Channeling of fast ions through the bent carbon nanotubes: The extended two-fluid hydrodynamic model
Karbunar Lazar1, †, , Borka Duško2, ‡, , Radović Ivan2, §, , Mišković Zoran L3, ¶,
       

Dependences of the image potential Uim calculated from the extended two-fluid model (dotted curve), repulsive potential Ur (dashed curve), and the resulting total potential Ut (solid curve) on proton position y from the center of a straight nanotube in the cases of (a) (6,4) SWNT, (b) (8,6) SWNT, (c) (11,9) SWNT, and (d) (15,10) SWNT. Also shown are the results for the total potential Ut1f calculated with Uim from the one-fluid model with zero damping (dash-dotted curve). The proton velocity is v = 3 a.u. Vertical solid bars represent the positions of nanotube walls. The values of nanotube radius R are 0.346, 0.483, 0.689, and 0.865 nm for the (6,4), (8,6), (11,9), and (15,10) SWNTs, respectively. Vertical dotted bars refer to the value Rasc for each nanotube, where asc is the nanotube atom screening radius.