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Two component doping of fullerene-cubane cocrystals

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Two component doping of fullerene-cubane cocrystals. / Kurti, Jeno; Koltai, Janos; Zolyomi, Viktor et al.
In: physica status solidi (b), Vol. 246, No. 11-12, 01.12.2009, p. 2618-2621.

Research output: Contribution to Journal/MagazineJournal articlepeer-review

Harvard

Kurti, J, Koltai, J, Zolyomi, V & Pekker, S 2009, 'Two component doping of fullerene-cubane cocrystals', physica status solidi (b), vol. 246, no. 11-12, pp. 2618-2621. https://doi.org/10.1002/pssb.200982332

APA

Kurti, J., Koltai, J., Zolyomi, V., & Pekker, S. (2009). Two component doping of fullerene-cubane cocrystals. physica status solidi (b), 246(11-12), 2618-2621. https://doi.org/10.1002/pssb.200982332

Vancouver

Kurti J, Koltai J, Zolyomi V, Pekker S. Two component doping of fullerene-cubane cocrystals. physica status solidi (b). 2009 Dec 1;246(11-12):2618-2621. doi: 10.1002/pssb.200982332

Author

Kurti, Jeno ; Koltai, Janos ; Zolyomi, Viktor et al. / Two component doping of fullerene-cubane cocrystals. In: physica status solidi (b). 2009 ; Vol. 246, No. 11-12. pp. 2618-2621.

Bibtex

@article{e672bdf26b2e439d91d39c539225844d,
title = "Two component doping of fullerene-cubane cocrystals",
abstract = "We present a first principles study of the electronic band structure of doped fullerene–cubane (C60C8H8) cocrystals using density functional theory at the local density approximation level. Three high symmetry orientations of the fullerene molecules were considered. The calculated electronic bands of the fullerene–cubane cocrystal are narrower than those of the pristine fullerene, indicating a possible higher superconducting critical temperature in the doped cocrystal. However, the charge transfer turned out to be incomplete thus acting in the opposite way. Different oxidation state of the fullerene molecules can be achieved by doping with various alkali (K, Na) and alkali earth (Ba, Ca) atoms. Depiction of the C60C8H8 cocrystal. The large green and orange orbs are the tetrahedral voids, which can in principle be filled with, for example, alkali or alkali earth atoms.",
author = "Jeno Kurti and Janos Koltai and Viktor Zolyomi and Sandor Pekker",
note = "23rd Winterschool on Electronic Properties of Novel Materials, Kirchberg, GERMANY, MAR 14, 2009",
year = "2009",
month = dec,
day = "1",
doi = "10.1002/pssb.200982332",
language = "English",
volume = "246",
pages = "2618--2621",
journal = "physica status solidi (b)",
issn = "0370-1972",
publisher = "Wiley-VCH Verlag",
number = "11-12",

}

RIS

TY - JOUR

T1 - Two component doping of fullerene-cubane cocrystals

AU - Kurti, Jeno

AU - Koltai, Janos

AU - Zolyomi, Viktor

AU - Pekker, Sandor

N1 - 23rd Winterschool on Electronic Properties of Novel Materials, Kirchberg, GERMANY, MAR 14, 2009

PY - 2009/12/1

Y1 - 2009/12/1

N2 - We present a first principles study of the electronic band structure of doped fullerene–cubane (C60C8H8) cocrystals using density functional theory at the local density approximation level. Three high symmetry orientations of the fullerene molecules were considered. The calculated electronic bands of the fullerene–cubane cocrystal are narrower than those of the pristine fullerene, indicating a possible higher superconducting critical temperature in the doped cocrystal. However, the charge transfer turned out to be incomplete thus acting in the opposite way. Different oxidation state of the fullerene molecules can be achieved by doping with various alkali (K, Na) and alkali earth (Ba, Ca) atoms. Depiction of the C60C8H8 cocrystal. The large green and orange orbs are the tetrahedral voids, which can in principle be filled with, for example, alkali or alkali earth atoms.

AB - We present a first principles study of the electronic band structure of doped fullerene–cubane (C60C8H8) cocrystals using density functional theory at the local density approximation level. Three high symmetry orientations of the fullerene molecules were considered. The calculated electronic bands of the fullerene–cubane cocrystal are narrower than those of the pristine fullerene, indicating a possible higher superconducting critical temperature in the doped cocrystal. However, the charge transfer turned out to be incomplete thus acting in the opposite way. Different oxidation state of the fullerene molecules can be achieved by doping with various alkali (K, Na) and alkali earth (Ba, Ca) atoms. Depiction of the C60C8H8 cocrystal. The large green and orange orbs are the tetrahedral voids, which can in principle be filled with, for example, alkali or alkali earth atoms.

U2 - 10.1002/pssb.200982332

DO - 10.1002/pssb.200982332

M3 - Journal article

VL - 246

SP - 2618

EP - 2621

JO - physica status solidi (b)

JF - physica status solidi (b)

SN - 0370-1972

IS - 11-12

ER -