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Development of a fully automated desktop chemical vapor deposition system for programmable and controlled carbon nanotube growth

Abstract

We have rationally designed and developed a fully automated desktop furnace system that enables programmable chemical vapour deposition growth of carbon nanotubes with controlled height, density, and pattern architecture. Comprising several essential components involving a heating furnace, mass flowmeters, and computer controller, the developed system realizes controlled and practical carbon nanotube growth without resort to expensive and ponderous instruments. By programming, modifying, and loading the reusable recipes in the developed system, systematic and reproducible growths of carbon nanotubes with desired morphology and dimension can be performed. Growth results with controlled height, density, and pattern are demonstrated through the actual operations, confirming the validity and usefulness of the developed system towards various practical applications.

Introduction

Since discovered almost two decades ago [1], carbon nanotubes (CNTs) have been extensively utilized in many diverse functional components and practical applications due to their extraordinary mechanical, electrical, chemical, and photonic characteristics [2,3,4]. To meet the unbounded needs in both academia and industry, reliable and rational manufacturing of CNTs with controlled density, desired length and diameter, and high quality has always been of great importance. Among several methods involving arc discharge and laser ablation, chemical vapour deposition (CVD) has played a central role in controlled CNT growth [5,6,7,8]. The CVD-based CNT growth method possesses many advantages compared to the other methods. It can generally provide highly crystalline, low-defect CNTs with good uniformity and reproducibility. It can lead to more scalable growth of CNTs well-bound to large area substrates, which can be more easily engineered, transferred, or harvested for subsequent uses. It also can readily control the density, alignment degree, length, and diameter of CNTs, based on the modulation of several CVD processing parameters such as gas composition and flow rate, temperature, and growth time. Additionally, CVD growth enables facile fabrication of CNT micro- and nanostructures by selective growth on the patterned catalyst.

However, the typical CVD system demands complex instrumentation and ponderous vacuum apparatus with numerous components most of which are not frequently used but costly. This restricts the otherwise much wider research and more practical development utilizing CNTs. As described in detail in our previous reports that our developed growth ‘recipe’ is based on the atmospheric pressure (AP) CVD [9], the CVD system for CNT growth does not necessitate complicated vacuum processing. Hence, what we essentially need may include the heating furnace, source gas feeder, and their controller. To this end, we develop a compact, desktop-scale CVD growth system comprising essential components with much reduced cost and volume, but effectively working for reliable and programmable CNT growth through the computer-controlled fully automated operation. In this work, we present the rational design and setup of the system, and demonstrate CNT growth results with controlled height, density, and alignment, as well as the specific micro- and nanopatterned architectures by operating the completed system with recipe modulations.

Process overview and system requirement

The APCVD process for CNT growth is briefly as follows. First, the catalyst layers comprising Fe on Al2O3 with nominal thicknesses of 1 nm and 10 nm, respectively, are sequentially deposited on a 300 nm-thick SiO2-coated Si wafer. Cut to the fit size, the catalyst pieces are loaded inside the CVD chamber at proper temperature gradient positions. After ample Ar purging, the chamber is heated up to the peak temperature (~ 800 °C) at a proper ramp rate under Ar/H2 flowing. Dwelled at the peak temperature for catalyst annealing (mostly H2-driven reduction) for a while, C2H4 is then added as a carbon source for CNT growth. Once growth is done, the chamber is cooled down to room temperature under slight Ar flowing. Between runs, air baking is performed at around 800 °C for 30 min to clean the chamber by removing the inside carbon-based residues. The quantitative values of the gas flow composition, temperature ramp rate, peak temperature, time period for each step, and so on, can be tuned for optimizing the growth results, which will be discussed later.

In this regard, the CVD system may be designed to carry out the above-described process with precise controls of such parameters without excessive parts. Namely, the essential components of the system may consist of the heating chamber, four mass flow controller (MFC) channels designated for Ar, H2, C2H4, and air, and the computer controller, along with surrounding plumbing and wiring.

System design and setup: hardware and software

Figure 1 illustrates the overall system design that can perform the necessary processes under computer control. First, we employed the 1″-diameter single-zone tube furnace that can heat up to 1200 °C equipped with RS-232/485 serial communication ports (TF55035C-1, Lindberg/Blue M™ Mini-Mite™, Thermo Fisher Scientific, Ltd.), to use as a computer-controllable heating chamber (Fig. 2a). An 1″-diamter quartz tube was assembled with the O ring-sealed stainless steel endcaps having the plumbing holes, and was mounted inside the tube furnace. Next, we designed and setup the MFC box (Fig. 2b; Sci-En Tech Corp.) comprising four MFC channels (AFC 500/600 series, ATOVAC Co., Ltd.) and their integrated throttle valve controller with a display monitor (GMC 1200, ATOVAC Co., Ltd.). Four MFCs were respectively connected to the designated gas tanks (as depicted in Fig. 1) through the stainless steel pipes and safety/regulator valves. The MFC box outlet was made by merging individual MFC outlets. Here to avoid dangerous flowing of H2 and air at the same time, a three-way valve was connected between H2 and air channels; either H2 or air could flow at a certain time, not ever simultaneously. The chamber inlet endcap hole and MFC box outlet valve were connected to each other by using a flexible stainless steel hose (Swagelok Company). The chamber outlet endcap hole was connected to the vent through the glycerine-filled bubbler that can prevent possible backflow, by using flexible Tygon® tubes (Saint Gobain Corp.). Finally, the furnace and MFC valve controller were wired to the computer via RS-485 and RS-232 communication cables, respectively.

Fig. 1
figure 1

Schematic diagram of the computer-controlled fully automated compact CVD system for CNT growth, consisting of the furnace, 4-channel MFC box, and controller. Serial communications between hardware components enable reliable and reproducible operation. Valves and anti-backflow bubbler ensure safety

Fig. 2
figure 2

Photographs of the main hardware and software components comprising the desktop CVD system for controlled CNT growths: a 1″-diameter tube furnace equipped with a serial-communicable temperature control module, b completed MFC box assembly containing four MFC channels (upper part) and their throttle valve controller (lower part), and c screenshot of the front panel of a CVD system-controlling LabVIEW software. The left side shows step-wise setting lines for temperatures, gas flows, and step period times, and the right side displays the real-time traces of such parameters during the process operation

The controlling software was designed and developed by using LabVIEW (version 2017, National Instruments Corp.), for the automated and reliable operations of the furnace and MFCs. Step-wise settings of temperatures, gas flow rates, and step period times can be put in the left side of the software’s front panel shown in Fig. 2c, which transmit to and operate the furnace and MFC box via serial communications. The furnace temperature and gas flow rates can be real-time tracked in the right side monitor with the elapsed time as an x-axis. The sensors installed in the furnace and MFC box, in conjunction with the LabVIEW monitor enable the feedback control of temperature and gas flows to maintain the set values with minimal disturbances. Temperature ramp and dwell can also be straightforwardly programmed in this software panel; if the temperature different from the previous step is set, the furnace ramps up or down during the set period time; if the same temperature is set as the previous step, the furnace temperature dwells during the set period time. Further, we added the “preset” function; the set values of temperatures, gas flow rates, and step period times for all step lines can be saved as an ASCII text file, and this file can be reloaded later for repeated uses (as a “recipe”). This “Export and Import” function can facilitate the recipe development and management for various CNT growth conditions.

System operation results: controlled carbon nanotube growth

As aforementioned, the system design and setup have been implemented with a focus on the compact volume and affordable cost. Figure 3a shows the completed CVD system. The system volume was cut down to ~ 15% of the commercial CVD system (comparatively shown in Fig. 3b), and indeed could be put on the desktop with a minimal space. Meanwhile, the total expense was ~ 78% saved (from USD 55,000 to 12,500, approximately). While such a successful reduction in both volume and cost is mostly attributed to the curtail of vacuum-related and other uncritical components so far, we now evaluate the key function of the system, that is programmable, reliable, and practical CNT growth, by actual operations.

Fig. 3
figure 3

Completed CVD system in comparison to a commercially-available one and the developed standard recipe: a our developed desktop CVD, b commercial CVD, and c standard recipe for CNT growth in the completed CVD system

Figure 3c demonstrates one of the recipes we have investigated for optimal CNT growth using the developed compact CVD system, where the prime parameters involving temperature, gas flow composition and rates, and times for each step for CNT growth are fully marked in detail. These recipes can be loaded, modified, saved, and reloaded in the LabVIEW controller for repeated controlled growths. Figure 4 shows the exemplary growth results obtained by using the recipe shown in Fig. 3c. The high-density CNTs (i.e., CNT “forest”) were uniformly grown on the catalyst substrates with up to a millimetre-scale height (Fig. 4a) and/or over the large area (Fig. 4b), confirming reliable and effective CNT growth. Figure 4c reveals typical nanoscale morphology of the as-grown CNT forests, with the average diameter and interspacing range of 10 nm and 50–100 nm, respectively. The growth height can be controlled mainly by the growth time (time of C2H4 flowing, as shown in Fig. 3c); Fig. 4d–f disclose three different examples with different heights, obtained by different growth times.

Fig. 4
figure 4

CNT forests grown in the developed CVD system: a and b photographs of exemplary samples, c nanoscale morphology of the sidewalls of as-grown CNTs (inset shows the top view), df CNT forests with different heights controlled by growth time

Controlled growth of CNTs having specific density along with various alignment degree can also be readily conducted by modulation of recipe parameters. The density control can be induced by many means such as feed gas regulation [10, 11] and catalyst patterning [12,13,14], but here we demonstrate one strategy for density control based on the modulation of annealing time (i.e., time of Ar/H2 flowing at the peak temperature, as marked in Fig. 3c) [15]. Figure 5 shows three cases of CNTs having different areal densities grown by varying the annealing time; annealing times were controlled to 5 min, 10 min, and 20 min for cases 1, 2, and 3, respectively. Insets to the left-side top images in Fig. 5, taken from the ‘blank’ runs (i.e., recipe runs with no C2H4 flowing), reveal the morphologies of annealed catalysts for each case. From the right-side sidewall images of Fig. 5, we can find that CNTs are better aligned with increased density at shorter annealing time in our experimental space; even shorter annealing time may end up with insufficient catalyst annealing. During the annealing step, the thin Fe catalyst film is clustered to nanoscale particles on the Al2O3 layer. The longer the annealing time is (case 3), the Fe nanocluster size becomes larger while the number of clusters decreases as agglomerated together [15]. This leads to low-density, vertically less-aligned CNTs. On the other hand, when grown from the catalyst nanoclusters with higher density (case 1), the resulting CNT density becomes higher [16]. In this case, CNTs may grow more upright, as the interspaces between neighbouring CNTs get smaller (i.e., “crowding effect”) [17].

Fig. 5
figure 5

Three cases of CNTs having different areal densities and alignments grown by varying annealing times: The annealing times were set for a 5 min, b 10 min, and c 20 min. Left and right images show the top and sidewall SEM images of each case, respectively. Insets show the catalyst morphologies taken from blank runs for each case

Finally, we demonstrate that the system enables the direct growth of CNT architectures comprising specifically designed micro- and nanoscale patterns, through selective CNT growth on patterned catalysts. The catalyst layers can be patterned by suitable methods such as photolithography [18] and nanoimprint lithography [13]. The recipe modification can be performed to optimize the selective growth of CNT patterns, usually by controls of annealing time and C2H4 flow rate. Such micro- and nanoarchitectures with specifically designed CNT structures can be capitalized in many devices involving mechanics, photonics, metastructures, sensors, and energy converters [3, 19], as well as provide the templates for growing other complimentary nanomaterials towards more functional hybrid architectures [9, 18]. While further investigation on the systematic fabrications of diverse application-specific CNT architectures is underway for the following report, Fig. 6 shows several examples of the patterned CNT growths, confirming that the developed CVD system achieves reliable and practical CNT architecture fabrication.

Fig. 6
figure 6

Fabrication examples of CNT architectures comprising micro- and nanoscale patterns by using the developed CVD system: a and b CNT micropillar arrays with various diameters and c and d microsheet patterns

Conclusions

In summary, we have developed a computer-controlled compact CVD system that enables programmable growths of CNTs with desired height, density, and pattern architecture. Rational system design and setup of essential components involving a heating furnace, MFCs, and computer controller, realize the fully automated desktop-scale system with significantly reduced volume and cost, compared to commercial CVD instruments. We have demonstrated that the controlled CNT growth with desired morphology and dimension could be conducted by programming, modifying, and loading the reusable recipes in the developed system. This study will facilitate practical developments of many applications utilizing CNTs and their derivative architectures such as CNT thin films, coatings, and micro- and nanoarchitectures.

Availability of data and materials

All data generated or analysed during this study are included in the article.

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Acknowledgements

We thank Bo Kyung Kim for assistance with SEM imaging and the National NanoFab Center (NNFC) for assistance with microfabrication.

Funding

This work was supported by the Research Program funded by the Seoul National University of Science and Technology (Grant Number 2018-0788).

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JGO conceived, designed, and supervised the research. All authors contributed to experiments, characterizations, data analyses, and manuscript preparation. All authors read and approved the final manuscript.

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Correspondence to Jong G. Ok.

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Ahn, J.H., Na, M., Koo, S. et al. Development of a fully automated desktop chemical vapor deposition system for programmable and controlled carbon nanotube growth. Micro and Nano Syst Lett 7, 11 (2019). https://doi.org/10.1186/s40486-019-0091-8

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