Possibility of graphene growth by close space sublimation
© Sopinskyy et al.; licensee Springer. 2014
Received: 3 December 2013
Accepted: 3 April 2014
Published: 14 April 2014
Carbon films on the Si/SiO2 substrate are fabricated using modified method of close space sublimation at atmospheric pressure. The film properties have been characterized by micro-Raman and X-ray photoelectron spectroscopy and monochromatic ellipsometry methods. Ellipsometrical measurements demonstrated an increase of the silicon oxide film thickness in the course of manufacturing process. The XPS survey spectra of the as-prepared samples indicate that the main elements in the near-surface region are carbon, silicon, and oxygen. The narrow-scan spectra of C1s, Si2p, O1s regions indicate that silicon and oxygen are mainly in the SiO x (x ≈ 2) oxide form, whereas the main component of C1s spectrum at 284.4 eV comes from the sp2-hybridized carbon phase. Micro-Raman spectra confirmed the formation of graphene films with the number of layers that depended on the distance between the graphite source and substrate.
PACS: 68.65.Pq; 81.15.-z; 81.05.ue
KeywordsGraphene films Deposition Graphite Sublimation Si/SiO2 substrate Raman spectroscopy Ellipsometry
Graphene attracts enormous interest due to its unique properties, such as high charge carrier mobility and optical transparency, in addition to flexibility, high mechanical strength, environmental stability[1–3]. These properties have already had a huge impact on fundamental science and are making graphene and graphene-based materials very promising for the whole series of applications starting with electronics and ending with medicine[2, 3]. It should be noted that currently the studies dealing with graphene are not limited to single-layer samples; the structures containing two or more graphene layers are also of interest.
In addition to deepening the understanding of the fundamental aspects of this material, the present stage of graphene research should target applications and manufacturing processes. Large-scale and cost-effective production methods are required with the balance between ease of fabrication and materials' quality[2, 3]. The placement of graphene on arbitrary substrates is also of key importance to its applications. The ideal approach would be to directly grow graphene where required (including dielectric surfaces). Despite the fact that at present there are quite a few proposed methods for the preparation of graphene films, we are still far from these goals. Therefore, further development of the existing methods of graphene film production as well as invention of new ones is in order.
Our first attempts to deposit graphene films directly onto the Si-SiO2 substrate should be considered in view of the abovementioned requirements. The close space sublimation (CSS) technique is very attractive in this sense because it is simple, inexpensive, and can be adapted for industrial use. Here we report our research into growing graphene films using CSS at atmospheric pressure.
The CSS technique was first proposed 50 years ago. It is based on the thermal-heating-induced sublimation of the source's material followed by vapor condensation onto the closely spaced substrate. The cross dimensions of the source and the substrate greatly exceed the distance between the source and the substrate. So far the CSS technique has been widely used in the production of thin films for solar cell applications. To our knowledge, CSS has not yet been used for production of graphene films. We simplified the design of the setup intended for film deposition as much as possible. In our case, carbon films were deposited using the thermal sublimation of the graphite at atmospheric pressure in the quasi-closed volume created inside a muffle furnace. This volume was the fused quartz crucible with ground stopper filled with densely packed fine TiO2 powder. (TiO2 was used because of its good chemically stability, high temperature stability, and corrosion resistance). Such a design has ensured reproducible results. The growth temperature was 850°C. The substrate was 130-nm-thick SiO2 film on silicon wafer obtained by oxidizing it in air at 1,100°C. Two types of film were investigated: one obtained using direct contact between the graphite plate and substrate (type I) and another obtained at 300-μm distance (type II).
Raman spectroscopy is one of the most effective tools for characterization of sp2 nanostructures, including graphene films. Specifically, the shape of the 2D Raman peak may serve as the fingerprint to distinguish single-, bi- and few-layer graphenes. That is why initially the prepared samples have been investigated by Raman spectroscopy. X-ray photoelectron spectroscopy (XPS) and ellipsometry are among the most powerful tools for investigation of very thin films. This determined the choice of these methods for the characterization of the obtained carbon deposits.
Micro-Raman spectra in the 1,000 to 3,000 cm-1 spectral range at room temperature and excitation wavelength 488 nm were registered using Horiba Jobin-Yvon T-64000 Raman spectrometer (Horiba Ltd., Edison, Kyoto, Japan). The laser spot size at the focus was around 1 μm in diameter, and laser power at the sample was 1 mW. The laser power density used (approximately 1 mW/μm2) was the maximum at which the heating of the sample there was not observed yet (i.e., at which there was no observable temperature shift of the phonon bands). Spectral resolution was 0.15 cm-1.
Isotropic uniform transparent layer (IUTL) with n, h
Isotropic uniform absorbing layer (IUAL) with n, k, h
Unaxially anisotropic uniform transparent layer (UAUTL) with n o, n e, h
Isotropic linearly non-uniform transparent layer (ILNUTL) with n b, n t, h
Isotropic linearly non-uniform absorbing layer (ILNUAL) with n b, n t, k b, k t, h
Here, h is the layer thickness and n, k are refractive and absorption index, respectively. Lower subscripts denote the following: o, ordinary; e, extraordinary; b, bottom; t, top.
The measured area was approximately 1 μm2 for micro-Raman, approximately 1 mm2 for ellipsometric, and approximately 20 mm2 for XPS measurements.
Results and discussion
More detailed information about the structure of sp2 carbon phase can be obtained from the 2D band analysis. Both the position and the shape of this band are different in these two spectra. The 2D band in both spectra is asymmetric. However, the details of this asymmetry differ.
In the type II sample, the band has the maximum at 2,709 cm-1 with the gentler drop on the high-energy side. The enlarged 2D band region of the type II sample is shown on Figure 2b. A detailed visual examination of this band shows that its shape and position are analogous to those observed for graphene films with number of layers 2 ≤ n ≤ 4[10–12]. From Figure 2b, it is also seen that the experimental 2D band is well fitted by two Lorentzian components. The characteristics of the deconvolution are similar to the characteristics of the 2D band deconvolution for micromechanically cleaved three- to four-layer graphene sheets on SiO2/Si substrate. There is yet another indication that the type II sample film has fewer graphene layers as compared to the type I sample - despite the greater number of defects in the type II sample (confirmed by the presence of D band in its spectrum), the I2D/IG ratio in the type II sample is still greater than in the type I sample.
Since the type II sample had fewer graphene layers, it had been studied in greater detail using XPS and ellipsometrical methods.
This should be considered as sufficient condition for IUTL-model adequacy. Thus, the oxide film obtained by oxidation of silicon on air is isotropic, uniform, and transparent. We emphasize that the n = 1.460 value corresponds to the refractive index value for SiO2 thermal oxide films.
As it can be seen within the framework of the IUTL-model, there is little change of n value, yet there is substantial increase of h value. This result shows that as far as the sample's optical properties are concerned, the most substantial result of carrying out the graphite sublimation process has been the thickening of the oxide film.
As it follows from these solutions, the anisotropy is the least responsible factor for the deviation of the sample's optical properties from the IUTL model; to a greater extent, this deviation is due to the appearance of absorption as well as vertical non-uniformity.
Lower subscripts denote the following: l, lower; u, upper. Note that in terms of both of these models, the n value of oxide film is below 1.46. It may be due to the appearance of porosity in the oxide film and/or change of its composition through the partial replacement of silicon atoms by carbon atoms.
The complication of the two-layer model by introducing birefringence, dichroism, non-uniformity in both lower and upper layers did not lead to any noticeable reduction of MSEmin, despite the fact that the number of variable parameters increased to 8. The obtained values of the parameters describing the deviation of these models from the ‘lower IUTL - upper IUAL’ model were small in this case. This indicates the sufficient adequacy of the ‘lower IUTL - upper IUAL’ model. Let us turn to the values of the optical constants of thin upper film. Its refractive index value (3.24) is higher and absorption index value (0.463) is lower than the reported values for bulk graphite, the film consisting of 8 to 9 graphene layers, and single-layer graphene (n = 2.73, k = 1.42 are found at λ = 633 nm for bulk graphite; n = 2.68, k = 1.24 at λ = 633 nm are found for the film consisting of 8 to 9 layers of graphene; n = 2.7 to 2.8, k = 1.4 to 1.6 and n = 2.5 to 2.7, k = 1.1 to 1.4 have been reported for single-layer graphene). On the other hand, these values are very close to the values of the optical constants for a-C films deposited using pulsed laser deposition (n ~ 3.10, k ~ 0.40 at λ = 633 nm). Also, the value of Imϵ = 2 × 3.24 × 0.463 = 3.00 calculated based upon our data is in the middle of the range for the values Imϵ = 2.0 to 4.0. This range has been previously obtained at λ = 633 nm for laser-irradiated carbon films with a large amount of graphite phase and dominating sp2-type bonds.
Thus, from the ellipsometric analysis, it follows that as a whole, the upper film can be treated as a disordered graphite-like layer having the thickness approximately equal to three-layer graphene. This result proves the realization of the first scenario among those that are compatible with XPS measurements. Weak intensity as well as unstructured micro-Raman spectra in most of the measured points of the type II sample indicates the formation of the strongly disordered amorphous carbon-based phase with large number of defects. (Similar character of the Raman spectra had been observed, for example, in the carbon films obtained by the electron-beam-induced high-speed evaporation of graphite on substrates preheated to 700°C to 800°C). The structure of such a type leads to significant (order of magnitude) decrease in inelastic light scattering cross-section. This, together with the small thickness of the film, explains the low intensity of the Raman signal in our case.
Thus, based on the data of all three characterization methods, we can state that in the sample of type II, the SiO2 film is covered with approximately 1-nm-thick film consisting of sp2 carbon-based highly disordered amorphous phase with some number of three-layer defective graphene inclusions.
Possible reasons for greater disordering and the number of defects of the in the type II sample deposited carbon film as compared to the type I one can be the greater distance between the source and substrate as well as a lot more gases of air in the sandwich during the type II sample preparation. Substantial changes in the silicon oxide film indicate the significant impact of the atmosphere taking place during the fabrication of the type II sample. First, its thickness increased, and its refractive index decreased. Second, attention should be given to the silicon oxide film growth rate during the graphite sublimation process: the oxide thickness increase was 13.4 nm in type II sample, but only 4.0 nm in the control Si-SiO2 sample placed in the oven near the quartz box. Such difference in the silicon oxidation rate can be explained by increase in the ‘source-substrate’ sandwich temperature. The increase in local temperature inside the sandwich is possible because the heating of graphite to 850°C in air should cause exothermic oxidation reactions with oxygen and water molecules. Authors showed that exposure of a few layer graphene films in air at T ≥ 600°C leads to the formation of defects. The defects are initially sp3 type and become vacancy-like at higher temperature. Thus, the abovementioned facts make it possible to think that more defective structure of carbon deposit in the type II sample is to great extent caused by the greater amount of the active air gases (oxygen, water vapor) as well as the higher local temperature in the sandwich. All of this is the consequence of greater distance between the graphite plate and the substrate.
The possibility of graphene fabrication using the simple and low-cost modified method of close space sublimation at the atmospheric pressure has been demonstrated. When carrying out carbon deposition under the same conditions, the thickness of several-layer graphene film decreases and its defectiveness increases with increase in the distance between the source and the substrate. This motivates further in-depth study of the mechanism of the film formation in order to develop the technological regimes that would allow fabrication of the better graphene films. First of all, it would be necessary to determine the influence of the atmosphere on the graphene film deposition process.
Close space sublimation
Highly ordered pyrolytic graphite
Isotropic linearly non-uniform absorbing layer
Isotropic linearly non-uniform transparent layer
Inverse task of ellipsometry
Isotropic uniform absorbing layer
Isotropic uniform transparent layer
Unaxially anisotropic uniform transparent layer
X-ray photoelectron spectroscopy.
- Castro Neto AH, Guinea F, Peres NMR, Novoselov KS, Geim AK: The electronic properties of graphene. Rev Mod Phys 2009, 81(1):109–162. 10.1103/RevModPhys.81.109View Article
- Grayfer ED, Makotchenko VG, Nazarov AS, Kim S-J, Fedorov VE: Graphene: chemical approaches to the synthesis and modification. Russ Chem Rev 2011, 80(8):751–770. 10.1070/RC2011v080n08ABEH004181View Article
- Bonaccorso F, Lombardo A, Hasan T, Sun Z, Colombo L, Ferrari AC: Production and processing of graphene and 2d crystals. Mater Today 2012, 15(12):564–589. 10.1016/S1369-7021(13)70014-2View Article
- Rao CNR, Sood AK, Voggu R, Subrahmanyam KS: Some novel attributes of graphene. J Phys Chem Lett 2010, 1(2):572–580. 10.1021/jz9004174View Article
- Nicoll FH: The use of close spacing in chemical-transport systems for growing epitaxial layers of semiconductors. J Electrochem Soc 1963, 110(11):1165–1167. 10.1149/1.2425614View Article
- Kiriya D, Zheng M, Kapadia R, Zhang J, Hettick M, Yu Z, Takei K, Wang H-HH, Lobaccaro P, Javey A: Morphological and spatial control of InP growth using closed-space sublimation. J Appl Phys 2012, 112(12):123102–1-123102–6.View Article
- Ferrari AC, Meyer JC, Scardaci V, Casiraghi C, Lazzeri M, Mauri F, Piscanec S, Jiang D, Novoselov KS, Roth S, Geim AK: Raman spectrum of graphene and graphene layers. Phys Rev Lett 2006, 97(18):187401–1-18740–4.View Article
- Sopinskyy MV, Shepeliavyi PE, Stronski AV, Venger EF: Ellipsometry and AFM study of post-deposition transformations in vacuum-evaporated As-S-Se films. J Optoelectron Adv Mater 2005, 7(5):2255–2266.
- Yoon D, Moon H, Cheong H, Choi JS, Choi JA, Park BH: Variations in the Raman spectrum as a function of the number of graphene layers. J Korean Phys Soc 2009, 55(3):1299–1303.
- Nagashio K, Nishimura T, Kita K, Toriumi A: Mobility variations in mono- and multi-layer graphene films. Appl Phys Express 2009, 2(2):025003–1-025003–3.
- Wang K, Tai G, Wong KH, Lau SP, Guo W: Ni induced few-layer graphene growth at low temperature by pulsed laser deposition. AIP Adv 2011, 1(2):022141–1-022141–9.View Article
- Wang YY, Ni ZH, Yu T, Shen ZX, Wang HM, Wu YH, Chen W, Wee ATS: Raman studies of monolayer graphene: the substrate effect. J Phys Chem C 2008, 112(29):10637–10640. 10.1021/jp8008404View Article
- Ren PG, Yan DX, Ji X, Chen T, Li ZM: Temperature dependence of graphene oxide reduced by hydrazine hydrate. Nanotechnology 2011, 22: 055705–1-055705–8.
- Werner H, Schedel-Niedrig T, Wohlers M, Herein D, Herzog B, Schlögl R, Keil M, Bradshaw AM, Kirschner J: Reaction of molecular oxygen with C60: spectroscopic studies. J Chem Soc Faraday Trans 1994, 90(3):403–409. 10.1039/ft9949000403View Article
- Kalita G, Adhikari S, Aryal HR, Umeno M, Afre R, Soga T, Sharon M: Fullerene (C60) decoration in oxygen plasma treated multiwalled carbon nanotubes for photovoltaic application. Appl Phys Lett 2008, 92(6):063508–1-063508–3.View Article
- Borghesi A, Guizzetti G: Graphite (C). In Handbook of Optical Constants of Solids, vol. II. Edited by: Palik ED. San Diego: Academic; 1991:449–460.
- Albrektsen O, Eriksen RL, Novikov SM, Schall D, Karl M, Bozhevolnyi SI, Simonsen AC: High resolution imaging of few-layer graphene. J Appl Phys 2012, 111(6):064305–1-064305–8.View Article
- Kravets VG, Grigorenko AN, Nair RR, Blake P, Anissimova S, Novoselov KS, Geim AK: Spectroscopic ellipsometry of graphene and an exciton-shifted van Hove peak in absorption. Phys Rev 2010, B81(15):155413–1-155413–6.
- Weber JW, Calado VE, van de Sanden MCM: Optical constants of graphene measured by spectroscopic ellipsometry. Appl Phys Lett 2010, 97(9):091904–1-091904–3.View Article
- Miyajima Y, Henley SJ, Adamopoulos G, Stolojan V, Garcia-Caurel E, Drévillon B, Shannon JM, Silva SRP: Pulsed laser deposited tetrahedral amorphous carbon with high sp3 fractions and low optical bandgaps. J Appl Phys 2009, 105(7):073521–1-073521–8.View Article
- Grigonis A, Rutkuniene Z, Medvid A, Onufrijevs P, Babonas J: Modification of amorphous a-C:H films by laser irradiation. Lithuanian J Phys 2007, 47(3):343–350. 10.3952/lithjphys.47321View Article
- Evtukh AA, Klyui MI, Krushins’ka LA, Kurapov YA, Litovchenko VG, Luk’yanov AM, Movchan BO, Semenenko MO: Emission properties of structured carbon films. Ukr J Phys 2008, 53(2):177–184.
- Marsh H: Introduction to Carbon Science. London: Butterworths; 1989.
- Nan HY, Ni ZH, Wang J, Zafar Z, Shi ZX, Wang YY: The thermal stability of graphene in air investigated by Raman spectroscopy. J Raman Spectr 2013, 44(7):1018–1021. 10.1002/jrs.4312View Article
This article is published under license to BioMed Central Ltd. This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/2.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly credited.