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Not AvailableAmphidynamic crystals are a type of condensed matter that blends two extremes of the dynamic spectrum: rigid components forming a static lattice and rapidly moving parts. Among them, ordered rotor arrays within metal-organic frameworks (MOFs) constitute a promising platform to explore unchartered territories, such as gas phase-like dynamics in the crystalline state. Through quantum mechanical (QM) calculations and molecular dynamics (MD) simulations we verified that nearly barrierless cubane rotators in CUB-5 display rotational dynamics that transitions from continuous or inertial at high tempera-ture, to chaotic behavior, and ultimately to discrete jumps, as the temperature decreases from room temperature down to cry-ogenic conditions. 1H NMR spin-lattice (T1) relaxation measurements corroborate our theoretical predictions, with experi-mental rotational activation energy of 0.17 kcal/mol and an attempt frequency of 1.03×1012 s-1 that compare well with calcu-lated values of 0.15 kcal/mol and 0.38×1012 s-1, respectively. 

Unambiguous identification of the superconducting order parameter symmetry in ${\text{Sr}}_2{\text{RuO}}_4$has remained elusive for more than a quarter century. While a chiral p-wave ground state analogue to superfluid³He-A was ruled out only very recently, other proposed triplet-pairing scenarios are still viable. Establishing the condensate magnetic susceptibility reveals a sharp distinction between even-parity (singlet) and odd-parity (triplet) pairing since the superconducting condensate is magnetically polarizable only in the latter case. Here field-dependent¹⁷O Knight shift measurements, being sensitive to the spin polarization, are compared to previously reported specific heat measurements for the purpose of distinguishing the condensate contribution from that due to quasiparticles. We conclude that the shift results can be accounted for entirely by the expected field-induced quasiparticle response. An upper bound for the condensate magnetic response of <10% of the normal state susceptibility is sufficient to exclude all purely odd-parity candidates.