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Volumn 43, Issue 30, 2004, Pages 5669-5681

Quantitative imaging through a spectrograph. 1. Principles and theory

Author keywords

[No Author keywords available]

Indexed keywords

CAMERAS; CHARGE COUPLED DEVICES; DATA ACQUISITION; ELECTROMAGNETIC WAVE DIFFRACTION; LIGHT SCATTERING; RAMAN SCATTERING; SPECTROGRAPHS;

EID: 8344268634     PISSN: 1559128X     EISSN: 15394522     Source Type: Journal    
DOI: 10.1364/AO.43.005669     Document Type: Article
Times cited : (8)

References (34)
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    • note
    • Unless explicitly stated otherwise, the integration limits will be from -∞ to + ∞ for (reciprocal) space coordinates and from 0 to +∞ for wavelengths and frequencies.
  • 19
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    • note
    • out).
  • 20
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    • note
    • The line at λ = 579.40 nm is an unresolved doublet. In fact, the exact wavelengths used do not matter for the processing of OMA graphs.
  • 24
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    • note
    • As input signal S(x) of the FT is purely real, the Fourier-transformed data S̄̃(k) are even under complex conjugation; i.e., S̄̃(-k) = S̄̃*(k). Therefore, only the positive k components need to be plotted to represent all power information.
  • 30
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    • note
    • This is a general property of Fourier transformation. For visual clarity, the reconstructions presented in this paper (Figs. 4 and 6) have been recentered in the image frames.
  • 32
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    • See, e.g., Ref. 1, Sec. 3.6
    • See, e.g., Ref. 1, Sec. 3.6.
  • 34
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    • note
    • 2 = S × S*), and the norm of the signal ∥S∥ is the integral over S.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.