In an electron-donor (D)electron-acceptor (A) three-dimensional assembly series with a D 2 A formulation, their magnetic properties were tuned by doping another D unit with a stronger electron-donating ability capable of reducing A ¹ to A 2¹ . The magnetic-phase-transition temperature (T c ) of doped compounds nonlinearly decreases with increasing doping rate.The control of magnetic behavior in a flexible framework of materials is an important topic of materials science, which has been carried out not only by physical stimuli such as temperature, 1 pressure, 2 electric field, 3 and photoirradiation 3b,4 but also by chemical techniques. 5,6 One of the chemical techniques is based on hostguest chemistry that has recently attracted much attention in the field of molecular porous materials, 7 in which the adsorptiondesorption of guest molecules such as crystallization solvents and common gas molecules reversibly tunes the magnetism of materials without the collapse of frameworks; 5,6 they are often called "magnetic sponge;" 8 another technique involves the use of chemical doping of, for example, alternate metal ions, elements, and organic functional groups.9,10 The former is a serendipitous technique, while the latter is a strategic one. However, the chemical doping in molecular materials is not easy to perform in a framework of materials because molecular materials relatively flexibly vary their frameworks in reflections of steric hindrance and the variation of bonding geometry around dopants. Hence, not many cases are known in which the effect of chemical doping has been systematically investigated for tuning magnetism in molecular materials.Here, we report doped magnetic materials whose magnetism is closely associated with the electron transfer around dopants in a framework. ) are paramagnetic species with S = 1 and S = 3/2, respectively, and the one-electron-reduced BTDA-TCNQ (i.e., BTDA-TCNQ•¹ as A ¹ ) is a radical with S = 1/2, providing a ferrimagnet with a magnetic-phase-transition temperature, T c = 107 K.12 Meanwhile, a similar D 2 A-type three-dimensional compound using m- 4 } 2x (BTDA-TCNQ)] (x = 0.1, 10%; 0.125, 12.5%; 0.15, 15%). They are still magnets, but interestingly, T c nonlinearly decreases on increasing the doping rate x and is rather abruptly reduces at lower temperatures in compounds with over 10% doping. This behavior can well be described using the percolation theory for their magnetic superexchange pathways.It is not easy to accurately characterize the doping rate of the doped compounds because of the difference between F and Me groups in [Ru 2 ] units; therefore, the doping rate given as 10%, 12.5%, and 15% implies the mixing ratio in the synthetic procedure. Nevertheless, the doping nature can be seen in the IR spectra. The doped compounds 10%, 12.5%, and 15% have characteristic two vibrational modes of¯(C¸N) for the BTDA-TCNQ moiety at 2198 and 2136 cm (Figure 2a). Meanwhile, thē (C¸N) peak at ca. 2196 cm ¹1 broadens with increasing doping rate, and a broad weak peak newly appear...