Chem. J. Chinese Universities ›› 2016, Vol. 37 ›› Issue (6): 1108.doi: 10.7503/cjcu20160100
• Physical Chemistry • Previous Articles Next Articles
ZHANG Chao, PAN Chengling*(), SHENG Shaoding
Received:
2016-02-17
Online:
2016-06-10
Published:
2016-05-26
Contact:
PAN Chengling
E-mail:chengling_pan@126.com
Supported by:
CLC Number:
TrendMD:
ZHANG Chao, PAN Chengling, SHENG Shaoding. Study on the Penetrating Energy of Zigzag Single-walled Carbon Nanotubes†[J]. Chem. J. Chinese Universities, 2016, 37(6): 1108.
Index | Diameter/nm | Number | Length/nm |
---|---|---|---|
(5,0) | 0.39 | 120 | 2.60 |
(7,0) | 0.55 | 168 | 2.60 |
(9,0) | 0.71 | 216 | 2.60 |
(11,0) | 0.86 | 264 | 2.60 |
(13,0) | 1.02 | 312 | 2.60 |
(15,0) | 1.17 | 360 | 2.60 |
(17,0) | 1.33 | 408 | 2.60 |
(19,0) | 1.49 | 456 | 2.60 |
Table 1 Parameters of carbon nanotubes
Index | Diameter/nm | Number | Length/nm |
---|---|---|---|
(5,0) | 0.39 | 120 | 2.60 |
(7,0) | 0.55 | 168 | 2.60 |
(9,0) | 0.71 | 216 | 2.60 |
(11,0) | 0.86 | 264 | 2.60 |
(13,0) | 1.02 | 312 | 2.60 |
(15,0) | 1.17 | 360 | 2.60 |
(17,0) | 1.33 | 408 | 2.60 |
(19,0) | 1.49 | 456 | 2.60 |
Parameter | Two-body | Parameter | Three-body |
---|---|---|---|
q1 | 10.149804 | Z/eV | 20.0 |
q2/nm-1 | 79.36986 | h | 0.205 |
q3/eV | 261.527033 | p | 1.34 |
q4/nm-1 | 5.27263 | b/nm-1 | 5.88 |
q5/nm | 0.3071221 |
Table 2 Parameters of the THTL potential[23]
Parameter | Two-body | Parameter | Three-body |
---|---|---|---|
q1 | 10.149804 | Z/eV | 20.0 |
q2/nm-1 | 79.36986 | h | 0.205 |
q3/eV | 261.527033 | p | 1.34 |
q4/nm-1 | 5.27263 | b/nm-1 | 5.88 |
q5/nm | 0.3071221 |
Fig.2 Time evolutions of the kinetic energies of the projectile(EPk, a), the PKA(EkPKA, b) and the SKA(EkSKA, c) for the(8,0) single-walled CNT at the incident energy of 1 keV
Fig.4 Atomic processes(A1—D1) and corresponding to the charge density distributions(A2—D2) at the incident energy of 40.0 eV t/fs: (A1, B1) 50; (A2, B2) 65; (C1, C2) 74; (D1, D2) 82.
Fig.5 Penetrating energy(EptPKA) as a function of the Ein for the (2n+1,0)(n=2—9) single-walled carbon nanotubesInsert shows the static penetrating energy(Ept0PKA) and the slope of the linear curve as functions of nanotube diameter. a. n=2; b. n=3; c. n=4; d. n=5; e. n=6; f. n=7; g. n=8; h. n=9.
Fig.6 Time evolutions of the potential energies of PKA(EpPKA) for incident energies ranging from 40.0 eV to 100.0 eVEin/eV: a. 40; b. 50; c. 60; d. 70; e. 80; f. 90; g. 100. The solid triangles and the solid dots indicate the extreme points of the potential energy of PKA, which are attributed to the collisions of the incident ions and the interactions between the PKA and the atoms on the rear wall, respectively. Insert shows the time evolutions EkPKA(h) and EpPKA(i) of the PKA, and the distance(j) between the incident carbon ion and the PKA at the incident energy of 40.0 eV, respectively.
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