Journal of NanomaterialsVolume 2011 (2011), Article ID 279686, 7 pagesdoi:10.1155/2011/279686

Research Article

Angular Distribution of Damping Coefficient of Ablated Particle in Pure He, Ne, and Ar Gases

Yinglong Wang, Xiaolin Zhai, Xuecheng Ding, Ziqiang Hu, Lizhi Chu, Zechao Deng, Weihua Liang, Yajun Zhao, and Guangsheng Fu

College of Physics Science and Technology, Hebei University, Baoding 071002, Hebei, China

Received 5 June 2011; Revised 26 July 2011; Accepted 26 July 2011

Academic Editor: Gong Ru Lin

Copyright © 2011 Yinglong Wang et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

Abstract.

To investigate the angular distribution of damping coefficient of ablated particle under various ambient gases, nanocrystalline silicon films are systemically deposited on a circular substrate by pulse laser ablation in pure He, Ne, and Ar gases, respectively. Scanning electron microscopy images and Raman and X-ray diffraction spectra indicate that the average size of Si nanoparticles decreases with the increase of the departure angle between the film and the plume, and Ne gas induces the smallest and most uniform Si nanoparticles in size among all the three gases. Further theoretical simulation demonstrates the bigger the departure angle, the smaller the damping coefficient of ablated particle, and the damping coefficient in Ne gas is largest for the same angle, implying the most effective energy transfer between Si and ambient atoms.

1. Introduction

There is a significant growing interest in nanocrystalline silicon (nc-Si) thin films [1–3] containing a lot of Si nanoparticles (np-Sis) for their potential applications in optoelectronic integration and high-efficiency solar cell [4–7]. In these applications, the controllability of the average size and size distribution of the np-Sis in the prepared films should be crucial aspects to be considered. In order to better control the size and its distribution of the np-Sis, it is fundamental and necessary to study the main factors that affect nucleation and growth during their preparation. Several preparation methods of the nc-Si films have been developed, such as the chemical vapor deposition (CVD) [8, 9], magnetron sputtering (MS) [10], molecular-beam epitaxy (MBE) [11, 12], heterogeneous dilution (HD) [13], and pulsed laser deposition (PLD) [14–17]. PLD technology is of great importance due to the high growth rate and high purity of the prepared thin films [18]. For PLD, the inert gas is introduced into the deposition chamber as the ambient gas, and both the experimental and theoretical results demonstrate that the average size of np-Sis can be altered by modulating the type of ambient gas, pressure, and so on. During nucleation and growth of the np-Si, collisions between Si atoms and ambient gas are crucial. An inertia fluid model can consistently explain the experimental results on dependence on the size of np-Sis He pressure [19]. This model indicates that the drag force of the ablated particle is proportional to the square of velocity , namely, , in which is the damping coefficient. And the kinetic energy difference between ablated particles initially ejected and ablated particles at end of flight is proportional to the cohesive energy of the as-formed np-Sis. Additionally, the size distribution of np-Sis prepared by PLD at various gases (He, Ar, and Ne) has been studied [20]. The results show that Ne induces the most uniform np-Sis among all the three deposition gases, which mainly results from the adjacent degree between the ambient gas and Si atomic weight. However, the above discussions are restricted to the axial direction of plasma.

In this paper, we report the dependence of damping coefficient on angle during PLD in pure He, Ne, and Ar gases, respectively.

2. Experimental Setup

The pulse laser deposition equipment is composed of a laser source and a vacuum system, as shown in Figure 1. A Lambda Physik XeCl excimer laser (wavelength: 308 nm, pulse duration: 15 ns, repetition: 1 Hz, energy fluence: 4 J/cm²) is focused on surface (ablation spot area: 2 mm²) of a single crystalline Si target (resistivity: 3000 Ω·cm) continually rotating during the deposition, intersection angle of the laser and target surface being 45°. A series of single Si (111) or glasses wafer are placed along the inner half circle of the substrate with diameter of 3 cm and center of circle locates at the ablation spot of the laser. High-purity (99.9995%) He, Ne, and Ar are introduced into the chamber, respectively, as the ambient gases are to be kept at 10 Pa after the base pressure reached  Pa. The nc-Si films are directly deposited on the substrate at the room temperature, and deposition time is 3 minutes and 3 hours for the Si and glasses wafer, respectively. The JSM-7500 type lull emission scanning electron microscopy (SEM) of Japanese electronics manufacturer, Rigaku D/Max type of X-ray diffraction (XRD) of Japan Rigaku Production Company and Raman scattering of MLI-2000 type apparatus are employed to characterize the surface morphology and microstructure of Si films.

Figure 1: The schematic diagram of the experiment used to study the angular distribution of damping coefficient of ablated particle in pure He, Ne, and Ar gases.

3. Results and Discussions

In the experiment, the nc-Si thin films are, respectively, deposited on the glass wafer at the 0° angle (facing the plume) under He, Ne, and Ar and then measured by the Raman spectrum and X-ray diffraction (XRD). The results are shown in Figures 2(a) and 2(b), respectively. In Figure 2(a), the Raman spectrum peaks of the thin films are located at 519.1, 518.2, and 517.4 cm⁻¹, respectively, all of them deviating from the monocrystalline Si peak of 520 cm⁻¹. In Figure 2(b), the 28.4° and 47.3° spectra with board width are present in XRD spectrum of the films, which correspond to Si (111) and (220) crystal diffraction, respectively, compared with the standard PDF cards. The measured values above indicate that np-Sis have been formed in the film.

(a)

(b)

Figure 2: The Raman sepctrum (a) and XRD (b) of Si films deposited by pulsed laser deposition in 10 Pa He, Ne, and Ar gases, respectively.

3.1. The Average Size versus the Angle

The SEM images of the nc-Si films prepared at the angles of −80°, −60°, −30°, 0°, 30°, 60°, and 80° under He, Ar, and Ne, respectively, are present in (a)–(g) of Figures 3, 4, and 5, in which the insets present the corresponding size distribution of np-Sis. Obviously, the nanoparticles are inserted in the films. Comparing the data at the same angle in the three gases, one can distinguish that the nanoparticles are more uniformly distributed in films prepared in Ar and Ne than in He and the sizes of nanoparticles formed in Ar and Ne are smaller than the ones in He at the 0° angle. At the same time, the widths of the size distribution of the nanoparticles increase gradually in Ne, Ar, and He, namely, the probable radius of the nanoparticles increases gradually.

(a)

(b)

(c)

(d)

(e)

(f)

(g)

Figure 3: SEM images of the Si films deposited by pulsed laser deposition in 10 Pa He environment gas, where (a), (b), (c),(d), (e), (f), and (g) correspond to various angles of fixed Si wafers: −80°,−60°, −30°, 0°, 30°, 60°, and 80°, respectively.

(a)

(b)

(c)

(d)

(e)

(f)

(g)

Figure 4: SEM images of the Si films deposited by pulsed laser deposition in 10 Pa Ne environment gas, where (a), (b), (c), (d), (e), (f), and (g) correspond to various angles of fixed Si wafers: −80°,−60°, −30°, 0°, 30°, 60°, and 80°, respectively.

(a)

(b)

(c)

(d)

(e)

(f)

(g)

Figure 5: SEM images of the Si films deposited by pulsed laser deposition in 10 Pa Ar environment gas, where (a), (b), (c), (d), (e), (f), and (g) correspond to various angle of fixed Si wafers: −80°,−60°, −30°, 0°, 30°, 60°, and 80°, respectively.

In order to quantitatively study the changing relationship between the size distribution of the nanoparticles and the angles in the three ambient gases, more than 100 nanoparticles in each SEM image are statistically analyzed by Photoshop software, displayed in Figure 6. The results show that the size of np-Sis decreases with the increase of the angle, all for He, Ar, and Ne. Moreover, the average sizes of nanoparticles in all the films prepared under the three gases are maximal at 0°, namely, at the position facing the plume. Because the substrate is not heated, the nanoparticles are formed by undergoing gas phase nucleation [21]. After the pulse laser ablates the single crystalline Si target, ablation particles are ejected out to all directions, with velocities approximately satisfying the Maxwell velocity distribution [22], and then transported and deposited on the substrates. In the transporting process, the ablated particles collide with the ambient gas atoms and constantly lose kinetic energy which supplies the cohesion energy forming np-Sis [23]. The initial velocity of ablation particles is related to the propagation direction and has the maximal value along axial direction of the plume. For 0° with maximal velocity, the lost kinetic energy is maximal; thus, the formed np-Si is the largest. Because the velocity of the ablated particles decreases with the angles, the smaller nanoparticles will be formed at larger angle. As we know, the adjacent degree between the ambient and Si atomic weight is the crucial factor to the size and its distribution of np-Sis [24]. If the ambient atomic weight is close to Si atomic weight, the size distribution range is narrow and the formed np-Si is small. The atomic weight of He, Ne, Ar, and Si is 4.00 u, 20.17 u, 39.95 u, and 28.09 u, respectively. Obviously, atomic weight of He is the most different from the Si. Thus, for the same angle, the largest and least uniform nanoparticles in size are found in He gas, and Ne induces the smallest and most uniform np-Sis among all the three deposition gases, which is in good agreement with the SEM images.

Figure 6: The average size versus the angle by pulsed laser deposition in 10 Pa He (-■-), Ar (-●-), and Ne (-▲-), respectively.

3.2. The Damping Coefficient versus the Angle

In inertia model [19], drag force is directly composed of mass displacement and is proportional to the square of velocity of the ejected material throughout flight in the inert ambient gas. The equation of motion for the ejected material is where is the damping coefficient.

In this tentative model, the kinetic energy difference between atoms initially ejected and atoms at the end of flight () is proportional to the cohesive energy of the as-formed nanoparticles () where is the initial velocity, is proportional constant, is the mass of the ablated particle, and is the distance from the target to the position that growth of np-Si ends. In our experimental condition, approximation of low ambient gas density and short target-substrate distance can be applied. Therefore, (2) can be rewritten as follows: We assume that cohesive energy of per unit volume () is a constant, and the cohesive energy for a spherical nanoparticle with average radius () can be defined as The Monte Carlo simulation is a convenient method to demonstrate PLD dynamic process [25]. Using this method, we can calculate that the average velocity of ablated particles along plume axis is  m/s, and the growth position (the mixed region of high density Si vapor and the ambient gas) oscillates continuously between the target and substrate. The maximal positions for He, Ar, and Ne are 0.97 cm, 0.71 cm, and 0.60 cm, respectively.

According to the literature [24], the velocity at directions is where represents the angle formed by the substrate position and plume axis. Combining (2) and (5), we can get the damping coefficient, defined as According to (6) and depending on the average size and velocity of ablated particles at different angles under pure He, Ne, and Ar gases, respectively, the relationship of damping coefficient and the angle is fitted, as shown in Figure 7. The theoretical simulation demonstrates the bigger the departure angle, the smaller the damping coefficient of ablated particle, and the damping coefficient in Ne gas is largest for the same angle, implying the most effective energy transfer between Si and ambient atoms.

Figure 7: The damping coefficient versus the angle by pulsed laser deposition in 10 Pa He (-■-), Ar(-●-), and Ne (-▲-), respectively.

4. Conclusions

In conclusion, angular distribution of damping coefficient of ablated particle under various ambient gases (He, Ar and Ne) has been studied. The results show that the average size of Si nanoparticles decreases with the increase of the departure angle between the film and the plume, and Ne gas induces the smallest and most uniform Si nanoparticles in size among all the three gases. Further theoretical simulation demonstrates the bigger the departure angle, the smaller the damping coefficient of ablated particle, and the damping coefficient in Ne gas is largest for the same angle, implying the most effective energy transfer between Si and ambient atoms. This may pave the way for effectively controlling the grain size and size distribution of nanoparticles of silicon as well as other materials prepared by the pulsed-laser ablation method.

Acknowledgments

The paper was financially supported by Project supported by the National Basic Research Program of China (Grant no. 2011CB612305), National Science Foundation of China (NSFC) (Grant no. 10774036), the NSF of Hebei Province (E2011201134) and foundation of Hebei University. Support from the Hebei Key Laboratory of Optic-electronic Information & Materials is also acknowledged.

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