Scaling of silicon nanoparticle growth in low temperature flowing plasmas

被引:8
作者
Lanham, Steven J. [1 ]
Polito, Jordyn [1 ]
Shi, Xuetao [2 ]
Elvati, Paolo [2 ]
Violi, Angela [1 ,2 ]
Kushner, Mark J. [1 ,3 ]
机构
[1] Univ Michigan, Dept Chem Engn, 1301 Beal Ave, Ann Arbor, MI 48109 USA
[2] Univ Michigan, Dept Mech Engn, 1301 Beal Ave, Ann Arbor, MI 48109 USA
[3] Univ Michigan, Dept Elect Engn & Comp Sci, 1301 Beal Ave, Ann Arbor, MI 48109 USA
基金
美国国家科学基金会;
关键词
PARTICLE-TRANSPORT; NANOCRYSTALS; PARTICULATE; SIMULATION; DEPOSITION; CHARGE;
D O I
10.1063/5.0062255
中图分类号
O59 [应用物理学];
学科分类号
摘要
Low temperature plasmas are an emerging method to synthesize high quality nanoparticles (NPs). An established and successful technique to produce NPs is using a capacitively coupled plasma (CCP) in cylindrical geometry. Although a robust synthesis technique, optimizing or specifying NP properties using CCPs, is challenging. In this paper, results from a computational investigation for the growth of silicon NPs in flowing inductively coupled plasmas (ICPs) using Ar/SiH4 gas mixtures of up to a few Torr are discussed. ICPs produce more locally constrained and quiescent plasma potentials. These positive plasma potentials produce an electrostatic trap for negatively charged NPs, which can significantly extend the residence time of NPs in the plasma, which in turn provides a controllable period for particle growth. The computational platforms used in this study consist of a two-dimensional plasma hydrodynamics model, a three-dimensional nanoparticle growth and trajectory tracking model, and a molecular dynamics simulation for deriving reactive sticking coefficients of silane radicals on Si NPs. Trends for the nanoparticle growth as a function of SiH4 inlet fraction, gas residence time, energy deposition per particle, pressure, and reactor diameter are discussed. The general path for particle synthesis is the trapping of small NPs in the positive electrostatic potential, followed by entrainment in the gas flow upon reaching a critical particle size. Optimizing or controlling NP synthesis then depends on the spatial distribution of plasma potential, the density of growth species, and the relative time that particles spend in the electrostatic trap and flowing through higher densities of growth species upon leaving the trap.
引用
收藏
页数:18
相关论文
共 54 条
  • [1] 49American Cancer Society, 2006, ENCY INORGANIC CHEM
  • [2] Numerical Modeling of an RF Argon-Silane Plasma with Dust Particle Nucleation and Growth
    Agarwal, Pulkit
    Girshick, Steven L.
    [J]. PLASMA CHEMISTRY AND PLASMA PROCESSING, 2014, 34 (03) : 489 - 503
  • [3] Sectional modeling of nanoparticle size and charge distributions in dusty plasmas
    Agarwal, Pulkit
    Girshick, Steven L.
    [J]. PLASMA SOURCES SCIENCE & TECHNOLOGY, 2012, 21 (05)
  • [4] On the orbital motion limited theory for a small body at floating potential in a Maxwellian plasma
    Allen, JE
    Annaratone, BM
    de Angelis, U
    [J]. JOURNAL OF PLASMA PHYSICS, 2000, 63 : 299 - 309
  • [5] PROBE THEORY - THE ORBITAL MOTION APPROACH
    ALLEN, JE
    [J]. PHYSICA SCRIPTA, 1992, 45 (05): : 497 - 503
  • [6] Atkinson C., 1979, APPL STAT C, V28, P29
  • [7] Plasma synthesis of single-crystal silicon nanoparticles for novel electronic device applications
    Bapat, A
    Anderson, C
    Perrey, CR
    Carter, CB
    Campbell, SA
    Kortshagen, U
    [J]. PLASMA PHYSICS AND CONTROLLED FUSION, 2004, 46 : B97 - B109
  • [8] A Non-Thermal Plasma Route to Plasmonic TiN Nanoparticles
    Barragan, Alejandro Alvarez
    Ilawe, Niranjan V.
    Zhong, Lanlan
    Wong, Bryan M.
    Mangolini, Lorenzo
    [J]. JOURNAL OF PHYSICAL CHEMISTRY C, 2017, 121 (04) : 2316 - 2322
  • [9] THERMOPHORETIC DEPOSITION OF PARTICLES IN GAS FLOWING OVER COLD SURFACES
    BATCHELOR, GK
    SHEN, C
    [J]. JOURNAL OF COLLOID AND INTERFACE SCIENCE, 1985, 107 (01) : 21 - 37
  • [10] Particle nucleation and growth in a low-pressure argon-silane discharge
    Boufendi, L.
    Bouchoule, A.
    [J]. PLASMA SOURCES SCIENCE & TECHNOLOGY, 1994, 3 (03) : 262 - 267