The combined effect of 13C isotope doping and vacancies on the phonon properties of a single-wall carbon nanotube is theoretically investigated using the forced oscillation method. The phonon density of states (PDOS) is calculated for all (0%–100%) 13C isotope contents and wide (0%–30%) vacancy concentrations. We found a redshift of the Raman active E2g peak in the PDOS with increasing isotope contents, while the disappearance of the E2g peak and the appearance of a new sharp peak in the low-energy region with increasing combined defects. Both 13C isotope and combined defects cause the localization of the high-energy optical phonons. We calculated the typical mode patterns for the in-plane longitudinal optical phonon to visualize the localization phenomena elaborately at the presence of isotope and vacancies. The calculated average localization length shows an asymmetric behavior with increasing 13C isotope concentrations which is in good agreement with the 13C isotope dependence localization length of single-layer graphene. We noticed that a typical localization length is on the order of ∼1 nm at 70% isotope concentrations. The combined effect of 13C isotope and vacancies shows an abruptly decreasing localization length with increasing defect densities. These results are important to understand the heat conduction as well as nanoscopic vibrational studies such as tip-enhanced Raman spectra in carbon nanotubes where the local phonon energies may be mapped.
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28 July 2020
Research Article|
July 24 2020
Phonon localization in single wall carbon nanotube: Combined effect of 13C isotope and vacancies
Special Collection:
Physics and Applications of Nanotubes
Md. Sherajul Islam
;
Md. Sherajul Islam
a)
1
Department of Electrical and Electronic Engineering, Khulna University of Engineering & Technology
, Khulna 9203, Bangladesh
a)Authors to whom correspondence should be addressed: sheraj_kuet@eee.kuet.ac.bd and ashraful.howlader@sydney.edu.au
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Ashraful Hossain Howlader
;
Ashraful Hossain Howlader
a)
2
School of Physics, The University of Sydney
, Sydney, NSW 2006, Australia
a)Authors to whom correspondence should be addressed: sheraj_kuet@eee.kuet.ac.bd and ashraful.howlader@sydney.edu.au
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Khalid N. Anindya
;
Khalid N. Anindya
3
Département de génie physique and Regroupement québécois sur les matériaux de pointe (RQMP), Polytechnique Montréal
, Montréal, Québec H3C 3A7, Canada
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Rongkun Zheng
;
Rongkun Zheng
2
School of Physics, The University of Sydney
, Sydney, NSW 2006, Australia
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Jeongwon Park
;
Jeongwon Park
4
School of Electrical Engineering and Computer Science, University of Ottawa
, Ottawa, Ontario K1N 6N5, Canada
5
Department of Electrical and Biomedical Engineering, University of Nevada
, Reno, Nevada 89557, USA
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Akihiro Hashimoto
Akihiro Hashimoto
6
Graduate School of Engineering, University of Fukui
, Fukui 910-8507, Japan
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a)Authors to whom correspondence should be addressed: sheraj_kuet@eee.kuet.ac.bd and ashraful.howlader@sydney.edu.au
Note: This paper is part of the Special Topic on Physics and Applications of Nanotubes
J. Appl. Phys. 128, 045108 (2020)
Article history
Received:
April 24 2020
Accepted:
July 09 2020
Citation
Md. Sherajul Islam, Ashraful Hossain Howlader, Khalid N. Anindya, Rongkun Zheng, Jeongwon Park, Akihiro Hashimoto; Phonon localization in single wall carbon nanotube: Combined effect of 13C isotope and vacancies. J. Appl. Phys. 28 July 2020; 128 (4): 045108. https://doi.org/10.1063/5.0011810
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