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Electrical and Optical Properties of Au-Catalyzed GaAs Nanowires Grown on Si (111) Substrate by Molecular Beam Epitaxy
Nanoscale Research Lettersvolume 12, Article number: 290 (2017)
In this study, defect-free zinc blende GaAs nanowires on Si (111) by molecular beam epitaxy (MBE) growth are systematically studied through Au-assisted vapor-liquid-solid (VLS) method. The morphology, density, and crystal structure of GaAs nanowires were investigated as a function of substrate temperature, growth time, and As/Ga flux ratio during MBE growth, as well as the thickness, annealing time, and annealing temperature of Au film using scanning electron microscopy (SEM), transmission electron microscopy (TEM), X-ray diffraction (XRD), cathodoluminescence (CL), and Raman spectroscopy. When the As/Ga flux ratio is fixed at 25 and the growth temperature at 540 °C, the GaAs nanowires exhibit a defect-free zinc blende structure with uniform and straight morphology. According to the characteristics of GaAs nanowires grown under varied conditions, a growth mechanism for defect-free zinc blende GaAs nanowires via Au-assisted vapor-liquid-solid (VLS) method is proposed. Finally, doping by Si and Be of nanowires is investigated. The results of doping lead to GaAs nanowires processing n-type and p-type semiconductor properties and reduced electrical resistivity. This study of defect-free zinc blende GaAs nanowire growth should be of assistance in further growth and applications studies of complex III-V group nanostructures.
Semiconductors are expected to shrink in scale to sub 10 nm. In this regard, the semiconductor industry is being severely challenged to produce semiconductor materials of suitable mobility (boosted processing speed) and architecture (for reduced power leakage) on a nanometric scale . There is an urgent need for the development of semiconductor materials that can address this problem. Since unique electrical and optical properties are required, III-V group semiconductors have been proposed as candidates to replace Si as a high-speed device material [2–5]. One such material is gallium arsenide (GaAs). It is representative of III-V group semiconductor materials and possesses a direct bandgap of 1.424 eV [6, 7]. III-V group semiconductor nanowire arrays of high volume to surface ratios are potential materials whose bandgap can be tuned for the efficient transfer of solar energy to electric energy [8–10]. The literature presents various examples of the growth of binary and ternary III-V group semiconductor nanowires with controlled bandgaps on various substrates. Among these studies, single-crystal GaAs is used as a homogeneous substrate for growing GaAs semiconductor nanowires [11, 12]. However, single-crystal GaAs substrate is expensive and difficult to integrate into the present Si-based industry. On this basis, Si substrates are more desirable in support of III-V group semiconductor nanowire growth via vapor-liquid-solid (VLS) mechanism or deposit of a GaAs film as a buffer layer [13–15]. VLS as a growth method is popular as it facilitates reduced growth temperatures. Lower growth temperatures inhibit strain and defects causing lattice mismatching. Furthermore, small lattice mismatch also helps zinc blende GaAs to overcome strain issue as grown on Si substrate. Si is diamond structure and its lattice constant is 0.5431 nm, on the other hand, GaAs is zinc blende structure and its lattice constant is 0.5653 nm. The small lattice mismatch, ~4%, leads to GaAs nanowires could epitaxial growth on Si substrate . There are many studies point that diameters, density, and quality of nanowires/nanorods are influenced by growth parameters, such as thickness and annealing temperature via Au-catalyzed VLS growth mechanism [16–19]. Over the past several years, the synthesis of GaAs nanowires (NWs) on Si has predominantly been investigated using metal organic vapor phase epitaxy via a Au-catalyzed VLS mechanism [20–24]. On the other hand, few studies have employed molecular beam epitaxy (MBE) technique. In this systematic study, GaAs nanowires are grown under an MBE system on Si (111) via Au-catalyzed VLS mechanism. The investigation includes thickness and annealing conditions of the Au film, Ga to As flux ratio, growth temperature, dopant (Si and Bi) effects on electrical properties, and optical properties.
Samples were grown on Au film-coated Si (111) substrates in a Varian Modular GEN-II MBE system. Before using an e-gun to deposit thickness-varied Au film (0.6, 1, 1.5, and 2.0 nm), the silicon native oxide on the Si (111) substrate is removed by 1 wt% HF then rinsed with DI water and dried with N2 gas. In this work, all MBE system sources for growing nanowires are solid elements (including Ga, Be, Si, and As) and their flux is controlled using a temperature controller and shutter under 1 × 10−10 Torr. Au film is annealed to form nanoparticles on the Si (111) substrate then Ga and As are provided to grow GaAs nanowires. For in situ Si- and Be-doped GaAs nanowires, the concentrations of Si and Be are tuned by controlling the solid elements temperature. Doping temperatures of Si and Be are 1250~1400 °C and 1000~1150 °C, respectively. The corresponding concentrations and carrier species of Si- and Be-doped GaAs samples are calibrated by Hall measurement to confirm. To prepare samples for Hall measurement, (111) Si substrate without Au film is used to deposit GaAs films with different dopant source temperatures. SEM images were obtained using a HITACHI-S4700 field-emission SEM, operated at 5–15 kV accelerating voltage. The TEM samples were prepared by drop-casting nanostructures from toluene dilute dispersions onto 200-mesh carbon-coated copper grids (Electron Microscope Sciences). Energy dispersive spectrometry was conducted using a 200-kV accelerating voltage on a JEOL JEM-2100F. X-ray diffraction (XRD) was performed with a Rigaku Ultima IV X-ray diffractometer using Cu Kα radiation (λ = 1.54 Å) with of 1°/min scan rate. A cathodoluminescence (CL) detector was attached to SEM, and Raman spectrum was measured through Horiba, HR 800 by 633 nm laser and electrical properties measured by Keithly-590 for I-V curves.
Results and Discussion
The growth temperature window of Au-catalyzed GaAs nanowires is 520–620 °C [4, 8]. In this work, the optimal conditions for Au film thickness and annealing temperature are 1.0 nm and 580 °C for 10 min, respectively. Figure 1a shows a representative SEM image of Au-catalyzed GaAs nanowires grown on Si (111) substrate at 540 °C for 15 min with Ga/As flux ratio of 1/25. The diameter and length of Au-catalyzed GaAs nanowires are 26.2 ± 3.4 nm and 424.4 ± 13.4 nm, respectively. The products were further analyzed using grazing-incident X-ray diffraction (XRD). The result shown in Fig. 1b indicates that GaAs nanowires are crystalline and all peaks can be ascribed to a zinc blende structure with lattice constants of a = 0.5653 nm (JCPDS No. 89-2770). A strong (111) peak implies that the GaAs nanowires are textured on the Si (111) substrate. Since arsenic evaporates from GaAs at high temperatures, a high-As ambience is needed to produce high-quality GaAs nanowires. The growth rate of Au-catalyzed GaAs nanowires is limited by the participation of Ga from saturated AuGa x alloy. Environmental Ga atoms react with excess As to form polycrystalline GaAs on Si (111) surface, and the taper-shaped GaAs nanowires will be formed . Raman spectroscopy is shown in Fig. 1c. Peaks at 291 and 267 cm−1 are contributed by GaAs zinc blende structure. No wurtzite structure peaks are found at 259 cm−1 (the peak at 520 cm−1 is contributed from the Si substrate). The bandgap of the zinc blende structure and wurtzite structure of GaAs are 1.424 and 1.46 eV at 300 K, respectively; their corresponding illumination wavelengths are 870 and 850 nm. Figure 1d is the CL result of Au-catalyzed growth GaAs nanowires that measured at room temperature. The density of GaAs NWs and thickness of lateral grown GaAs layer are different for varied growth conditions that the CL intensity of GaAs NWs does not be compared but their full width at half maximum (FWHM) is similar. Furthermore, the CL peak at 870 nm confirms the product of GaAs nanowires is a zinc blende structure. The CL results show that the strong emission signal at 870 nm relates to the bandgap of the GaAs array nanowires. Because the CL peak is sharp, the Au-catalyzed growth GaAs array nanowires must have a good crystalline structure. No other peak was detected by CL spectrometry meaning no other defect was introduced into Au-catalyzed growth GaAs array nanowires. Even if high-concentration dopants of Si or Be are added into the Au-catalyzed growth GaAs array nanowires, the spectra of Raman and CL are consistent with XRD results in Fig. 1b.
Figure 2a gives a bright-field transmission electron microscope (TEM) image of a representative Au-catalyzed GaAs nanowire. An AuGa x alloy nanoparticle with dark contrast is clearly shown at the top of the straight and smooth GaAs nanowire. A high-resolution TEM (HRTEM) image and selected area electron diffraction (SAED) pattern of the corresponding GaAs nanowire are shown in Fig. 2b, c, respectively. The HRTEM image shows that the Au-catalyzed GaAs nanowire has a single-crystalline structure and (111) planes are observable along the  direction with a 3.26-nm spacing. The SAED pattern result in Fig. 2c further confirms the Au-catalyzed GaAs nanowire is a zinc blende structure grown in the (111) direction. This result is consistent with XRD, Raman, and CL results in Fig. 1b–d. Figure 2d, e is the energy dispersive spectrometer (EDS) spectra of Au-catalyzed GaAs nanowires taken from the top of the AuGa x nanoparticle and stem of the GaAs nanowire, respectively. EDS spectrum of Fig. 2d shows the compositions of the nanoparticle at the top are Au and Ga without As proving that the GaAs nanowires are catalyzed by AuGa x droplets and As atoms react with Ga segregated at AuGa x -GaAs interface. The ratio of Ga/As of EDS spectrum in Fig. 2e is about 1 meaning Au-catalyzed GaAs nanowires are grown at a moderate growth rate. The signal peaks for Cu and C come from the carbon-coated copper grid used as the electron transmission holder to suspend GaAs nanowires for TEM analysis.
As growth times increase (15, 30, 45, and 60 min), the length and diameter of GaAs nanowires increases but so too does the surface roughness. Longer GaAs nanowires are formed when As atoms experience longer diffusion paths to reach Au-Ga interface to form GaAs. Further, environmental Ga reacts with As at the sidewall of GaAs nanowires increasing nanowire diameters. SEM images in Fig. 3a–d show the length and diameter of GaAs nanowires with time: (a) 15, (b) 30, (c) 45, and (d) 60 min. The length of GaAs nanowires grows from hundreds of nanometers to micrometers, and diameters increase from 26.2 to 35.1 nm. These results indicate the importance of controlling Ga and As flux to manage GaAs nanowire morphology and surface roughness. Figure 3e, f shows growth time vs nanowire diameter and length, respectively. The results imply that the growth rate is not limited by diffusion since the length of GaAs nanowires is linearly proportional to the growth time not the root mean square of time (t 1/2) [25, 26]. It is likely controlled by precipitation of Ga from the interface of liquid AuGa x droplets and solid GaAs nanowires or the As diffusion rate. Tapered structures are observed in Fig. 3c, d as growth time increases . As mentioned above, this is caused by As experiencing a longer diffusion path before reacting with Ga at the interface between liquid AuGa x droplets and solid GaAs, as well as As atoms reacting with precipitated ambient Ga atoms provided by the MBE chamber to produce GaAs at the sidewall of nanowires forming tapered structures. Since tapering and surface roughness increase with time and these factors may negatively affect optimal optical and electrical properties of GaAs nanowires, we analyze the optical and electrical properties of nanowires grown at a fixed time of 10 min. Figure 3g–j give Au film thickness, As flux, annealing temperature, and growth temperature for Au-catalyzed GaAs nanowires. The figures show the progression of a typical VLS nanowire growth mechanism. Initially, Au film annealed to form droplets (Fig. 3g) then an Au-Ga alloy forms to produce the AuGa x alloy catalyst (Fig. 3h). Subsequently, Ga is segregated from the AuGa x under supersaturation conditions (Fig. 3j) to form axial growth of GaAs nanowires. From SEM images, the fast growth rate of Au-catalyzed GaAs nanowires suppresses lateral growth meaning overcoating on the surface of GaAs nanowires does not occur. The exclusive supply of Ga and As atoms from AuGa x droplets results in this fast growth rate with no lateral overgrowths. Fewer lateral overgrowths means fewer nanowire defects. Varied Au films, 0.6, 1.0, 1.5, and 2.0 nm, deposited by e-gun then annealed at 580 °C for 10 min are used to study the influence of Au thickness in GaAs NW growth. SEM images in Fig. 4 display Au film cannot form drop as its thickness is thicker than 1.5 nm; on the other hand, thinner Au film, 0.6 nm, leads to grow lower density of GaAs NWs.
In situ Si and Be doping effects are investigated in terms of the electrical properties of Au-catalyzed GaAs nanowires with different dopant source temperatures to control doping concentrations. In this work, FIB is used for depositing Pt as contact electrodes for the electrical characterization. Figure 5f, g is the results of electrical measurements with different concentrations of Si and Be dopants, respectively. The I-V curves of Fig. 5a are Si dopant source temperatures at 1250, 1300, 1350, and 1400 °C for fabricating single Au-catalyzed GaAs nanowire devices for measurement. High Si source temperatures mean high concentrations of Si; however, I-V measurements show lower conductivity for Si source at higher than 1300 °C. According to XRD, TEM, CL, and Raman results of GaAs grown at 1350 °C, the structure is still zinc blend. Since Si is an amphoteric dopant for GaAs, it seems that As sites are substituted by partial Si atoms. Be is a typical n-type dopant for a GaAs donor. In this work, Be source temperatures are 1000, 1050, and 1100 °C for adjusting Be concentrations in the Au-catalyzed GaAs nanowires. Figure 5b shows the corresponding I-V measurement results of varied Be source temperatures. As temperature increases, conductivity increases meaning donor Be atoms successfully substitute As sites enhancing carrier transport. Furthermore, the dopant concentrations affect to the electrical resistivity but do not change the structure of GaAs nanowire as the doping levels are 1019~1018/cm3 and 1015~1018/cm3 with Si and Be as a dopant, respectively. Concentrations of Si and Be doped GaAs samples are calibrated by Hall measurement to confirm whether the carrier types are electrons or holes. To prepare samples for Hall measurement, (111) Si substrate without Au film is used to deposit GaAs films with different dopant source temperatures. Table 1 gives the results of Si-doped and Be-doped Au-catalyzed GaAs nanowire electrical measurements. Electrical resistivity is determined by single Au-catalyzed GaAs nanowire devices, carrier concentrations, and carrier species are determined by Hall measurement.
Au-catalyzed GaAs nanowires were grown using an MBE system. Diameter and length density were controlled for thickness, annealing time, annealing temperature of the Au film, Ga/As ratio, and growth temperature. A growth model for Au-catalyzed GaAs nanowires was elucidated based on the analysis of SEM, XRD, and TEM results. Electrical properties of Au-catalyzed GaAs nanowires can be adjusted by controlling concentrations of Be and Si dopants through source temperatures. The carrier species and concentrations in Au-catalyzed GaAs nanowires are calibrated through Hall measurement at room temperature. High Si dopant source temperatures affect substitution sites; further, different concentrations of Si-doped and Be-doped Au-catalyzed GaAs nanowires are fabricated as single devices to measure their electrical resistivity and compare these results using Hall measurement.
Molecular beam epitaxy
Scanning electron microscopy
Transmission electron microscopy
Selected area electron diffraction
Energy dispersive spectrometer
Leong M, Doris B, Kedzierski J, Rim K, Yang M (2004) Silicon Device Scaling to the Sub-10-nm Regime. Science 306:2057–2060
Dayeh SA, Aplin DPR, Zhou X, Yu PKL, Yu ET, Wang D (2007) High Electron Mobility InAs Nanowire Field-Effect Transistors. Small 3:326–332
Ford AC, Ho JC, Chueh YL, Tseng YC, Fan Z, Guo J, Bokor J, Javey A (2009) Diameter-Dependent Electron Mobility of InAs Nanowires. Nano Lett 9:360–365
Chueh YL, Ford AC, Ho JC, Jacobson ZA, Fan Z, Chen CY, Chou LJ, Javey A (2008) Formation and characterization of NixInAs/InAs nanowire heterostructures by solid source reaction. Nano Lett 8:4528–4533
Ko H, Takei K, Kapadia R, Chuang S, Fang H, Leu PW, Ganapathi K, Plis E, Kim HS, Chen SY, Madsen M, Ford AC, Chueh YL, Krishna S, Salahuddin S, Javey A (2010) Ultrathin compound semiconductor on insulator layers for high-performance nanoscale transistors. Nature 468:286–289
Hoang TB, Moses AF, Zhou HL, Dheeraj DL, Fimland BO, Weman H (2009) Observation of free exciton photoluminescence emission from single Wurtzite GaAs nanowires. Appl Phys Lett 94:133105
Wang H (2013) High gain single GaAs nanowire photodetector. Appl Phys Lett 103:093101
Saxena D, Mokkapati S, Parkinson P, Jiang N, Gao Q, Tan HH, Jagadish C (2013) Optically pumped room-temperature GaAs nanowire lasers. Nat Photonics 7:963–968
Czaban JA, Thompson DA, LaPierre RR (2009) GaAs core-shell nanowires for photovoltaic applications. Nano Lett 9:148–154
Mariani G, Scofield AC, Hung CH, Huffaker DL (2013) GaAs nanopillar-array solar cells employing in situ surface passivation. Nat Commun 4:1497
Morral AFI, Spirkoska D, Arbiol J, Heigoldt M, Morante JR, Abstreiter G (2008) Prismatic quantum heterostructures synthesized on molecular-beam-epitaxy GaAs nanowires. Small 4:899–903
Noborisaka J, Motohisa J, Hara S, Fukui T (2005) Fabrication and characterization of freestanding GaAs/AlGaAs core-shell nanowires and AlGaAs nanotubes by using selective-area metalorganic vapor phase epitaxy. Appl Phys Lett 87:093109
Wen L, Li X, Zhao Z, Bu S, Zeng XS, Huang JH, Wang Y (2012) Theoretical consideration of III-V nanowire/Si triple-junction solar cells. Nanotechnology 23:505202
Chen SY, Wang CY, Ford AC, Chou JC, Wang YC, Wang FY, Ho JC, Wang HC, Javey A, Gan JY, Chen LJ, Chueh YL (2013) Influence of catalyst choices on transport behaviors of InAs NWs for high-performance nanoscale transistors. Phys Chem Chem Phys 15:2654–2659
Chu CP, Arafin S, Nie T, Yao K, Kou X, He L, Wang CY, Chen SY, Chen LJ, Qasim SM, BenSaleh MS, Wang KL (2014) Nanoscale growth of GaAs on patterned Si(111) substrates by molecular beam epitaxy. Cryst Growth Des 14:593–598
He L, Xiong B, Zhou P, Luo W, Song P, Wang X, Hao Z, Yang X, Niu C, Tian X, Yan M, Mai L (2016) P-doped germanium nanowires with Fano-broadening in Raman spectrum. J Wuhan Univ Technol-Mater Sci Ed 31:52–57
Li CB, Usami K, Mizuta H, Oda S (2009) Vapor-solid-solid radial growth of Ge nanowires. J Appl Phys 106:046102
Gong NW, Lu MY, Wang CY, Chen Y, Chen L (2008) Au (Si)-filled β-Ga2O3 nanotubes as wide range high temperature nanothermometers. J Applied Physics Letters 92:073101
Tian B, Xie P, Kempa TJ, Bell DC, Lieber CM (2009) Single-crystalline kinked semiconductor nanowire superstructures. Nat Nanotechnol 4:824–829
Jiang N, Parkinson P, Gao Q, Breuer S, Tan HH, Wong-Leung J, Jagadish C (2012) Long minority carrier lifetime in Au-Catalyzed GaAs/AlxGa1-xAs core-shell nanowires. Appl Phys Lett 101:023111
Fortuna SA, Wen J, Chun IS, Li X (2008) Planar GaAs nanowires on GaAs (100) substrates: self-aligned, nearly twin-defect free, and transfer-printable. Nano Lett 8:4421–4427
Ihn SG, Song JI, Kim TW, Leem DS, Lee T, Lee SG, Koh EK, Song K (2007) Morphology- and orientation-controlled gallium arsenide nanowires on silicon substrates. Nano Lett 7:39–44
Mårtensson T, Svensson CPT, Wacaser BA, Larsson MW, Seifert W, Deppert K, Gustafsson A, Wallenberg LR, Samuelson L (2004) Epitaxial III−V nanowires on silicon. Nano Lett 4:1987–1990
Plante MC, LaPierre RR (2006) Growth Mechanisms of GaAs Nanowires by Gas Source Molecular Beam Epitaxy. J Crystal Growth 286:394–399
Chou YC, Wu WW, Chen LJ, Tu KN (2009) Homogeneous Nucleation of Epitaxial CoSi2 and NiSi in Si Nanowires. Nano Lett 9:2337–2342
Chou YC, Wu WW, Cheng SL, Yoo BY, Myung N, Chen LJ, Tu KN (2008) In-situ TEM Observation of Repeating Events of Nucleation in Epitaxial Growth of Nano CoSi2 in Nanowires of Si. Nano Lett 8:2194–2199
The research was supported by the Ministry of Science and Technology through Grant Nos. MOST 103-2218-E-011-007-MY3, MOST 105 - 2221 - E - 492 - 030 - MY2 and MOST 104-2112-M-007-011-MY3.
CYW, YCH, and ZJK performed the experiments, analyzed the results, and wrote the manuscript. CYW, YCH, and ZJK participated in the sample fabrication and characterizations. CYW, YWS, and JHH contributed to the data interpretation, manuscript writing, and supervised the research. All authors read and approved the final version of the manuscript.
The authors declare that they have no competing interests.
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