Abstract

The local mean field approximation is applied to an inhomogeneous 3D spin crossover (SCO) nanoparticle configuration with a special focus on its systemic effect on molecules in the bulk, at the corner, at the edge and at surface. The matrix effect at the surface is introduced through a specific interaction term, L. The partition function for each region allows the determination of the total free-energy F from which the stability of each configuration is analyzed through thermodynamic considerations.

Highlights

  • Fe(II) Spin-crossover (SCO) shows a particular first-order phase transition, with thermal hysteresis [1,2,3,4,5] that is mediated between two spin states, Low-Spin (LS) with degeneracy gLS, stable at low temperatures and High-Spin (HS) with degeneracy gHS (> gLS ), stable at high temperatures

  • Namely termed as Tdown and Tup, a spin crossover (SCO) molecule can be in one of these two states depending on its thermal history

  • Simulations are performed whose parameter values are chosen from experimental data of typical SCO solids characterized by: Δ/kB=3126 K, ln(g)= 8.45

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Summary

Introduction

Fe(II) Spin-crossover (SCO) shows a particular first-order phase transition, with thermal hysteresis [1,2,3,4,5] that is mediated between two spin states, Low-Spin (LS) with degeneracy gLS , stable at low temperatures and High-Spin (HS) with degeneracy gHS (> gLS ), stable at high temperatures. Namely termed as Tdown and Tup , a SCO molecule can be in one of these two states depending on its thermal history.

Results
Conclusion
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