2009
DOI: 10.1103/physrevb.80.165414
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Dispersion interactions between optically anisotropic cylinders at all separations: Retardation effects for insulating and semiconducting single-wall carbon nanotubes

Abstract: We derive the complete form of the van der Waals dispersion interaction between two infinitely long anisotropic semiconducting/insulating thin cylinders at all separations. The derivation is based on the general theory of dispersion interactions between anisotropic media as formulated in Munday et al. ͓Phys. Rev. A 71, 042102 ͑2005͔͒. This formulation is then used to calculate the dispersion interactions between a pair of single-walled carbon nanotubes at all separations and all angles. Nonretarded and retarde… Show more

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Cited by 30 publications
(45 citation statements)
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“…In some cases (not shown here), the dielectric responses of materials allow for a repulsive interaction, i.e., a negative Hamaker coefficient. 32,47 Consequently, this implies that torques also have a sign opposite to that of attractive interaction cases. If for illustration purposes we compare the symmetric system, (9; 3; m)-Al 2 O 3 -(9;3;m), with the asymmetric one, (9;3,m)-Al 2 O 3 -GC(10), 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60 14 we see that indeed the torque as well as the force change sign.…”
Section: Asymmetric Systemsmentioning
confidence: 86%
“…In some cases (not shown here), the dielectric responses of materials allow for a repulsive interaction, i.e., a negative Hamaker coefficient. 32,47 Consequently, this implies that torques also have a sign opposite to that of attractive interaction cases. If for illustration purposes we compare the symmetric system, (9; 3; m)-Al 2 O 3 -(9;3;m), with the asymmetric one, (9;3,m)-Al 2 O 3 -GC(10), 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60 14 we see that indeed the torque as well as the force change sign.…”
Section: Asymmetric Systemsmentioning
confidence: 86%
“…1(b)], and thus to a torque τ = −∂ θ E(z, θ) between the two structures, that is absent in the case of two flat homogeneous slabs. The existence and properties of this Casimir torque has been a topic of intense theoretical interest since the seventies [25][26][27][28][29][30][31][32][33][34][35][36][37][38][39][40][41][42], for both gratings and other symmetry-breaking systems. Due to the smallness of the effect, only very recently has the first measurement of this torque been realized [43].…”
mentioning
confidence: 99%
“…Such calculations have been successfully applied to many complex crystals 15,16 including carbon nanotubes. 17,18 Although there or more advanced theories in recent years for describing optical excitations in molecules and crystals such as time-dependent density-functional theory or the inclusion of excitonic effects based on many-body theory, they cannot yet be applied to large complex crystals such as herapathite. Figure 4 shows the calculated 2 ͑ប͒ up to 6 eV for the three components parallel to the a, b, and c axes of the crystal.…”
Section: Methods and Results Of Calculationmentioning
confidence: 99%
“…Ab initio calculation of optical spectra can provide such data which could potentially lead to quantitative evaluation of van der Waals forces 20 through the electrodynamic theory of Lizfshitz 21 as recently demonstrated in the carbon nanotube systems. 17,18 We believe that accurate optical spectral calculation for complex crystals and molecules can play a significant role in the understanding the long-range interactions at nanoscale. 22 …”
Section: Discussionmentioning
confidence: 99%