메뉴 건너뛰기




Volumn 86, Issue 4, 2001, Pages 700-703

Counting statistics of photons produced by electronic shot noise

Author keywords

[No Author keywords available]

Indexed keywords

ELECTRIC CURRENTS; ELECTRON TUNNELING; PHOTODETECTORS; POISSON EQUATION; RADIATION; SEMICONDUCTOR QUANTUM DOTS; STATISTICAL METHODS;

EID: 0035138384     PISSN: 00319007     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevLett.86.700     Document Type: Article
Times cited : (114)

References (26)
  • 2
    • 0000671430 scopus 로고    scopus 로고
    • For a discussion of the experiments by M. Henny et al. [Science 284, 296 (1999)] and W. D. Oliver et al. [Science 284, 299 (1999)], see M. Büttiker, Science 284, 275 (1999).
    • (1999) Science , vol.284 , pp. 296
    • Henny, M.1
  • 3
    • 0000528418 scopus 로고    scopus 로고
    • For a discussion of the experiments by M. Henny et al. [Science 284, 296 (1999)] and W. D. Oliver et al. [Science 284, 299 (1999)], see M. Büttiker, Science 284, 275 (1999).
    • (1999) Science , vol.284 , pp. 299
    • Oliver, W.D.1
  • 4
    • 0007278150 scopus 로고    scopus 로고
    • For a discussion of the experiments by M. Henny et al. [Science 284, 296 (1999)] and W. D. Oliver et al. [Science 284, 299 (1999)], see M. Büttiker, Science 284, 275 (1999).
    • (1999) Science , vol.284 , pp. 275
    • Büttiker, M.1
  • 11
    • 0342334572 scopus 로고    scopus 로고
    • note
    • The double-quantum-dot photodetector has a dead time of 1/δω, set by the width δω of the inelastic transition. Photon bunching occurs on the time scale of the inverse bandwidth of the detected radiation, which is also 1/δω. This is why one would need at least two such devices to measure deviations from Poisson statistics due to photon bunching. The theory presented here, appropriate for an array of devices, does not include dead-time effects.
  • 12
    • 34548601250 scopus 로고
    • R. J. Glauber, Phys. Rev. Lett. 10, 84 (1963); P. L. Kelley and W. H. Kleiner, Phys. Rev. 136, A316 (1964).
    • (1963) Phys. Rev. Lett. , vol.10 , pp. 84
    • Glauber, R.J.1
  • 14
    • 0342334568 scopus 로고    scopus 로고
    • note
    • This binomial coefficient is called "negative" because it appears as the expansion coefficient of 1 - x to a negative power - v. It counts the number of partitions of n bosons among v states.
  • 15
    • 0000320598 scopus 로고
    • L. S. Levitov and G. B. Lesovik, JETP Lett. 58, 230 (1993); L. S. Levitov, H. Lee, and G. B. Lesovik, J. Math. Phys. (N.Y.) 37, 4845 (1996).
    • (1993) JETP Lett. , vol.58 , pp. 230
    • Levitov, L.S.1    Lesovik, G.B.2
  • 22
    • 0343204127 scopus 로고    scopus 로고
    • note
    • p»f increase linearly with the detection time τ in the long-time limit.
  • 23
    • 0039600042 scopus 로고
    • The case of photodetection by emission was studied within the framework of Glauber's photodetection theory by L. Mandel, Phys. Rev. 152, 438 (1966). The photocount at low temperatures is then dominated by vacuum fluctuations, so that this mode of operation is less well suited for the study of nonequilibrium fluctuations such as shot noise.
    • (1966) Phys. Rev. , vol.152 , pp. 438
    • Mandel, L.1


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.