초록 ▼

Quasi-phasematching design to provide an approximation to a desired spectral amplitude response A(f) is provided. An initial phase response φ(f) corresponding to A(f) is generated. Preferably, d2φ(f)/df2 is proportional to A2(f). Alternatively, φ(f) can be a polynomial in f. A functi

Quasi-phasematching design to provide an approximation to a desired spectral amplitude response A(f) is provided. An initial phase response φ(f) corresponding to A(f) is generated. Preferably, d2φ(f)/df2 is proportional to A2(f). Alternatively, φ(f) can be a polynomial in f. A function h(x) is computed such that h(x) and H(f)=A(f)exp(iφ(f)) are a Fourier transform pair. A domain pattern function d(x) can be computed by binarizing h(x) (i.e., approximating h(x) with a constant-amplitude approximation). In some cases, the response provided by this d(x) is sufficiently close to A(f) that no further design work is necessary. In some embodiments of the invention, the need for binarization can be reduced or eliminated by providing amplitude modulation of the effective nonlinearity.

대표청구항 ▼

The invention claimed is: 1. A method for designing a quasi-phasematched optical frequency converter, the method comprising: a) specifying a non-negative real target spectral amplitude response A(f), wherein A(-f)=A(f); b) providing a real initial phase response φ(f) associated with A(f), wher

The invention claimed is: 1. A method for designing a quasi-phasematched optical frequency converter, the method comprising: a) specifying a non-negative real target spectral amplitude response A(f), wherein A(-f)=A(f); b) providing a real initial phase response φ(f) associated with A(f), wherein φ(f)=-φ(-f); c) calculating a real function h(x) such that h(x) and H(f)=A(f) exp(i φ(f)) are a Fourier transform pair; d) determining a real constant-amplitude domain pattern function d(x) and a real amplitude modulation function q(x) such that d(x)q(x) is an approximation to h(x). 2. The method of claim 1, wherein said providing a phase response comprises providing φ(f) such that d2φ(f)/df2 is proportional to A2(f). 3. The method of claim 1, wherein h(x) and H(f) are a discrete Fourier transform pair. 4. The method of claim 1, wherein h(x) and H(f) are a continuous Fourier transform pair. 5. The method of claim 1, wherein φ(f) is a polynomial in f. 6. The method of claim 5, wherein said providing a real initial phase response comprises determining coefficients of said polynomial to minimize a deviation of h2(x) from a constant value. 7. The method of claim 6, wherein said coefficients of said polynomial are coefficients of members of a predetermined polynomial basis set. 8. The method of claim 7, wherein said predetermined polynomial basis is selected from the group consisting of a power basis, a Legendre polynomial basis, a Chebyshev polynomial basis, and a basis of orthonormal polynomials. 9. A quasi-phasematched optical frequency converter comprising: a quasi-phasematched active region having a real constant-amplitude domain pattern function d(x) and having a real amplitude modulation function q(x); wherein an effective pattern function d'(x)=d(x)q(x) has a non-constant amplitude; wherein a function D(f) and d'(x) are a Fourier transform pair; wherein a non-negative real amplitude response A(f) and a real phase response φ(f) of the active region are defined via D(f)=A(f) exp(i φ(f)); wherein d2φ(f)/df2 is substantially proportional to A2(f). 10. A quasi-phasematched optical frequency converter comprising: a quasi-phasematched active region having a real constant-amplitude domain pattern function d(x) and having a real amplitude modulation function q(x); wherein an effective pattern function d'(x)=d(x)q(x) has a non-constant amplitude; wherein a function D(f) and d'(x) are a Fourier transform pair; wherein a non-negative real amplitude response A(f) and a real phase response φ(f) of the active region are defined via D(f)=A(f) exp(i φ(f)); wherein φ(f) is substantially non-sinusoidal; and wherein φ(f) includes a substantial contribution from 4th and higher order terms in a polynomial fit. 11. A quasi-phasematched optical frequency converter comprising: a quasi-phasematched active region having a real constant-amplitude domain pattern function d(x); an optical waveguide passing through part or all of said active region; wherein an overlap of an optical mode of said waveguide with said active region is varied along a length of said active region to provide an effective domain pattern function d'(x) having non-constant amplitude; wherein said overlap is varied by altering a transverse waveguide profile along said length of said active region; wherein said active region has a constant transverse domain width along said length. 12. The optical frequency converter of claim 11, wherein said overlap is varied by varying a transverse position of said waveguide relative to a transverse boundary of said active region. 13. The optical frequency converter of claim 11, wherein said overlap is varied by tapering said waveguide. 14. The optical frequency converter of claim 11, wherein said frequency converter has an input and an output, wherein said overlap is varied to smoothly decrease as said output is approached from within said converter, and wherein said overlap is varied to smoothly decrease as said input is approached from within said converter, whereby apodization of said converter is provided.