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Transport and optical properties of c-axis oriented wedge shaped GaN nanowall network grown by molecular beam epitaxy

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Transport and optical properties of c-axis oriented wedge shaped GaN nanowall network grown by molecular beam epitaxy. / Bhasker, H.P.; Thakur, Varun; Kesaria, Manoj et al.
In: AIP Conference Proceedings, Vol. 1583, 252, 2014.

Research output: Contribution to Journal/MagazineJournal articlepeer-review

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APA

Bhasker, H. P., Thakur, V., Kesaria, M., Shivaprasad, S. M., & Dhar, S. (2014). Transport and optical properties of c-axis oriented wedge shaped GaN nanowall network grown by molecular beam epitaxy. AIP Conference Proceedings, 1583, Article 252. https://doi.org/10.1063/1.4865647

Vancouver

Bhasker HP, Thakur V, Kesaria M, Shivaprasad SM, Dhar S. Transport and optical properties of c-axis oriented wedge shaped GaN nanowall network grown by molecular beam epitaxy. AIP Conference Proceedings. 2014;1583:252. doi: 10.1063/1.4865647

Author

Bhasker, H.P. ; Thakur, Varun ; Kesaria, Manoj et al. / Transport and optical properties of c-axis oriented wedge shaped GaN nanowall network grown by molecular beam epitaxy. In: AIP Conference Proceedings. 2014 ; Vol. 1583.

Bibtex

@article{2cde46df08c3462e91d10a5d1d1107e3,
title = "Transport and optical properties of c-axis oriented wedge shaped GaN nanowall network grown by molecular beam epitaxy",
abstract = "The transport and optical properties of wedge-shaped nanowall network of GaN grown spontaneously on cplane sapphire substrate by Plasma-Assisted Molecular Beam Epitaxy (PAMBE) show interesting behavior. The electron mobility at room temperature in these samples is found to be orders of magnitude higher than that of a continuous film. Our study reveals a strong correlation between the mobility and the band gap in these nanowall network samples. However, it is seen that when the thickness of the tips of the walls increases to an extent such that more than 70% of the film area is covered, it behaves close to a flat sample. In the sample with lower surface coverage (≈40% and ≈60%), it was observed that the conductivity, mobility as well as the band gap increase with the decrease in the average tip width of the walls. Photoluminescence (PL) experiments show a strong and broad band edge emission with a large (as high as ≈ 90 meV) blue shift, compared to that of a continuous film, suggesting a confinement of carriers on the top edges of the nanowalls. The PL peak width remains wide at all temperatures suggesting the existence of a high density of tail states at the band edge, which is further supported by the photoconductivity result. The high conductivity and mobility observed in these samples is believed to be due to a “dissipation less” transport of carriers, which are localized at the top edges (edge states) of the nanowalls.",
author = "H.P. Bhasker and Varun Thakur and Manoj Kesaria and S.M. Shivaprasad and S. Dhar",
year = "2014",
doi = "10.1063/1.4865647",
language = "English",
volume = "1583",
journal = "AIP Conference Proceedings",
issn = "0094-243X",
publisher = "American Institute of Physics Publising LLC",

}

RIS

TY - JOUR

T1 - Transport and optical properties of c-axis oriented wedge shaped GaN nanowall network grown by molecular beam epitaxy

AU - Bhasker, H.P.

AU - Thakur, Varun

AU - Kesaria, Manoj

AU - Shivaprasad, S.M.

AU - Dhar, S.

PY - 2014

Y1 - 2014

N2 - The transport and optical properties of wedge-shaped nanowall network of GaN grown spontaneously on cplane sapphire substrate by Plasma-Assisted Molecular Beam Epitaxy (PAMBE) show interesting behavior. The electron mobility at room temperature in these samples is found to be orders of magnitude higher than that of a continuous film. Our study reveals a strong correlation between the mobility and the band gap in these nanowall network samples. However, it is seen that when the thickness of the tips of the walls increases to an extent such that more than 70% of the film area is covered, it behaves close to a flat sample. In the sample with lower surface coverage (≈40% and ≈60%), it was observed that the conductivity, mobility as well as the band gap increase with the decrease in the average tip width of the walls. Photoluminescence (PL) experiments show a strong and broad band edge emission with a large (as high as ≈ 90 meV) blue shift, compared to that of a continuous film, suggesting a confinement of carriers on the top edges of the nanowalls. The PL peak width remains wide at all temperatures suggesting the existence of a high density of tail states at the band edge, which is further supported by the photoconductivity result. The high conductivity and mobility observed in these samples is believed to be due to a “dissipation less” transport of carriers, which are localized at the top edges (edge states) of the nanowalls.

AB - The transport and optical properties of wedge-shaped nanowall network of GaN grown spontaneously on cplane sapphire substrate by Plasma-Assisted Molecular Beam Epitaxy (PAMBE) show interesting behavior. The electron mobility at room temperature in these samples is found to be orders of magnitude higher than that of a continuous film. Our study reveals a strong correlation between the mobility and the band gap in these nanowall network samples. However, it is seen that when the thickness of the tips of the walls increases to an extent such that more than 70% of the film area is covered, it behaves close to a flat sample. In the sample with lower surface coverage (≈40% and ≈60%), it was observed that the conductivity, mobility as well as the band gap increase with the decrease in the average tip width of the walls. Photoluminescence (PL) experiments show a strong and broad band edge emission with a large (as high as ≈ 90 meV) blue shift, compared to that of a continuous film, suggesting a confinement of carriers on the top edges of the nanowalls. The PL peak width remains wide at all temperatures suggesting the existence of a high density of tail states at the band edge, which is further supported by the photoconductivity result. The high conductivity and mobility observed in these samples is believed to be due to a “dissipation less” transport of carriers, which are localized at the top edges (edge states) of the nanowalls.

U2 - 10.1063/1.4865647

DO - 10.1063/1.4865647

M3 - Journal article

VL - 1583

JO - AIP Conference Proceedings

JF - AIP Conference Proceedings

SN - 0094-243X

M1 - 252

ER -