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. 2018 Apr 13;8:5945. doi: 10.1038/s41598-018-24343-w

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© The Author(s) 2018

Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/.

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(a) The relation of the linear velocity of circular motion and laser power at a field frequency of 2 kHz and field voltage of 1.5 Vpp. Inset: The trajectories of the circular motion in the co-field direction, the radiuses of which are linearly proportional to laser power. The time interval of each point is 0.07 s. (b) The relation of the angular velocity of circular motion and laser power, which is independent of laser power. (c) The relation of the linear velocity of circular motion and voltage at a field frequency of 2 kHz and with a laser irradiation of 360 mW. (d) The relation of the angular velocity of circular motion and voltage, which is proportional to the square of voltage.