Honda Research Institute USA Inc. , Columbus, Ohio 43212, United States.
Department of Physics, The Pennsylvania State University , University Park, Pennsylvania 16801, United States.
ACS Nano. 2017 Oct 24;11(10):9941-9949. doi: 10.1021/acsnano.7b03957. Epub 2017 Oct 2.
Elucidating the origin of carbon nanotube chirality is key for realizing their untapped potential. Currently, prevalent theories suggest that catalyst structure originates chirality via an epitaxial relationship. Here we studied chirality abundances of carbon nanotubes grown on floating liquid Ga droplets, which excludes the influence of catalyst features, and compared them with abundances grown on solid Ru nanoparticles. Results of growth on liquid droplets bolsters the intrinsic preference of carbon nuclei toward certain chiralities. Specifically, the abundance of the (11,1)/χ = 4.31° tube can reach up to 95% relative to (9,4)/χ = 17.48°, although they have exactly the same diameter, (9.156 Å). However, the comparative abundances for the pair, (19,3)/χ = 7.2° and (17,6)/χ = 14.5°, with bigger diameter, (16.405 Å), fluctuate depending on synthesis temperature. The abundances of the same pairs of tubes grown on floating solid polyhedral Ru nanoparticles show completely different trends. Analysis of abundances in relation to nucleation probability, represented by a product of the Zeldovich factor and the deviation interval of a growing nuclei from equilibrium critical size, explain the findings. We suggest that the chirality in the nanotube in general is a result of interplay between intrinsic preference of carbon cluster and induction by catalyst structure. This finding can help to build the comprehensive theory of nanotube growth and offers a prospect for chirality-preferential synthesis of carbon nanotubes by the exploitation of liquid catalyst droplets.
阐明碳纳米管手性的起源对于实现其未开发的潜力至关重要。目前,流行的理论认为,催化剂结构通过外延关系产生手性。在这里,我们研究了在悬浮的液态 Ga 液滴上生长的碳纳米管的手性丰度,这排除了催化剂特征的影响,并将其与在固态 Ru 纳米颗粒上生长的手性丰度进行了比较。在液滴上生长的结果支持了碳核对手性的固有偏好。具体来说,(11,1)/χ = 4.31°管的丰度相对于(9,4)/χ = 17.48°管可以达到 95%,尽管它们具有完全相同的直径,(9.156 Å)。然而,对于直径较大的(19,3)/χ = 7.2°和(17,6)/χ = 14.5°管对,其相对丰度则取决于合成温度而波动。在悬浮的多面体 Ru 纳米颗粒上生长的相同管对的丰度表现出完全不同的趋势。通过 Zeldovich 因子与生长核偏离平衡临界尺寸的偏差间隔的乘积表示的成核概率分析,解释了这些发现。我们认为,纳米管的手性通常是碳簇的固有偏好与催化剂结构诱导之间相互作用的结果。这一发现有助于建立纳米管生长的综合理论,并为利用液态催化剂液滴实现碳纳米管的手性优先合成提供了前景。