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Volumn 81, Issue 1, 2002, Pages 46-48

Electronic and field emission properties of boron nitride/carbon nanotube superlattices

Author keywords

[No Author keywords available]

Indexed keywords

AB INITIO CALCULATIONS; BAND-OFFSET; FIELD EMISSION PROPERTY; FIELD EMITTER; NANO DEVICE; ORDERS OF MAGNITUDE; QUASI-ONE-DIMENSIONAL;

EID: 79955982800     PISSN: 00036951     EISSN: None     Source Type: Journal    
DOI: 10.1063/1.1491013     Document Type: Article
Times cited : (64)

References (26)
  • 8
    • 79958219488 scopus 로고    scopus 로고
    • E. J. Mele, P. Král, and D. Tomanek, http://www.aps.org/meet/ MAR01/baps/abs/S8658005.html;
    • Mele, E.J.1
  • 9
    • 4244101016 scopus 로고    scopus 로고
    • prl PRLTAO 0031-9007
    • Phys. Rev. Lett. 88, 056803 (2002). prl PRLTAO 0031-9007
    • (2002) Phys. Rev. Lett. , vol.88 , pp. 056803
  • 11
    • 79958220135 scopus 로고    scopus 로고
    • S. Nakhmanson, V. Meunier, J. Bernholc, and M. Buongiorno Nardelli (unpublished)
    • S. Nakhmanson, V. Meunier, J. Bernholc, and M. Buongiorno Nardelli (unpublished).
  • 12
    • 0000328286 scopus 로고
    • The ab initio calculations were carried out via a combination of standard multigrid-based real-space [, and, ; prb PRBMDO 0163-1829
    • The ab initio calculations were carried out via a combination of standard multigrid-based real-space [ E. L. Briggs, D. J. Sullivan, and J. Bernhole, Phys. Rev. B 52, R5471 (1995); prb PRBMDO 0163-1829
    • (1995) Phys. Rev. B , vol.52 , pp. 5471
    • Briggs, E.L.1    Sullivan, D.J.2    Bernhole, J.3
  • 13
    • 79958241353 scopus 로고    scopus 로고
    • 54, 14362 and plane-wave methods After a careful minimization of the atomic coordinates, the structural parameters and electronic band structures obtained were in perfect agreement with those of previous calculations (see Ref. 7)
    • 54, 14362 (1996)] and plane-wave methods [S. Baroni et al., http://www.pwscf.org]. After a careful minimization of the atomic coordinates, the structural parameters and electronic band structures obtained were in perfect agreement with those of previous calculations (see Ref. 7).
    • (1996)
    • Baroni, S.1
  • 14
    • 79958204204 scopus 로고    scopus 로고
    • In contrast to three-dimensional solids, the asymptotic band offsets of such heterojunctions are conveniently computed from the bulk properties of their isolated components, since the vacuum level (i.e., the ionization potential) may be used as an unequivocal reference energy [R. Resta (private communication)
    • In contrast to three-dimensional solids, the asymptotic band offsets of such heterojunctions are conveniently computed from the bulk properties of their isolated components, since the vacuum level (i.e., the ionization potential) may be used as an unequivocal reference energy [R. Resta (private communication);
  • 15
    • 0001433702 scopus 로고
    • see also, ]. prb PRBMDO 0163-1829
    • see also L. Kleinman, Phys. Rev. B 24, 7412 (1981)]. prb PRBMDO 0163-1829
    • (1981) Phys. Rev. B , vol.24 , pp. 7412
    • Kleinman, L.1
  • 17
    • 79958242001 scopus 로고    scopus 로고
    • In 1D systems, the volume of the cell is not relevant to the evaluation of averages and for that reason we have defined the effective volume as being the one in which 99% of the total charge is located (see Ref. 9)
    • In 1D systems, the volume of the cell is not relevant to the evaluation of averages and for that reason we have defined the effective volume as being the one in which 99% of the total charge is located (see Ref. 9).
  • 19
    • 0000584883 scopus 로고    scopus 로고
    • prb PRBMDO 0163-1829
    • C. L. Kane and E. J. Mele, Phys. Rev. B 59, R12759 (1999). prb PRBMDO 0163-1829
    • (1999) Phys. Rev. B , vol.59 , pp. 12759
    • Kane, C.L.1    Mele, E.J.2
  • 21
    • 0005311621 scopus 로고    scopus 로고
    • prb PRBMDO 0163-1829
    • S. Han and J. Ihm, Phys. Rev. B 61, 9986 (2000). prb PRBMDO 0163-1829
    • (2000) Phys. Rev. B , vol.61 , pp. 9986
    • Han, S.1    Ihm, J.2
  • 24
    • 0001048838 scopus 로고    scopus 로고
    • We used the so-called dipole correction in order to avoid nondesirable supercell effects and to ensure the flatness of the electrostatic potential in the vacuum [, ]. prb PRBMDO 0163-1829
    • We used the so-called dipole correction in order to avoid nondesirable supercell effects and to ensure the flatness of the electrostatic potential in the vacuum [ L. Bengtsson, Phys. Rev. B 59, 12301 (1999)]. prb PRBMDO 0163-1829
    • (1999) Phys. Rev. B , vol.59 , pp. 12301
    • Bengtsson, L.1
  • 25
    • 0034883236 scopus 로고    scopus 로고
    • car CRBNAH 0008-6223
    • M. Shiraishi and M. Ata, Carbon 39, 1913 (2001). car CRBNAH 0008-6223
    • (2001) Carbon , vol.39 , pp. 1913
    • Shiraishi, M.1    Ata, M.2


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.