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Volumn 66, Issue 3, 2002, Pages 338031-3380310

Dispersive properties of quasi-phase-matched optical parametric amplifiers

Author keywords

[No Author keywords available]

Indexed keywords

COMPUTER SIMULATION; CONSTRAINT THEORY; CRYSTAL LATTICES; ELECTROMAGNETIC DISPERSION; GAIN CONTROL; LIGHT PROPAGATION; LITHIUM NIOBATE; MATHEMATICAL TRANSFORMATIONS; NONLINEAR OPTICS; OPTICAL PUMPING; SECOND HARMONIC GENERATION; SPECTRUM ANALYSIS;

EID: 0036756937     PISSN: 10502947     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevA.66.033803     Document Type: Article
Times cited : (13)

References (44)
  • 24
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    • M.J. Ablowitz, D.J. Kaup, A.C. Newell, and H. Segur, Stud. Appl. Math. 53, 249 (1973); M.J. Ablowitz, ibid. 58, 17 (1978).q
    • (1978) Stud. Appl. Math. , vol.58 , pp. 17
    • Ablowitz, M.J.1
  • 29
    • 85015755990 scopus 로고    scopus 로고
    • note
    • 12(Ω).
  • 31
    • 0031572718 scopus 로고    scopus 로고
    • A similar constraint occurs for the group delay in transmission of fiber Bragg gratings, which can be uniquely determined from the amplitude response of the grating [see L. Poladian, Opt. Lett. 22, 1571 (1997)].
    • (1997) Opt. Lett. , vol.22 , pp. 1571
    • Poladian, L.1
  • 35
    • 85015765664 scopus 로고    scopus 로고
    • note
    • A possible profile may be obtained by imposing the minimal phase shift requirement for r(δ), that is, by choosing the phase of r(δ) using a Hilbert transform again. More complex methods, that enable greater flexibility in the design, have recently been discussed in [33].
  • 36
    • 85015765885 scopus 로고    scopus 로고
    • note
    • The occurrence of abnormal (i.e., superluminal or negative) group velocities in pulse propagation through either atomic or photonic structures has been demonstrated on several occasions (see, for instance, [40] and references therein); however, the existence of negative group velocities for pulse propagation in photonic structures has not yet been predicted.
  • 37
    • 0036477831 scopus 로고    scopus 로고
    • In case of a Gaussian pulse envelope, a complex group delay and the inclusion of the second-order term in the asymptotic expansion of Eq. (A7) do not change the functional form of the pulse; however, they change the effective peak pulse delay, pulse duration, and pulse chirp. The role of the imaginary part of the complex delay time in the propagation of chirped Gaussian pulses has recently been investigated by: G. D'Aguanno, M. Centini, M.J. Bloemer, K. Myneni, M. Scalora, C.M. Bowden, C. Sibilia, and M. Bertolotti, Opt. Lett. 27, 176 (2002).
    • (2002) Opt. Lett. , vol.27 , pp. 176
    • D'Aguanno, G.1    Centini, M.2    Bloemer, M.J.3    Myneni, K.4    Scalora, M.5    Bowden, C.M.6    Sibilia, C.7    Bertolotti, M.8
  • 38
    • 85015732993 scopus 로고    scopus 로고
    • note
    • g2.
  • 40
    • 0000696181 scopus 로고    scopus 로고
    • M.W. Mitchell and R.Y. Chiao, Phys. Lett. A 245, 133 (1997); Am. J. Phys. 66, 14 (1998).
    • (1998) Am. J. Phys. , vol.66 , pp. 14


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.