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纳米颗粒超晶格中的偶极-偶极相互作用。

Dipole-dipole interactions in nanoparticle superlattices.

作者信息

Talapin Dmitri V, Shevchenko Elena V, Murray Christopher B, Titov Alexey V, Kral Petr

机构信息

The Molecular Foundry, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA.

出版信息

Nano Lett. 2007 May;7(5):1213-9. doi: 10.1021/nl070058c. Epub 2007 Mar 31.

Abstract

Nanoparticles often self-assemble into hexagonal-close-packed (hcp) structures although it is predicted to be less stable than face-centered-cubic (fcc) packing in hard-sphere models. In addition to close-packed fcc and hcp superlattices, we observe formation of nonclose-packed simple-hexagonal (sh) superlattices of nearly spherical PbS, PbSe, and gamma-Fe2O3 nanocrystals. This surprisingly rich phase diagram of monodisperse semiconducting nanoparticles is explained by considering the interactions between nonlocal dipoles of individual nanoparticles. By calculating the total electrostatic and dispersive energies, we explain stability of the hcp and sh nanoparticle superlattices, introduce the superlattice phase diagram, and predict antiferroelectric ordering in dipolar nanoparticle superlattices.

摘要

纳米粒子通常会自组装成六方密堆积(hcp)结构,尽管在硬球模型中预计其稳定性低于面心立方(fcc)堆积。除了密堆积的fcc和hcp超晶格外,我们还观察到近球形的PbS、PbSe和γ-Fe2O3纳米晶体形成了非密堆积的简单六方(sh)超晶格。通过考虑单个纳米粒子的非局部偶极子之间的相互作用,可以解释这种单分散半导体纳米粒子令人惊讶的丰富相图。通过计算总静电能和色散能,我们解释了hcp和sh纳米粒子超晶格的稳定性,引入了超晶格相图,并预测了偶极纳米粒子超晶格中的反铁电有序性。

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