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Volumn 105, Issue 23, 1996, Pages 10263-10277

The superposition principle and cavity ring-down spectroscopy

Author keywords

[No Author keywords available]

Indexed keywords

BANDWIDTH; ELECTROMAGNETIC FIELDS; ETALONS; FOURIER TRANSFORMS; FREQUENCIES; FREQUENCY DOMAIN ANALYSIS; LIGHT TRANSMISSION; OPTICAL RESONATORS; PULSED LASER APPLICATIONS; RESONANCE;

EID: 0030379628     PISSN: 00219606     EISSN: None     Source Type: Journal    
DOI: 10.1063/1.472955     Document Type: Article
Times cited : (196)

References (33)
  • 11
    • 85033058709 scopus 로고    scopus 로고
    • note
    • In this paper we will follow the common convention of using complex values for the time dependent electric fields, with the implicit understanding that one should add the complex conjugate of the expressions to obtain the physical field. In the frequency domam, this convention implies that the value of Ẽ(ω) should be replaced by Ẽ(ω) + Ẽ(-ω).
  • 21
    • 85033064209 scopus 로고    scopus 로고
    • note
    • As discussed in Ref. 11, we need to use both Eq. (1) and its complex conjugate. Since only the term oscillating as exp(-iωt) will cause significant excitation (the rotating wave approximation), for positive frequencies (by the present phase convention), we will retain only the complex conjugate term.
  • 24
    • 0003434416 scopus 로고
    • University Science Books, Mill Valley, California
    • A. E. Siegman, Lasers (University Science Books, Mill Valley, California, 1986).
    • (1986) Lasers
    • Siegman, A.E.1
  • 25
    • 85033054228 scopus 로고    scopus 로고
    • note
    • -iwt″dt″. Then, treating explicitly the term exp(-ikz) present in the TEM functions, we can integrate over la producing a δ(t″-t + nz/c), which is eliminated by further integration over t″.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.