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硫化铅和硒化铅纳米颗粒电场定向自组装的原位透射电子显微镜观察

In Situ TEM Observation of Electric Field-Directed Self-Assembly of PbS and PbSe Nanoparticles.

作者信息

Zelenina Iryna, Böttner Harald, Schmidt Marcus, Grin Yuri, Simon Paul

机构信息

Max-Planck-Institut für Chemische Physik Fester Stoffe, Nöthnitzer Str. 40, 01187 Dresden, Germany.

Fraunhofer Institut für Physikalische Messtechnik, Georges-Köhler-Allee 30, 79110 Freiburg, Germany.

出版信息

Nanomaterials (Basel). 2025 Aug 18;15(16):1275. doi: 10.3390/nano15161275.

DOI:10.3390/nano15161275
PMID:40863855
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC12388880/
Abstract

Nano-sized particles of semiconducting lead sulfide and selenide and their 2D thin layers show high potential in applications, such as field-effect transistors, photodetectors, solar cells, and thermoelectric devices. The generation of PbS and PbSe nanobars and nanocubes is evoked by in situ electron beam treatment, leading to the formation of thin, extended 2D nanolayers. The initial single crystals are decomposed via sublimation of PbS and PbSe in terms of molecular and atomic fragments, which finally condense on the cold substrate to form nanostructures. The fragments in the gas phase were proven using mass spectrometry. In the case of PbS, Pb and PbS species could were detected, whereas PbSe disintegrated into Pb, Se, and PbSe. The threshold current that initiates fragmentation increases from PbTe via PbSe up to PbS, which is in line with the increasing crystal formation energies. The uniform orientation of independently formed nanoparticles on the macroscopic scale can be explained by an external electric field acting on emerging dipolar nanospecies. The external dipole field originates from the sputtered mother crystal, where the electron flux is initiated; thus, a current arises between the crystal's hot and cold ends. On the contrary, in small single crystals, due to the lack of sufficient charge carriers, only local material excavation is detected instead of extended depletion and subsequent nanoparticle deposition. This fragmentation process may represent a new preparation route that provides lead chalcogenide nanofilms that are free of contamination or surfactant participation, which are typical drawbacks associated with the application of wet chemical methods.

摘要

半导体硫化铅和硒化铅的纳米级颗粒及其二维薄层在诸如场效应晶体管、光电探测器、太阳能电池和热电器件等应用中显示出很高的潜力。通过原位电子束处理引发了硫化铅和硒化铅纳米棒和纳米立方体的生成,导致形成薄的、延伸的二维纳米层。初始的单晶通过硫化铅和硒化铅以分子和原子碎片的形式升华而分解,这些碎片最终在冷基板上凝聚形成纳米结构。气相中的碎片通过质谱法得到了证实。对于硫化铅,可以检测到铅和硫化铅物种,而硒化铅分解为铅、硒和硒化铅。引发碎片化的阈值电流从碲化铅经硒化铅到硫化铅逐渐增加,这与晶体形成能的增加是一致的。宏观尺度上独立形成的纳米颗粒的均匀取向可以通过作用于新兴偶极纳米物种的外部电场来解释。外部偶极场源自溅射的母晶体,在那里电子通量被引发;因此,在晶体的热端和冷端之间会产生电流。相反,在小单晶中,由于缺乏足够的电荷载流子,只能检测到局部材料挖掘,而不是扩展的耗尽和随后的纳米颗粒沉积。这种碎片化过程可能代表了一种新的制备途径,它提供了无污染或无表面活性剂参与的硫族化铅纳米薄膜,而这些是与湿化学方法应用相关的典型缺点。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7a69/12388880/14058fdf0380/nanomaterials-15-01275-g014.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7a69/12388880/e285e9f717bb/nanomaterials-15-01275-g001.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7a69/12388880/8dcff8b7d622/nanomaterials-15-01275-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7a69/12388880/7a93ae185067/nanomaterials-15-01275-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7a69/12388880/a982220db703/nanomaterials-15-01275-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7a69/12388880/81ca26ea9601/nanomaterials-15-01275-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7a69/12388880/fed7b515ddc0/nanomaterials-15-01275-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7a69/12388880/b9f1a5ba6072/nanomaterials-15-01275-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7a69/12388880/211515d02982/nanomaterials-15-01275-g011a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7a69/12388880/3f959d676bf3/nanomaterials-15-01275-g012.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7a69/12388880/db2459bd67b2/nanomaterials-15-01275-g013.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7a69/12388880/14058fdf0380/nanomaterials-15-01275-g014.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7a69/12388880/e285e9f717bb/nanomaterials-15-01275-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7a69/12388880/5d9f7176115a/nanomaterials-15-01275-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7a69/12388880/08607c756b11/nanomaterials-15-01275-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7a69/12388880/8adf3ea30fab/nanomaterials-15-01275-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7a69/12388880/8dcff8b7d622/nanomaterials-15-01275-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7a69/12388880/7a93ae185067/nanomaterials-15-01275-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7a69/12388880/a982220db703/nanomaterials-15-01275-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7a69/12388880/81ca26ea9601/nanomaterials-15-01275-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7a69/12388880/fed7b515ddc0/nanomaterials-15-01275-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7a69/12388880/b9f1a5ba6072/nanomaterials-15-01275-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7a69/12388880/211515d02982/nanomaterials-15-01275-g011a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7a69/12388880/3f959d676bf3/nanomaterials-15-01275-g012.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7a69/12388880/db2459bd67b2/nanomaterials-15-01275-g013.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7a69/12388880/14058fdf0380/nanomaterials-15-01275-g014.jpg

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