Various arylenediimides (ADIs) have been applied to construct photoresponsive coordination polymers (CPs), while the size effect of ADI π-conjugate systems on the photoresponsive behaviors in CPs has been overlooked in the past few years. Herein, we emphasize the size effect of ADI π-conjugate systems on photoinduced electron transfer (ET) in CPs, taking two Eu3+-based CPs, [Eu­(H2BINDI)­(BINDI)0.5(H2O)2]·NH2(CH3)2·8H2O (1) and [Eu2(BIPMDI)­(DMF)4(NO3)2]·H2O·2DMF (2) [H4BINDI = N,N′-bis­(5-isophthalic acid)­naphthalenediimide; H4BIPMDI = N,N′-bis­(5-isophthalic acid)­pyromellitic diimide; DMF = N,N-dimethylformamide], as a case. Both 1 and 2 display ET-based photochromic behaviors with distinct photoresponsive rates and coloration contrast, which can contribute to the size effect of diimide cores on the interfacial contacts of electron donors/acceptors. Meanwhile, ET between the neighboring larger NDI cores of the H4BINDI ligands can block ligand-to-metal charge transfer and quench luminescence of the Eu3+ metal center in 1. Therefore, this work will provide a theoretical basis for the development and exploration of photoresponsive materials.

Comprehensive SummaryBetter understanding the determining factors of dynamic magnetic relaxation in polynuclear lanthanide based single‐molecule magnets (SMMs) remains a challenge due to the complexity of such architectures involving interactions between the magnetic centers. To address this issue, two structurally related heterometal DyIII2ZnII2 SMMs, [Zn2Dy2(L)4(Ac)2(DMF)(CH3OH)]·CH3OH·2H2O (1) and [Zn2Dy2(L)4(Ac)2(DMF)2]·4CH3CN (2) (H2L = (E)‐2‐((2‐hydroxy‐3‐methoxybenzylidene)amino)‐4‐methyphenol, DMF = N,N‐dimethylformamide), are introduced and investigated. Through modifying the auxiliary ligands on one DyIII site while retaining that on the other DyIII, the intramolecular magnetic interactions and relaxation dynamics in these two heterometallic‐DyIII2ZnII2 SMMs can be tuned, demonstrating a dramatic change in the magnet relaxation behavior with energy barrier changing from a negligible value for 1 to 305 K for 2. Ab initio calculations reveal that changing the coordination geometries on the DyIII sites can significantly affect the magnetic interactions as well as single‐ion anisotropy.