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Volumn 53, Issue 20, 1996, Pages 13694-13699

Stochastic treatment of the dynamics of excitons and excitonic molecules in CuCl nanocrystals

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EID: 0001580141     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.53.13694     Document Type: Article
Times cited : (12)

References (20)
  • 9
    • 0642357409 scopus 로고
    • There is a questionable point between Fig. 1 and Fig. 4 of the first reference. When luminescence shows exponential decay, the total luminescence intensity is given by τI(0), where τ is the decay time constant and I(0) is the luminescence intensity at t=0. The ratio of the time-integrated luminescence of the (Formula presented) exciton to that of the excitonic molecule should be about 190:13, because (Formula presented), (Formula presented), (Formula presented) (0), and (Formula presented) (0) are 380 ps, 65 ps, 500, and 200, respectively, in Fig. 4. In the luminescence spectrum of Fig. 1, however, the ratio of the intensity is about 3.4:1. This discrepancy is too large
    • see also T. Itoh et. al Jpn. J. Appl. Phys. 34, 1 (1995) and S. Yano et. al Phys. Rev. B 34, 140 (1994). There is a questionable point between Fig. 1 and Fig. 4 of the first reference. When luminescence shows exponential decay, the total luminescence intensity is given by τI(0), where τ is the decay time constant and I(0) is the luminescence intensity at t=0. The ratio of the time-integrated luminescence of the (Formula presented) exciton to that of the excitonic molecule should be about 190:13, because (Formula presented), (Formula presented), (Formula presented) (0), and (Formula presented) (0) are 380 ps, 65 ps, 500, and 200, respectively, in Fig. 4. In the luminescence spectrum of Fig. 1, however, the ratio of the intensity is about 3.4:1. This discrepancy is too large.
    • (1994) Phys. Rev. B , vol.34 , pp. 140
    • Itoh, T.1    Yano, S.2


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.