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5
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0033591304
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Electromechanical effects have been recently used to manufacture nanoactuators and nanotweezers. See, R. H. Baughman, C. Cui, A. A. Zakhidov, Z. Iqbal, J. N. Barisci, G. M. sprinks, G. G. Wallace, A. Mazzoldi, D. De Rossi, A. G. Rinzler, O. Jaschinski, S. Roth, M. Kertesz, Science 284, 1340 (1999); P. Kim and C. M. Lieber, Ibid. 286, 2148 (1999).
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6
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0032787499
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Electromechanical effects have been recently used to manufacture nanoactuators and nanotweezers. See, R. H. Baughman, C. Cui, A. A. Zakhidov, Z. Iqbal, J. N. Barisci, G. M. sprinks, G. G. Wallace, A. Mazzoldi, D. De Rossi, A. G. Rinzler, O. Jaschinski, S. Roth, M. Kertesz, Science 284, 1340 (1999); P. Kim and C. M. Lieber, Ibid. 286, 2148 (1999).
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7
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3242735477
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note
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γ= 0.577216 is the Euler constant, and ψ(x)=d ln Γ(x)/dx is the digarnma function.
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9
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3242664974
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Details of the numerical method are explained in Ref. 8
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Details of the numerical method are explained in Ref. 8.
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11
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3242703823
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note
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If a conducting rod is held at a constant electrostatic potential, the charge distribution along the rod is known to be nearly uniform. The slight logarithmic buildup of charge at the ends of the rod leads to no significant change in the electrostatic energetics of the buckled rod; the conclusions reported in the body [Eq. (3) and the related discussions] are not materially affected.
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13
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3242721123
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Seoul, Korea, 21-26 May
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L. Dong, F. Arai, and T. Fukuda, Proceedings of the 2001 IEEE International Conference on Robotics & Automation, Seoul, Korea, 21-26 May, 2001; J. Robotics Mechatronics 14, 245 (2002).
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0345706831
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15
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3242685792
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note
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c≃420 V for L = 1 mm, which is a factor of 2 larger than the suggested applid voltage to ensure the length-independence of the critical buckling force.
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16
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0037122333
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P. Keblisnki, S. K. Nayak, P. Zapol, and P. M. Ajayan, Phys. Rev. Lett. 89, 255503-1 (2003).
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17
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0043268003
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A. M. Fennimore, T. D. Yuzvinsky, W. Q. Han, M. S. Fuhrer, J. Cumings, and A. Zettl, Nature (London) 424, 408 (2003).
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