Carrier tunneling through CdMnTe barriers of different thicknesses is investigated in CdTe/CdMnTe asymmetric double quantum wells. Steady-state photoluminescence at 1.8 K and time-resolved photoluminescence experiments between 10 K and 50 K were performed.PACS numbers: 78.66. Hf; 78.20.Ls, 78.47.+pa Semimagnetic semiconductors are of great interest because of their novel properties [1]. In particular, the strong interaction between the spins of carriers and the magnetic ions leads to giant magnetooptical effects such as extremely large Zeeman splittings.In contrast to previous studies of Mn-based asymmetric double quantum wells (ADQWs) where the quantum wells (QW) were made of CdTe [2,3], in our system the wide well (WW) contains Mn, so as to increase drastically the influence of a magnetic field on the confined levels [4].In this report we will present steady-state and time-resolved experiments at zero tesla, focusing on the influence of the tunnel barrier thickness on the tunneling.The samples were grown by molecular beam epitaxy in the (100) direction. The stuctures were deposited on a CdMnTe buffer layer of the same Mn concentration as the barriers. Table compiles for the samples the Mn concentrations (of the barriers (xΒ), of the WW (xW)), and the thicknesses measured by Reflection High Energy Electron Diffraction (RHEED) oscillations (WW (LW), narrow well (LN), tunnel barrier (LB)).The photoluminescence (PL) spectra are depicted in Fig. 1. The emission of the fundamental excitons of both QWs is observed: e1Nhh1N at lower energy and e1Whh1W at higher energy. The labels hh 1 N (hh1W) mean the first heavy hole level in the narrow CdTe (wide,CdMnTe) QW. Note that because the gap increases with the Mn content, the WW luminescence appears at higher energy. The relative intensity of their luminescence (R = IW/IN) reflects the strength of the coupling. The observed increase in R when LB increases indicates a less efficient tunneling (637)