Influence of Isotope Substitution on Lattice and Spin‐Peierls‐Type Transition Features in One‐Dimensional Nickel Bis‐dithiolene Spin Systems

Four new 1D spin‐Peierls‐type compounds, [D 5 ]1‐(4′‐ R ‐benzyl)pyridinium bis(maleonitriledithiolato)nickelate ([D 5 ]R‐Py; R=F, I, CH 3 , and NO 2 ), were synthesized and characterized structurally and magnetically. These 1D compounds are isostructural with the corresponding non‐deuterated compounds, 1‐(4′‐ R ‐benzyl)pyridinium bis(maleonitriledithiolato)nickelate (R‐Py; R=F, I, CH 3 , and NO 2 ). Compounds [D 5 ]R‐Py and R‐Py (R=F, I, CH 3 , and NO 2 ) crystallize in the monoclinic space group P 2 1 / c with uniform stacks of anions and cations in the high‐temperature phase and triclinic space group P $\bar 1$ with dimerized stacks of anions and cations in the low‐temperature phase. Similar to the non‐deuterated R‐Py compounds, a spin‐Peierls‐type transition occurs at a critical temperature for each [D 5 ]R‐Py compound; the magnetic character of the 1D S =1/2 ferromagnetic chain for [D 5 ]F‐Py and the 1D S =1/2 Heisenberg antiferromagnetic chain for others appear above the transition temperature. Spin‐gap magnetic behavior was observed for all of these compounds below the transition temperature. In comparison to the corresponding R‐Py compound, the cell volume is almost unchanged for [D 5 ]F‐Py and shows slight expansion for [D 5 ]R‐Py (R=I, CH 3 , and NO 2 ) as well as an increase in the spin‐Peierls‐type transition temperature for all of these 1D compounds in the order of F>I≈CH 3 ≈NO 2 . The large isotopic effect of nonmagnetic countercations on the spin‐Peierls‐type transition critical temperature, T C , can be attributed to the change in ω 0 with isotope substitution.