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Volumn 12, Issue 5, 1995, Pages 753-771

Femtosecond phase spectroscopy by use of frequency-domain interference

Author keywords

[No Author keywords available]

Indexed keywords

CADMIUM SULFIDE; DISPERSIONS; FREQUENCY DOMAIN ANALYSIS; GLASS; PHASE MODULATION; PROBES; SELENIUM COMPOUNDS;

EID: 4243691870     PISSN: 07403224     EISSN: None     Source Type: Journal    
DOI: 10.1364/JOSAB.12.000753     Document Type: Article
Times cited : (59)

References (69)
  • 3
    • 0004904985 scopus 로고
    • [Sov. Phys. JETP 16, 217 (1963)]
    • Sh. M. Kogan, Zh. Eksp. Teor. Fiz. 43, 304 (1962) [Sov. Phys. JETP 16, 217 (1963)].
    • (1962) Zh. Eksp. Teor. Fiz. , vol.43 , pp. 304
    • Kogan, S.M.1
  • 34
    • 84975596606 scopus 로고    scopus 로고
    • 0, so that the essentials of the following discussion are not affected. For example, Eq. (15) is unchanged. Also, because of the beam splitter’s thickness, there is a path difference between the reference and the probe, leading to the chirp difference between the two pulses. But this effect is negligibly small, so it is ignored in Eqs. (1)
    • 0, so that the essentials of the following discussion are not affected. For example, Eq. (15) is unchanged. Also, because of the beam splitter’s thickness, there is a path difference between the reference and the probe, leading to the chirp difference between the two pulses. But this effect is negligibly small, so it is ignored in Eqs. (1).
  • 35
    • 84975596039 scopus 로고    scopus 로고
    • To compare the transmission change directly with DF, it is more appropriate to use ln(ΔT/T)/2 = -ΔK than ΔT/T, especially when ΔK is large. But we use ΔT/T in this paper because conventionally it has been used most frequently
    • To compare the transmission change directly with DF, it is more appropriate to use ln(ΔT/T)/2 = -ΔK than ΔT/T, especially when ΔK is large. But we use ΔT/T in this paper because conventionally it has been used most frequently.
  • 42
    • 84975582152 scopus 로고
    • Phys. Rev. B 38, 7607 (1988)
    • M. Lindberg and S. W. Koch, J. Opt. Soc. Am. B5, 139 (1988). Phys. Rev. B 38, 7607 (1988).
    • (1988) J. Opt. Soc. Am. , vol.B5 , pp. 139
    • Lindberg, M.1    Koch, S.W.2
  • 52
    • 84975648622 scopus 로고    scopus 로고
    • From Eq. (29) it follows that for a two-level system the real and the imaginary parts of Δx(Ω) show the same dynamics as a function of τ for all Ω‘s. The assumption of the twolevel system in Subsection 3.A is based on this equation
    • From Eq. (29) it follows that for a two-level system the real and the imaginary parts of Δx(Ω) show the same dynamics as a function of τ for all Ω‘s. The assumption of the twolevel system in Subsection 3.A is based on this equation.
  • 54
    • 84975596547 scopus 로고    scopus 로고
    • Δφ(τ) of Fig. 3 of Ref. 8 shows a less sharp peak near zero delay than the present result in Fig. 12. This is because DFstd - RΔφ(τ) = ∫ T+ΔT T-ΔT dtπ (t,τ) was used previously instead of Δφ(τ) = π (t,τ), in Eqs. (B4) used here
    • Δφ(τ) of Fig. 3 of Ref. 8 shows a less sharp peak near zero delay than the present result in Fig. 12. This is because DFstd - RΔφ(τ) = ∫ T+ΔT T-ΔT dtπ (t,τ) was used previously instead of Δφ(τ) = π (t,τ), in Eqs. (B4) used here.
  • 64
    • 84975648609 scopus 로고    scopus 로고
    • To be strict, the results at the left and the right in the middle of Fig. 15 also do not satisfy the K-K relations, because they diverge to infinity as |Ω| → ∞, although conditions B are strictly satisfied together with the additional conditions because a hyperbolic-secant envelope is assumed for E(Ω). This means that the additional conditions are not sufficient but only necessary conditions
    • To be strict, the results at the left and the right in the middle of Fig. 15 also do not satisfy the K-K relations, because they diverge to infinity as |Ω| → ∞, although conditions B are strictly satisfied together with the additional conditions because a hyperbolic-secant envelope is assumed for E(Ω). This means that the additional conditions are not sufficient but only necessary conditions.
  • 65
    • 84975621474 scopus 로고    scopus 로고
    • The chirped-pulse case is discussed in Refs. 49 and 50
    • The chirped-pulse case is discussed in Refs. 49 and 50.
  • 67
    • 84975595939 scopus 로고    scopus 로고
    • Femtosecond continuum interferometer for transient phase and transmission spectroscopy
    • submitted to J. Opt. Soc. Am. B
    • E. Tokunaga, A. Terasaki, and T. Kobayashi, "Femtosecond continuum interferometer for transient phase and transmission spectroscopy," submitted to J. Opt. Soc. Am. B.
    • Tokunaga, E.1    Terasaki, A.2    Kobayashi, T.3
  • 69
    • 84975595960 scopus 로고    scopus 로고
    • Femtosecond phase spectroscopy of multi-level systems: Phthalocyanines
    • submitted to J. Opt. Soc. Am. B
    • E. Tokunaga, A. Terasaki, V. Valencia, T. Wada, H. Sasabe, and T. Kobayashi, "Femtosecond phase spectroscopy of multi-level systems: phthalocyanines," submitted to J. Opt. Soc. Am. B.
    • Tokunaga, E.1    Terasaki, A.2    Valencia, V.3    Wada, T.4    Sasabe, H.5    Kobayashi, T.6


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.