2019
DOI: 10.1134/s1063782619070236
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Size Dependence of the Melting Point of Silicon Nanoparticles: Molecular Dynamics and Thermodynamic Simulation

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Cited by 21 publications
(15 citation statements)
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“…This is more appropriately treated in the so-called surface-phonon instability model, 54 accounting for the lowering energy of the phonon modes with increasing concentration of defects, offering a better fit to the experimentally observed data. 55 , 56 These observations indicate that melting of the disordered surfaces occurs at lower temperatures compared to the melting of the crystalline core, in agreement with the aforementioned study by Talyzin et al 51 This could rationalize the formation of a crystalline core–amorphous shell Si-NP system.…”
Section: Resultssupporting
confidence: 89%
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“…This is more appropriately treated in the so-called surface-phonon instability model, 54 accounting for the lowering energy of the phonon modes with increasing concentration of defects, offering a better fit to the experimentally observed data. 55 , 56 These observations indicate that melting of the disordered surfaces occurs at lower temperatures compared to the melting of the crystalline core, in agreement with the aforementioned study by Talyzin et al 51 This could rationalize the formation of a crystalline core–amorphous shell Si-NP system.…”
Section: Resultssupporting
confidence: 89%
“…Another recent experimental study by Alessi et al 50 on plasma-synthesized Si-NPs suggested that the crystallinity of the Si-NP of the same size can be manipulated by changing the concentration of silane, which changes optical and electronic properties of the material. More importantly, a recent theoretical study by Talyzin et al 51 suggests that molten Si nanodroplets do not return to the crystalline form but remain fully amorphous and that Si-NP surface has a melting temperature different from that of its core. The phase-equilibrium model of crystallization indicates that the melting temperature of NPs decreases relative to the bulk melting temperature (∼1414 °C for Si) linearly with their reciprocal radius T m ( R –1 ), 52 , 53 though this model does not work very well for covalent materials like Si, where formation of defects (and hence also surfaces) has dynamics different from that in the simpler ionic/metallic nanosystems.…”
Section: Resultsmentioning
confidence: 99%
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“…However, nanosized primary Si particles in a micrometer-sized Si particle are easily activated at high temperature because of lattice vibration at the surface and are fused together to form lager particles. [29,30] As a result, nanopores within micrometer-sized porous Si particles (Figure 1) will shrink, and the micrometer-sized particles will lose their porous structure as shown in Figure 1a, thus defeating the purpose of forming Si nanostructures in the material design. Therefore, we developed a pitch impregnation method to protect the nanostructure from damage during fabrication of micrometer-sized Si particles with desired nanostructure.…”
Section: Resultsmentioning
confidence: 99%
“…Er 3+ /Yb 3+ CaF 2 (PL ratio) [145] 0.015 293-318 Tm 3+ /Yb 3+ CaF 2 (PL ratio) [145] 0.002 293-318 NaYF 4 :Er 3+ , Yb 3+ (PL ratio) [146] 0.0114 298-334 NaLuF 4 :Yb, Er [147] 0.009 273-348 ZnO:Er 3+ (PL ratio) [148] 0.0098 278-463 β-NaYF 4 :20%Yb 2 %Er (PL ratio) [149] 0.0157 294-334 (Gd,Yb,Er) 2 O 3 (PL ratio) [32] 0.017 300-1050 Nanodiamonds (NDs) NV (PL intensity) [150] 0.01 295-400 GeV (ZPL linewidth) [151] 0.0064 150-400 SiV (ZPL shift) [152] 1.61 ×10 −5 285-305 SnV (ZPL shift) [153] 8.66 ×10 −5 295-315 GeV (anti-Stokes) [154] 0.014 150-400 Optically resonant nanoparticles (RNPs) Au nanorod (anti-Stokes PL) [34] 10 −3 300-1300 [155] Si (Stokes Raman shift) [55] 2×10 −4 0-1685 [156,157,158] α-Fe 2 O 3 (Stokes Raman shift) [159] 4×10 −4 0-1840 [160] Table 1: Nanothermometers. List of materials and nanothermometry techniques based on light-emitting materials, nanostructures, and nanomaterials.…”
Section: Basic Properties Of Materials Employed For Thermonanophotonicsmentioning
confidence: 99%