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Volumn 65, Issue 23, 2002, Pages 1-12

Three-dimensional analysis of the electronic structure of cylindrical vertical quantum dots

Author keywords

[No Author keywords available]

Indexed keywords


EID: 85038324327     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.65.235323     Document Type: Article
Times cited : (1)

References (38)
  • 28
    • 85038342685 scopus 로고    scopus 로고
    • The agreement with 2D QMC simulations is very good up to (formula presented). However, for (formula presented), the QMC simulations (Refs. 12 and 13) give the singlet state (formula presented) as the lowest-energy state as opposed to the triplet state (formula presented) obtained in DFT, which is in agreement with experiments (Refs. 1234). This emphasizes the importance of the third dimension in realistically modeling the confining potential in the dot
    • The agreement with 2D QMC simulations is very good up to (formula presented). However, for (formula presented), the QMC simulations (Refs. 12 and 13) give the singlet state (formula presented) as the lowest-energy state as opposed to the triplet state (formula presented) obtained in DFT, which is in agreement with experiments (Refs. 1234). This emphasizes the importance of the third dimension in realistically modeling the confining potential in the dot.
  • 36
    • 85038273994 scopus 로고
    • Elements de Mecanique Ondulatoire, edited by, Bibliotheque Scientifique Internationale, Paris
    • Elements de Mecanique Ondulatoire, edited by W. Heitler (Bibliotheque Scientifique Internationale, Paris, 1964).
    • (1964)
    • Heitler, W.1
  • 37
    • 85038298220 scopus 로고    scopus 로고
    • The choice of a particular spin as well as the sign of the angular quantum number M is, of course, arbitrary. Similarly, for the third shell, we choose (formula presented) and (formula presented). For the fourth shell, (formula presented) and (formula presented)
    • The choice of a particular spin as well as the sign of the angular quantum number M is, of course, arbitrary. Similarly, for the third shell, we choose (formula presented) and (formula presented). For the fourth shell, (formula presented) and (formula presented).


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.