메뉴 건너뛰기




Volumn 81, Issue 3, 2010, Pages

Hole-spin mixing in InAs quantum dot molecules

Author keywords

[No Author keywords available]

Indexed keywords


EID: 77954826237     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.81.035308     Document Type: Article
Times cited : (67)

References (42)
  • 8
    • 59249084035 scopus 로고    scopus 로고
    • 10.1103/PhysRevB.79.045307
    • T. Andlauer and P. Vogl, Phys. Rev. B 79, 045307 (2009). 10.1103/PhysRevB.79.045307
    • (2009) Phys. Rev. B , vol.79 , pp. 045307
    • Andlauer, T.1    Vogl, P.2
  • 9
    • 77954822406 scopus 로고    scopus 로고
    • 10.1103/Physics.2.16
    • M. F. Doty and D. Gammon, Phys. 2, 16 (2009). 10.1103/Physics.2.16
    • (2009) Phys. , vol.2 , pp. 16
    • Doty, M.F.1    Gammon, D.2
  • 21
    • 27144468630 scopus 로고    scopus 로고
    • 10.1103/PhysRevLett.95.076805
    • D. V. Bulaev and D. Loss, Phys. Rev. Lett. 95, 076805 (2005). 10.1103/PhysRevLett.95.076805
    • (2005) Phys. Rev. Lett. , vol.95 , pp. 076805
    • Bulaev, D.V.1    Loss, D.2
  • 22
    • 0043210202 scopus 로고
    • 10.1103/PhysRev.97.869
    • J. M. Luttinger and W. Kohn, Phys. Rev. 97, 869 (1955). 10.1103/PhysRev.97.869
    • (1955) Phys. Rev. , vol.97 , pp. 869
    • Luttinger, J.M.1    Kohn, W.2
  • 30
  • 36
    • 77954823553 scopus 로고    scopus 로고
    • For the particular QDM shown in Fig. the dark exciton lies 202 μeV below the bright exciton.
    • For the particular QDM shown in Fig. the dark exciton lies 202 μ eV below the bright exciton.
  • 37
    • 77954829775 scopus 로고    scopus 로고
    • We observe that the coupling of the atomic ground state of the bottom dot with the first atomic excited state of the top dot leads to a larger anticrossing than the coupling of the two ground states. This is also consistent with a lateral misalignment of the dots, as the first atomic excited state has a p -like envelope function that could couple more easily to a misaligned bottom dot than the s -like envelope of the atomic ground state.
    • We observe that the coupling of the atomic ground state of the bottom dot with the first atomic excited state of the top dot leads to a larger anticrossing than the coupling of the two ground states. This is also consistent with a lateral misalignment of the dots, as the first atomic excited state has a p -like envelope function that could couple more easily to a misaligned bottom dot than the s -like envelope of the atomic ground state.
  • 38
    • 77954826849 scopus 로고    scopus 로고
    • For sufficiently strong tunneling they may even replace HH as the ground state, see Ref..
    • For sufficiently strong tunneling they may even replace HH as the ground state, see Ref..
  • 39
    • 77954832498 scopus 로고    scopus 로고
    • The misalignment modifies not only the magnitude of the spin-flip tunneling rate but also that of the spin-conserving one. Therefore, for a given barrier thickness and lateral offset, the states with opposite pseudospin may not intersect. This is why in Fig. inset we only plot segments.
    • The misalignment modifies not only the magnitude of the spin-flip tunneling rate but also that of the spin-conserving one. Therefore, for a given barrier thickness and lateral offset, the states with opposite pseudospin may not intersect. This is why in Fig. inset we only plot segments.
  • 40
    • 77954820206 scopus 로고    scopus 로고
    • We note that the kp theory with the inclusion of lateral offsets predicts two anticrossings with different magnitudes. Recent data suggests that this is observed in certain samples. We anticipate further exploration of this anticrossing asymmetry in a future publication.
    • We note that the k p theory with the inclusion of lateral offsets predicts two anticrossings with different magnitudes. Recent data suggests that this is observed in certain samples. We anticipate further exploration of this anticrossing asymmetry in a future publication.
  • 41
    • 77954820722 scopus 로고    scopus 로고
    • Sh would be even closer to ±1/2 if we included strain in our model, further reducing the LH contribution to the low-lying spinors.
    • S h would be even closer to ± 1 / 2 if we included strain in our model, further reducing the LH contribution to the low-lying spinors.
  • 42
    • 77954827830 scopus 로고    scopus 로고
    • Due to the strong tunneling of LHs, the corresponding antibonding states are much higher in energy and have negligible influence on the spin mixing.
    • Due to the strong tunneling of LHs, the corresponding antibonding states are much higher in energy and have negligible influence on the spin mixing.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.