Spin decoherence processes in the S = 1/2 scalene triangular cluster (Cu3(OH))

We report the synthesis and magnetic properties of the molecular cluster Cu _3 ( ${{\mu }_{3}}$ −OH)( μ -OH)( μ -O _2 Ar $^{4F-{\rm Ph}}$ ) _2 (py) _3 (OTf) _2 , abbreviated as (Cu _3 (OH)). Using magnetization, electron paramagnetic resonance and spin dimer analysis, we derive a microscopic magneti...

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Bibliographic Details
Main Authors: A N Ponomaryov, N Kim, Z H Jang, J van Tol, H-J Koo, J M Law, B J Suh, S Yoon, K Y Choi
Format: Article
Language:English
Published: IOP Publishing 2015-01-01
Series:New Journal of Physics
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Online Access:https://doi.org/10.1088/1367-2630/17/3/033042
Description
Summary:We report the synthesis and magnetic properties of the molecular cluster Cu _3 ( ${{\mu }_{3}}$ −OH)( μ -OH)( μ -O _2 Ar $^{4F-{\rm Ph}}$ ) _2 (py) _3 (OTf) _2 , abbreviated as (Cu _3 (OH)). Using magnetization, electron paramagnetic resonance and spin dimer analysis, we derive a microscopic magnetic model of (Cu _3 (OH)) and measure the electron T _1 and T _2 relaxation times. The Cu ^2+ ions are arranged to form a distorted triangular structure with the three different exchange coupling constants ${{J}_{1}}=-43.5$ K, ${{J}_{2}}=-53.0$ K, and ${{J}_{3}}=-37.7$ K. At T = 1.5 K T _1 is of the order of 10 ^−4 s and T _2 is evaluated to be $0.26\;\mu {\rm s}$ . We find that the temperature dependence of $1/{{T}_{1}}$ and $1/{{T}_{2}}$ is governed by Orbach process and spin bath fluctuations, respectively. We discuss the role of spin–phonon mechanism in determining a spin decoherence time in a class of spin triangular clusters.
ISSN:1367-2630