1H-NMR spin-lattice relaxation rate of the quantum spin system (CH3)2CHNH3Cu(Cl[x]Br1-x)3 with x = 0 and 0.35

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  • <SUP>1</SUP>H-NMR Spin–Lattice Relaxation Rate of the Quantum Spin System (CH<SUB>3</SUB>)<SUB>2</SUB>CHNH<SUB>3</SUB>Cu(Cl<I><SUB>x</SUB></I>Br<SUB>1−<I>x</I></SUB>)<SUB>3</SUB> with <I>x</I>=0 and 0.35
  • <sup>1</sup>H-NMR Spin–Lattice Relaxation Rate of the Quantum Spin System (CH<sub>3</sub>)<sub>2</sub>CHNH<sub>3</sub>Cu(Cl<sub><i>x</i></sub>Br<sub>1-<i>x</i></sub>)<sub>3</sub> with <i>x</i>=0 and 0.35

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The spin–lattice relaxation rate T1−1 of 1H-NMR has been measured in (CH3)2CHNH3Cu(ClxBr1−x)3 with x=0 and 0.35, in order to investigate their microscopic magnetism. Previous macroscopic magnetization and specific heat measurements suggested that these two exist in a singlet-dimer phase. The temperature dependence of T1−1 in an x=0 system decreased exponentially toward zero, providing microscopic evidence of a gapped singlet ground state, which is consistent with results of macroscopic experiments. At the same time, in the x=0.35 system, T1−1 showed a sharp peak structure at approximately 7.5 K but no splitting of 1H-NMR spectra, indicative of magnetic ordering. We discuss the observed sharp peak structure in the x=0.35 system with the soft mode toward the exotic magnetic ground state suggested by recent μSR experiments.

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