong>en</strong>tsin a two-subband system at low temperatures[Wiedmann et al., Phys. Rev. B 78, 121301(R) (2008)].In this contribution we report on experim<strong>en</strong>tal and theoreticalstudies of interfer<strong>en</strong>ce betwe<strong>en</strong> MIS oscillations andFMIROs. In a certain temperature range (8 K

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