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Optimizing Buffer Layers via Atomic Layer Deposition for High‑Performance Vertically Aligned Carbon Nanotube Arrays

Abstract

Vertically aligned carbon nanotube arrays (VACNTs) are key to next‑generation thermal interface materials (TIMs). While thermally oxidized SiO2 has traditionally served as a buffer layer, atomic layer deposition (ALD) offers a route to fabricate pinhole‑free, dense oxides such as Al2O3, TiO2, and ZnO prior to catalyst deposition. Our study shows that VACNT growth is highly sensitive to the buffer layer chemistry; Al2O3 delivers the thickest, densest arrays and predominantly triple‑walled tubes. Deposition temperature exerts a pronounced influence—growth rates peak below 650 °C and decline thereafter, likely due to Ostwald ripening and catalyst subsurface diffusion. Finally, we integrated the VACNTs with graphene in an epoxy matrix to create a composite film that demonstrates superior vertical (≈1.25 W m−1 K−1) and transverse (≈2.50 W m−1 K−1) thermal conductivities compared to bare epoxy. These results highlight the critical role of ALD‑grown buffer layers in tailoring VACNT properties for advanced heat‑management solutions.

Background

VACNTs possess extraordinary axial thermal conductivity and are increasingly employed in thermal packaging. High‑quality arrays are typically grown by chemical vapor deposition (CVD) on substrates pre‑coated with a buffer layer that prevents catalyst diffusion. Atomic layer deposition (ALD) delivers conformal, defect‑free oxides on complex geometries, making it an attractive choice for buffer layers. Prior work has demonstrated improved nucleation and uniform tube diameters when ALD‑grown Al2O3 or SiO2 are used as buffers, yet the mechanistic influence of different oxides on VACNT growth remains incompletely understood.

In this investigation, we systematically evaluate ALD‑deposited Al2O3, TiO2, ZnO, and thermally oxidized SiO2 as buffer layers for VACNT synthesis. We also develop a VACNT/graphene composite film for enhanced heat transfer, with VACNTs providing vertical pathways and graphene supplying transverse conduction.

Methods

Thin films of Al2O3, TiO2, and ZnO were deposited on Si wafers by ALD at 200 °C using TMA, TDMAT, and DEZ precursors with H2O as the oxidant, yielding 20 nm layers. SiO2 was grown thermally to the same thickness. A 1 nm Fe catalyst was then evaporated by electron‑beam onto all substrates. VACNT growth proceeded in a commercial CVD system (AIXRON Black Magic II): the catalyst was annealed in H2 (700 sccm) at 600 °C for 3 min; thereafter, C2H2 (100 sccm) and H2 (700 sccm) were introduced, and growth lasted 30 min at temperatures ranging from 550 to 700 °C.

For the composite film, patterned Fe catalysts (500 µm × 150 µm pitch) were deposited on Al2O3, VACNTs were grown at 650 °C for 30 min, then densified with acetone vapor for 20 s. Multilayer graphene (10 wt %) was mixed with epoxy resin, curing agent, and diluent, and the VACNTs were immersed and cured at 120 °C (1 h) followed by 150 °C (1 h). The resulting 300 µm film had protruding VACNT tips on both faces.

Morphology was examined by FESEM (Merlin Compact) and TEM (Tecnai G2 F20 S‑TWIN). Raman spectra (632.8 nm excitation) assessed tube structure. Thermal diffusivity and specific heat were measured by laser flash (Netzach LFA 467) and differential scanning calorimetry (DSC, Mettler Toledo DSC1), enabling calculation of thermal conductivity via λ = α × Cp × ρ.

Results and Discussion

Cross‑sectional SEM images (Fig. 2) reveal that VACNTs are successfully grown on Al2O3, TiO2, and SiO2, with the thickest, most densely packed arrays on Al2O3. In contrast, ZnO yields negligible VACNT growth, likely due to accelerated Ostwald ripening and Fe subsurface diffusion.

Raman analysis (Fig. 4) shows D, G, and G′ bands around 1360, 1580, and 2700 cm−1 respectively. The ID/IG ratios are ≥1 across all buffers, confirming multi‑walled tubes; TEM images (Fig. 5) confirm predominantly triple‑walled VACNTs on Al2O3 and ≥four‑walled tubes on TiO2, ZnO, and SiO2.

Growth rate versus temperature (Fig. 6) shows an initial increase followed by a decline above 650 °C for all buffers, with Al2O3 maintaining higher rates beyond 600 °C. This suggests a longer catalyst lifetime on Al2O3 and a lower activation energy for nucleation compared to SiO2.

The VACNT/graphene composite film exhibits enhanced thermal transport: vertical conductivity ≈1.25 W m−1 K−1 and transverse conductivity ≈2.50 W m−1 K−1 (Fig. 8). These values far exceed those of the epoxy matrix alone, confirming that VACNTs provide efficient vertical heat pathways while graphene augments lateral conduction.

Conclusions

ALD‑grown Al2O3 emerges as the optimal buffer layer for VACNT synthesis, delivering the thickest, densest, and best‑aligned arrays due to prolonged catalyst stability and lower nucleation barriers. Temperature control is critical, with growth rates peaking near 650 °C. Incorporating VACNTs onto graphene within an epoxy matrix yields a composite with markedly improved vertical and transverse thermal conductivities, underscoring the potential of this architecture for high‑performance thermal management.

Abbreviations

ALD:

Atomic layer deposition

C2H2:

Acetylene

CVD:

Chemical vapor deposition

DEZ:

Diethylzinc

DSC:

Differential scanning calorimeter

EB:

Electron‑beam

FESEM:

Field emission scanning electron microscopy

H2:

Hydrogen

LFA:

Laser flash thermal analyzer

RBMs:

Radial breathing modes

TDMAT:

Tetrakis(dimethylamino)titanium

TEM:

Transmission electron microscopy

TIMs:

Thermal interface materials

TMA:

Trimethylaluminum

VACNTs:

Vertically aligned carbon nanotubes

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