2015
DOI: 10.1615/telecomradeng.v74.i15.20
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Mutual Influence of Carbon Nanotubes

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Cited by 2 publications
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“…Though the choice of the values I 1,2 is limited only by an equality I 1 − I 2 = I t , it is reasonable to choose them to be close to zero in order to guarantee the longitudinal character of the field Π t in the vicinity of the CNTs. For simplicity we choose I 1 = I t and I 2 = 0 for j 1a in (24). Thus, the electric field produced by the charges +q t and q t in the CNTs can be replaced by the field produced by the currents j 1a and j 2a , respectively, as shown in Fig.…”
Section: Discussionmentioning
confidence: 99%
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“…Though the choice of the values I 1,2 is limited only by an equality I 1 − I 2 = I t , it is reasonable to choose them to be close to zero in order to guarantee the longitudinal character of the field Π t in the vicinity of the CNTs. For simplicity we choose I 1 = I t and I 2 = 0 for j 1a in (24). Thus, the electric field produced by the charges +q t and q t in the CNTs can be replaced by the field produced by the currents j 1a and j 2a , respectively, as shown in Fig.…”
Section: Discussionmentioning
confidence: 99%
“…The second component of the intertube voltage U 2 can be found in the same way from the field induced by j 2 and j 2a . Thus, the impact of the tunneling current on the current in the tubes could be taken into account by means of the boundary conditions (2) and ( 5) and introduction of the extra currents (24) and (25).…”
Section: Hallén Type Equationmentioning
confidence: 99%
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