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Bulletin of the American Physical Society

Atomic-clock transition behavior in a Cr 7 Mn molecular nanomagnet

Gajadhar Joshi, Ilija K. Nikolov, Guanchu Chen, Daniel Florin Sava, Grigore A. Timco, Richard E. P. Winpenny, Jonathan R. Friedman

Published Mar 3, 2020• 0 citations
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Molecular nanomagnets are zero-dimensional spin systems that exhibit quantum-mechanical behavior at low temperatures. Exploiting quantum-information theoretic measures, we quantify here the size of linear superpositions that can be generated within the ground multiplet of high- and low-spin nanomagnets. Amongst the former class of systems, we mainly focus on Mn${}_{12}$ and Fe${}_{8}$. General criteria for maximizing such measures are also outlined, and illustrated with reference to spin clusters of different geometries. The actual character (micro or macroscopic) of linear superpositions in low-spin systems is inherently ill-defined. Here, this issue is addressed with specific reference to the Cr${}_{7}$Ni and V${}_{15}$ molecules, characterized by an $S=1/2$ ground state. In both cases, the measures we obtain are larger than those of a single $s=1/2$ spin but not proportionate to the number and value of the constituent spins.

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Molecular nanomagnets are zero-dimensional spin systems that exhibit quantum-mechanical behavior at low temperatures. Exploiting quantum-information theoretic measures, we quantify here the size of linear superpositions that can be generated within the ground multiplet of high- and low-spin nanomagnets. Amongst the former class of systems, we mainly focus on Mn12{}_{12}12​ and Fe8{}_{8}8​. General criteria for maximizing such measures are also outlined, and illustrated with reference to spin clusters of different geometries. The actual character (micro or macroscopic) of linear superpositions in low-spin systems is inherently ill-defined. Here, this issue is addressed with specific reference to the Cr7{}_{7}7​Ni and V15{}_{15}15​ molecules, characterized by an S=1/2S=1/2S=1/2 ground state. In both cases, the measures we obtain are larger than those of a single s=1/2s=1/2s=1/2 spin but not proportionate to the number and value of the constituent spins.