The diketonate complex [Cu{OC( t Bu)CC(H)O} 2 ] (1) and its cocrystals with 1,4-diiodotetrafluorobenzene (1,4-FIB), 1,3,5-triiodotrifluorobenzene (1,3,5-FIB), and 1,4-dioxane were studied by X-ray diffraction. In the solid state, 1 exhibits the cis-geometry with syn-t Bu groups; the geometry is stable in storage at 20−25 °C or even in heating in the solid state, solutions, or sublimation. The DFT modeling for isolated molecules of cis-and trans-1 revealed that the cis-form is only slightly more energetically favorable. However, cocrystals trans-1FIB, and trans-1•1,3,5-FIB•C 4 H 8 O 2 display the trans-geometry with the anti-t Bu substituents; the comparison of the geometries revealed the facile crystalpacking-driven cis-to-trans isomerization of 1 upon the cocrystal growth. Compared to the cocrystals of the unsubstituted [Cu(acetylacetonate) 2 ] complex with the FIBs, in the assembled architectures of trans-1•1,4-FIB and trans-1•1,3,5-FIB•C 4 H 8 O 2 , the switch from the bridging (μ 2 -I)•••O,O to two-center I•••O halogen bonding is demonstrated. The theoretical study revealed that the energetic features of the (μ 2 -I)•••O,O halogen bonding in [Cu(acetylacetonate) 2 ]•1,4-FIB are similar to those of the I•••O halogen bonding in 1•1,4-FIB. Variable-temperature XRD data (at 100, 150, 200, 250, and 300 K) for cis-1 and trans-1•1,4-FIB indicate that the infinite chains of molecules stabilized by I•••O halogen bonding remain the main packing motif at all applied temperatures.