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Volumn 22, Issue 2, 1997, Pages 102-104

Optical pulse compression to 5 fs at a 1-MHz repetition rate

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EID: 0000852826     PISSN: 01469592     EISSN: None     Source Type: Journal    
DOI: 10.1364/OL.22.000102     Document Type: Article
Times cited : (325)

References (27)
  • 21
    • 84975553122 scopus 로고
    • C. H. Brito Cruz, P. C. Becker, R. L. Fork, and C. V. Shank, Opt. Lett. 13, 123 (1988); B. E. Lemoff and C. P. J. Barty, Opt. Lett. 18, 1651 (1993). Note that Eq. (4) in the former paper is approximate since it neglects the beam propagation through the first prism.
    • (1988) Opt. Lett. , vol.13 , pp. 123
    • Brito Cruz, C.H.1    Becker, P.C.2    Fork, R.L.3    Shank, C.V.4
  • 22
    • 0027685604 scopus 로고
    • C. H. Brito Cruz, P. C. Becker, R. L. Fork, and C. V. Shank, Opt. Lett. 13, 123 (1988); B. E. Lemoff and C. P. J. Barty, Opt. Lett. 18, 1651 (1993). Note that Eq. (4) in the former paper is approximate since it neglects the beam propagation through the first prism.
    • (1993) Opt. Lett. , vol.18 , pp. 1651
    • Lemoff, B.E.1    Barty, C.P.J.2
  • 23
    • 0014563660 scopus 로고
    • The GVD of the grating compressor was calculated according to E. Treacy, IEEE J. Quantum Electron. QE-5, 454 (1969).
    • (1969) IEEE J. Quantum Electron. , vol.QE-5 , pp. 454
    • Treacy, E.1
  • 24
    • 0029293413 scopus 로고
    • The GVD of the chirped mirrors was provided by the supplier: R. Szipöcz, R&D Lezer-Optika Bt. (Budapest, Hungary). For dispersion measurements see also A. P. Kovacs, K. Osvay, Z. Bor, and R. Szipöcs, Opt. Lett. 20, 788 (1995).
    • (1995) Opt. Lett. , vol.20 , pp. 788
    • Kovacs, A.P.1    Osvay, K.2    Bor, Z.3    Szipöcs, R.4
  • 25
    • 5244251630 scopus 로고    scopus 로고
    • note
    • A more favorable ratio between the third- and second-order GVD was found for prisms with a smaller than conventionally used Brewster apex angle.
  • 26
    • 5244327856 scopus 로고    scopus 로고
    • note
    • Historically, there is some confusion about this definition. To quote a number of optical cycles makes sense only if one refers to the electric-field envelope, which is longer than the duration of the pulse intensity envelope by a factor of ∼1.5. Therefore the electric-field envelope of our 5-fs pulse contains ∼2.7 optical cycles at FWHM.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.