메뉴 건너뛰기




Volumn 79, Issue 24, 2009, Pages

Förster energy-transfer signatures in optically driven quantum dot molecules

Author keywords

[No Author keywords available]

Indexed keywords


EID: 67650091244     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.79.245309     Document Type: Article
Times cited : (11)

References (46)
  • 12
    • 0141677049 scopus 로고    scopus 로고
    • 10.1103/PhysRevB.68.075315
    • A. O. Govorov, Phys. Rev. B 68, 075315 (2003). 10.1103/PhysRevB.68.075315
    • (2003) Phys. Rev. B , vol.68 , pp. 075315
    • Govorov, A.O.1
  • 13
    • 42749106160 scopus 로고    scopus 로고
    • 10.1103/PhysRevB.70.201302;
    • A. N. Al-Ahmadi and S. E. Ulloa, Phys. Rev. B, 70, 201302 (R) (2004) 10.1103/PhysRevB.70.201302
    • (2004) Phys. Rev. B , vol.70 , pp. 201302
    • Al-Ahmadi, A.N.1    Ulloa, S.E.2
  • 18
    • 18244397526 scopus 로고
    • 10.1063/1.1699044;
    • J. Dexter, J. Chem. Phys. 21, 836 (1953) 10.1063/1.1699044
    • (1953) J. Chem. Phys. , vol.21 , pp. 836
    • Dexter, J.1
  • 30
    • 33748863633 scopus 로고    scopus 로고
    • 10.1021/jp961448i
    • J. A. Leegwater, J. Phys. Chem. 100, 14403 (1996). 10.1021/jp961448i
    • (1996) J. Phys. Chem. , vol.100 , pp. 14403
    • Leegwater, J.A.1
  • 31
    • 0004275291 scopus 로고    scopus 로고
    • Wiley, New York
    • Y. Yamamoto and A. Imamoglu, Mesoscopic Quantum Optics (Wiley, New York, 1999). Fast oscillating terms in H (t) are removed by the transformation, H = Λ† HΛ+i Λ† t Λ, with Λ= k e-i ξk t |k k|, such that ξi - ξj =0.
    • (1999) Mesoscopic Quantum Optics
    • Yamamoto, Y.1    Imamoglu, A.2
  • 40
    • 67650053150 scopus 로고    scopus 로고
    • Exciton transition energies and structure parameters, consistent with, and derived from measurements are as follows: Figs. 1 1 2: interdot distance d8.4nm, te, th =2.0,0.1meV, VF =0.08meV, and ΩT (B) =40μeV. Exciton bare energies: E X 01 01 =1248.01meV and E X 10 10 = E X 01 01 +10μeV. Figures 3 4: d∼8.25nm, te, th =2.1,0.12meV, VF =0.09meV, and ΩT (B) =140μeV. Biexciton bare energies: E X 02 02 =2492.85meV, E X 11 02 = E X 02 02 +17meV, and E X 20 11 = E X 11 02 -20μeV. Interband transition moments μT (B) =6.2e. Exciton-radiation couplings (controlled by the laser-pulse amplitude) are in the strong pumping regime, ΩT (B) τX, (XX). Exciton (biexciton) radiative recombination times τX (τXX) ∼1.0 (0.5) ns.
    • Exciton transition energies and structure parameters, consistent with, and derived from measurements are as follows: Figs. 1 1 2: interdot distance d8.4nm, te, th =2.0,0.1meV, VF =0.08meV, and ΩT (B) =40μeV. Exciton bare energies: E X 01 01 =1248.01meV and E X 10 10 = E X 01 01 +10μeV. Figures 3 4: d∼8.25nm, te, th =2.1,0.12meV, VF =0.09meV, and ΩT (B) =140μeV. Biexciton bare energies: E X 02 02 =2492.85meV, E X 11 02 = E X 02 02 +17meV, and E X 20 11 = E X 11 02 -20μeV. Interband transition moments μT (B) =6.2e. Exciton-radiation couplings (controlled by the laser-pulse amplitude) are in the strong pumping regime, ΩT (B) τX, (XX). Exciton (biexciton) radiative recombination times τX (τXX) ∼1.0 (0.5) ns.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.