Abstract

Thermal properties of Zn2(C8H4O4)2•C6H12N2 metal-organic framework compound at 8–300 K suggest the possibility of subbarrier tunnelling transitions between left-twisted (S) and right-twisted (R) forms of C6H12N2 dabco molecules with D3 point symmetry. The data agree with those obtained for the temperature behavior of nuclear spin-lattice relaxation times. It is shown that there is a temperature range where the transitions are stopped. Therefore, Zn2(C8H4O4)2•C6H12N2 and related compounds are interesting objects to study the effect of spontaneous mirror-symmetry breaking and stabilization of chiral isomeric molecules in solids at low temperatures.

Highlights

  • Chirality-related interactions are demonstrated by chiral molecules, i.e. those that can exist in both left- and right-handed forms

  • energy barrier (Ea) values are assumed to correspond to activation energies only of hydrogen and carbon atoms of the dabco molecule, and nitrogen atoms are not involved in the reorientation

  • The temperature dependence of 1Н NMR T1 in Zn2(C8H4O4)2C6H12N2 at 310–165 K obeys the classical theory of nuclear spin-lattice relaxation and is characterized by a single-exponential recovery of the free induction decay (FID)[18, 19]

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Summary

Introduction

Chirality-related interactions are demonstrated by chiral molecules, i.e. those that can exist in both left- and right-handed forms. The expected fundamental conclusions are still not supported by detailed analysis of the interactions within crystal structures where the stabilization effect is not suppressed by other impacts[8, 9] In this respect, of high interest are metal-organic framework compounds with large pores, open internal channels, and large internal surface areas[10,11,12]. The untwisted D3h state of the dabco molecule corresponds to its transition state and its energy is equal to the value of the energy barrier Ea (Fig. 1)[13] This state can be stable in crystals, and the untwisted molecule can move using both the activation and the tunnelling mechanisms

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