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Controlled growth of oriented amorphous silicon nanowires via a solid–liquid–solid (SLS) mechanism

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Controlled growth of oriented amorphous silicon nanowires

via a solid–liquid–solid (SLS) mechanism D.P Yua; ∗, Y.J Xinga;b, Q.L Hanga, H.F Yana, J Xua, Z.H Xib, S.Q Fenga

a Department of Physics, Electron Microscopy Laboratory and Mesoscopic Physics National Laboratory, Peking University,

Beijing 100871, China

b Department of Electronics, Peking University, Beijing, China Received 19 May 2000; received in revised form 19 July 2000; accepted 24 July 2000

Abstract

Highly oriented amorphous silicon nanowires (a-SiNWs ) were grown on Si (1 1 1) The length and diameter of oriented SiNWs are almost uniform, which are 1 m and 25 nm, respectively Di erent from the well-known vapor–liquid–solid (VLS) for conventional whisker growth, it was found that growth of the a-SiNWs was controlled by a solid–liquid–solid mechanism (SLS) This synthesis method is simple and controllable It may be useful in large-scale synthesis of various nanowires

? 2001 Elsevier Science B.V All rights reserved

PACS: 61.46.+w; 68.65.+g; 73.20.Dx; 78.55.−m

Keywords: Si nanowires; Quantum con nement e ect; Low dimensionality

1 Introduction

Intensive research e orts on one-dimensional

nano-materials have been carried out since the rst

pio-neering work of the discovery of carbon nanotubes

by Iijima [1] and other quasi-one-dimensional

nanos-tructures such as silicon nanowires (SiNWs) [2,3]

Because bulk Si is an indirect gap material, the SiNWs

are useful one-dimensional nanostructure for tailoring

its physical properties from indirect to direct band gap

The synthesis of Si whiskers via the vapor–liquid–

solid (VLS) growth mechanism was rst described in

Corresponding author Fax: +86-10-6275-1615.

E-mail address: yudp@pku.edu.cn (D.P Yu).

detail by Wagner and co-workers [4,5] Givargizov developed the growth model and discussed it within

a kinetics framework [6] Yazawa [7] and Westwater [8], and Ozaki [9] produced SiNWs with VLS growth induced by Au metal layer on a Si surface Recently,

Yu et al reported oven-laser ablation method through simple physical evaporation approach [2,10], to pro-duce very pure ultra ne freestanding SiNWs In the previous work for SiNWs synthesis, however, vapor phase with considerable Si concentration was either supplied from laser ablation of a powder target, or directly from silane In this paper, we report that oriented a-SiNWs can be controllably grown on a silicon substrate via a solid–liquid–solid (SLS) growth mechanism

1386-9477/01/$ - see front matter ? 2001 Elsevier Science B.V All rights reserved.

PII: S 1386-9477(00)00202-2

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2 Experimentals

Heavily doped (1:5 × 10 −2

chips wafers were used as substrate The silicon

subs-trate was cleaned ultrasonically in pure petroleum

ether and in ethanol in turns for 5 min, and leached

in distilled water, then dried A thin layer of 40 nm

nickel was thermally deposited on the substrate The

substrate was placed in a quartz tube which was heated

in a tube furnace at 950C Ar (36 sccm) and H2 (4

sccm) were introduced during growth at an ambient

pressure of about 200 Torr After cooling down to

room temperature, a thin layer of gray-colored deposit

was found on the surface of the substrate An

Am-ray FEG-1910 scanning electron microscope (SEM),

and a Hitachi-9000NAR high-resolution

transmis-sion electron microscope (HREM) equipped with

energy-dispersive spectrum (EDS) were employed

for analysis of the morphology and microstructure of

the product

3 Results and discussions

Fig 1(a) shows plan view of SEM image revealing

the general morphology of the SiNWs grown on a

large area (10 mm × 10 mm) of 111 Si substrate The

nanowires grew directly on the substrate It is visible

that the deposit consists of pure SiNWs The growth

rate of the nanowires is estimated to be about 30 nm=s

EDS analysis (inset) proved that the nanowires are

composed of Si, but there exists a small amount of

oxygen in the SiNWs, which was attributed to the

surface oxidation sheathing the nanowires The TEM

image shown in Fig 1(b) reveals that the SiNWs have

diameter between 10 and 50 nm, and length up to a

few tens micrometers The highly di usive ring pattern

(inset) of selected area electron di raction (SAED)

revealed that the SiNWs are completely amorphous

(a-SiNWs)

To control the orientation of the a-SiNWs, a

three-step heating procedure was involved in the

growth of the oriented a-SiNWs Firstly, the system

was heated to 800C, and a mixture of H2(36 sccm)=

Ar (4 sccm) was introduced to the tube The

pure Ar (100 sccm) was used as a carrier gas in

this step The ambient pressure of the tube was

Fig 1 (a) SEM micrograph showing the general morphology of the SiNWs grown via a SLS growth mechanism The inset shows EDS spectrum with the peak corresponding to Si, (b) TEM image revealing that the SiNWs have smooth morphology and average diameter around 40 nm The SAED pattern shown in inset reveals characteristic di usive ring pattern, showing that the nanowires are completely amorphous.

kept near 750 Torr by adjusting the exit valve, then the tube was evacuated This procedure was repeated three times Finally, the temperature was held at 950C at the pressure of about 200 Torr for

1 hr A mixture of H2(4 sccm) and Ar (36 sccm) was introduced to the tube

A low-magni ed SEM image of the oriented a-SiNWs is shown in Fig 2(a), representing a gen-eral planar view of the oriented a-SiNWs It is visible that the nanowires were grown on centimeter-sized substrate An interesting phenomenon is that the nanowire lm was found chapped in a network

of white-contrasted lines The inclined view at a crossover point of the white in Fig 2(b) revealed the white lines are in fact V-shaped chaps From this im-age it is visible that the lm consists of pure SiNWs

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Fig 2 (a) SEM image of oriented SiNWs on the substrate (top

view, low magni cation), regions except white lines are composed

of SiNWs perpendicular to the substrate The length of SiNWs

is about 1 m, (b) SEM image of a cross part of the grooves.

SiNWs on the edge of grooves fall on to the substrate, (c) TEM

image of SiNWs with average diameter around 25 nm, which were

scrapped from the substrate The SAED pattern shown in inset

reveals characteristic ring pattern, showing that the nanowires are

completely amorphous (a-SiNWs).

Parts of a-SiNWs on the edge of chaps fall on the

substrate Fig 2(c) is the TEM image of ultra ne

SiNW, which were scratched from the substrate It

shows that the diameter of a-SiNWs is about 25 nm

The highly di usive ring pattern (inset) in select area

electron di raction (SAED) revealed that SiNWs are

completely amorphous Though the reason why the

resultant nanowires are amorphous instead of being

crystalline is not yet very clear, the authors think that

amorphous state was closely related to the fast growth speed in the present condition

It was found that the growth of the amorphous SiNWs here is di erent from the VLS mechanism for conventional whiskers [4–6], revealing a di er-ent growth mechanism In the case of oven-laser abla-tion approach [1,2], silicon source for SiNWs growth was supplied from the vapor phase in which atomic

Si species were ablated o by the laser beam, and the growth of the SiNWs is controlled by the well-known VLS mechanism The central idea of the VLS growth

of SiNWs is that, the catalysts (usually Ni, or Fe as impurity) act as a liquid-forming agent, which reacts with the vapor phase, and forms the NiSi2eutectic liq-uid droplets The vapor phase is rich in Si atoms With the further absorption of Si atoms into the droplets from the vapor phase, the droplets become supersat-urated, resulting in the precipitation of SiNWs from the droplets

In the present circumstance, however, the Si con-centration in the vapor phase is negligible at the growth temperature, because the speci c surface= volume ratio of bulk Si substrate is extremely low

On the other hand, the Si substrate was covered by a thin layer of Ni Therefore, the only possible silicon source comes from the bulk silicon substrate, because

no extra Si source was introduced in the vapor phase From the binary Ni–Si diagram, it is visible that the eutectic point of Si2Ni is 993C However, due to the melting e ect of small-size grains, the eutectic

lm can react with the Si substrate at temperature

C, and forms Si2Ni eutectic liquid alloy droplets Because of the relatively high solubility

di use through the solid (the substrate)–liquid inter-face into the liquid-phase (the Ni Si2 droplets) A second liquid–solid (nanowire) interface will form when the liquid phase becomes supersaturated due the growth of SiNWs Because this growth process involves solid–liquid–solid phases, it is named as a SLS growth, which is in fact an analogy of the VLS mechanism The growth process of the a-SiNWs via

an SLS model is depicted schematically in Fig 3 Cross-sectional SEM analysis of the sample pro-vided direct evidence to support the a-SiNW growth

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Fig 3 Schematic depiction of the SiNW growth via the SLS mechanism: (a) deposition of a thin layer of Ni on the Si (111) substrate; (b) formation of the Si–Ni eutectic liquid droplets; (c) the continuous di usion of Si atoms through the substrate–liquid (S–L) interface; (d) nal state of the SiNW growth The smooth surface of the original substrate becomes rough at the end of the SiNW growth.

via a SLS mechanism Fig 4(a) shows an SEM

image of oriented a-SiNWs grown on the substrate

(cross-sectional view) The a-SiNWs grew densely

and are all perpendicular to the substrate The length

of the SiNWs is about 1 m It is visible that

be-tween the SiNWs and the substrate there is a layer of

nano-sized particles which proved to consist of Ni and

Si Fig 4(b) shows a low-magni ed cross-sectional

SEM image It is visible that a layer of oriented

a-SiNWs was grown on the substrate EDS analysis

between the Si substrate and the a-SiNW layer further

con rmed that there is a thin layer of Si–Ni alloy,

which is indicated with a white arrow We found that

the a-SiNWs grow from base, which manifests itself

by the fact that the solidi ed Si–Ni nano particles

were visible between the surface of the substrate and

the a-SiNW lm, instead of being attached at the free

tip of the SiNWs

The SiNWs are interesting to evaluate the quantum

con nement e ect related to materials of low

dimen-sionality [10,11] The a-SiNWs grown on substrate

have remarkable surface=volume ratio, possibly

show-ing physical–chemical properties completely di erent

from the bulk From this point of view, it is speculated

that the a-SiNWs may have potential applications such

as rechargeable battery of high capacity with portable

size, which is closely related to the surface e ects In

fact, it was recently revealed that the lithium battery

using SiNWs as electrode materials showed a capacity

as high as 8 times than that of the ordinary one [12]

Fig 4 (a) Low and (b) magni ed cross-sectional SEM images of the SiNWs grown on Si (111) substrate, which is controlled by

a SLS mechanism The length of the SiNWs is about 1 m The Si–Ni particles are visible attached to the Si substrate surface.

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By optimizing dopants, it is believed that the a-SiNW

lm thus prepared will nd applications in future

nanotechnology

4 Summary remarks

In summary, oriented silicon nanowires have been

grown using Si substrate as Si source via a solid–

liquid–solid mechanism by heating They have

uni-form length and diameter The growth is explained

by solid–liquid–solid model This synthesis method of

oriented SiNWs is simple and controllable It can also

be used to synthesize other nanowires

Acknowledgements

This project was nancially supported by national

Natural Science Foundation of China (NSFC), and by

the Research Fund for the Doctoral Program of higher

Education (RFDP), China

References

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[2] D.P Yu, C.S Lee, I Bello, X.S Sun, Y.H Tang, G.W Zhou, Z G Bai, Z Zhang, S.Q Feng, Solid State Commun.

105 (1998) 403.

[3] D.P Yu, Z.G Bai, Y Ding, Q.L Hang, H.Z Zhang, J.J Wang, Y.H Zou, W Qian, H.T Zhou, G.C Xiong, S.Q Feng, Appl Phys Lett 72 (1998) 3458.

[4] R.S Wager, W.C Ellis, Appl Phys Lett 4 (1964) 89 [5] R.S Wager, W.C Ellis, Trans Metall Soc AIME 233 (1965) 1053.

[6] E.I Givargizov, J Crystal Growth 31 (1975) 20.

[7] M Yazawa, M Koguchi, A Muto, M Ozawa, K Hiruma, Appl Phys Lett 61 (1992) 2051.

[8] J Westwater, D.P Gosain, S Tomiya, S Usui, H Ruda,

J Vac Sci Technol B 15 (1997) 554.

[9] N Ozaki, Y Ohno, S Takeda, Appl Phys Lett 73 (1998) 3700.

[10] D.P Yu, Z.G Bai, J.J Wang, Y.H Zou, W Qian, J.S Fu, H.Z Zhang, Y Ding, G.C Xiong, S.Q Feng, Phys Rev B

59 (1999) 2498.

[11] J Hu, M Ouyang, P Yang, C.M Lieber, Nature 399 (1999) 48.

[12] G.W Zhou, H Li, H.P Sun, D.P Yu, Y.Q Wang, L.Q Chen, Ze Zhang, Appl Phys Lett 75 (1999) 2447.

... growth of SiNWs Because this growth process involves solid–liquid–solid phases, it is named as a SLS growth, which is in fact an analogy of the VLS mechanism The growth process of the a- SiNWs via. .. 4

Fig Schematic depiction of the SiNW growth via the SLS mechanism: (a) deposition of a thin layer of Ni on the Si (111) substrate; (b)... characteristic ring pattern, showing that the nanowires are

completely amorphous (a- SiNWs).

Parts of a- SiNWs on the edge of chaps fall on the

substrate

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