2007
A New Route to Large‐Scale Synthesis of Silicon Nanowires in Ultrahigh Vacuum
Abstract: An approach for the large‐scale synthesis of high‐purity silicon nanowires (SiNWs) in ultrahigh vacuum is presented. A mixture of Si and SiO2 is evaporated by an electron beam, and the growth temperature is 700 °C, which is much lower than those used for other oxide‐assisted growths. A new type of single‐crystal SiNWs, with [221] orientation, is thus synthesized. Moreover, it is experimentally demonstrated that SiO intermediates are formed in the process, and the nanowires are obtained via a disproportionation…
Search citation statements
Paper Sections
Select...
12
4
3
0
Citation Types
0
22
0
0
Year Published
2008
2024
Publication Types
Select...
14
2
Relationship
0
16
Authors
Journals
Cited by 16 publications
(22 citation statements)
References 28 publications
0
22
0
0
“…Finally, XPS Si 2p core lines with a shape of negative asymmetry, whose main signals are located at ∼101.1 eV and assigned to Si−N bonds, − appear and do not vary with the sputtering time once more. These reveal that highly oxidized compound (SiO 2 ) presents at the top surface, followed by a transition layer, and finally silicon nitride (SiN x ) distributed very uniformly at the bottom layer. The same conclusion could be drawn from the XPS N 1s spectra.…”
Section: Resultsmentioning
confidence: 99%
“…Finally, XPS Si 2p core lines with a shape of negative asymmetry, whose main signals are located at ∼101.1 eV and assigned to Si−N bonds, − appear and do not vary with the sputtering time once more. These reveal that highly oxidized compound (SiO 2 ) presents at the top surface, followed by a transition layer, and finally silicon nitride (SiN x ) distributed very uniformly at the bottom layer. The same conclusion could be drawn from the XPS N 1s spectra.…”
Section: Resultsmentioning
confidence: 99%
“…Figure a displays the XPS Si 2p spectra collected from the 110-nm SiN x /Si(100) as a function of Ar + sputtering time. It is seen that Si 2p signal first appears at the binding energy of ∼103.0 eV, corresponding to O−Si−O bonds, , and then rapidly shifts to lower binding energies after Ar + sputtering. Moreover, the shape of Si 2p peak is observed to first broaden asymmetrically toward high binding energies (positive asymmetry) and then toward low binding energies (negative asymmetry).…”
Section: Resultsmentioning
confidence: 99%
“…Furthermore, the SiO 2 layer formed around the Si NWs acts as a barrier, preventing further diameter expansion. [21][22][23] When the carbon atmosphere is introduced at a certain temperature, the pyrolysis of incoming CH 4 to produce C occurs, which then encapsulates the Si NWs by forming a carbon shell on the outside. The synthesis process for the Si NWs@C core/shell nanocomposites is characterized by its inherent simplicity, as it involves a single-step deposition method under temperature control.…”
Section: Resultsmentioning
confidence: 99%
“…This phenomenon (Figure 4 ) is completely different from that in VLS process (Figure 1 ). According to our previous study [ 16 ], SiNWs (Figure 4b ) are grown by OAG via a disproportionation reaction of 2SiO → Si + SiO 2 . The SiO intermediates are created by electron beam bombardment on the mixed Si and SiO 2 and play an important role in the SiNWs formation [ 16 ].…”
Section: Resultsmentioning
confidence: 99%
“…According to our previous study [ 16 ], SiNWs (Figure 4b ) are grown by OAG via a disproportionation reaction of 2SiO → Si + SiO 2 . The SiO intermediates are created by electron beam bombardment on the mixed Si and SiO 2 and play an important role in the SiNWs formation [ 16 ]. Firstly, SiO can be bonded to the SiO 2 surface through the overlap between the empty Si π 2p * orbits and the lone pair filled O 2p orbits (formation of an intermolecular Si ← O donor-acceptor bond) [ 26 ], which contributes the generation of stable nuclei for the growth of SiNWs.…”
Section: Resultsmentioning
confidence: 99%
