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7
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84894002106
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note
-
Note that the choice of normal incidence of the pump upon the crystal is made for convenience. However, the following results are independent of this choice, provided that the three angles remain small (paraxial approximation). Note also that the angular dependence of refractive indices does not appear at this order of the expansion.
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8
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0025429901
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0015630633
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84975603523
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0001344026
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Thermal self-frequency locking of a doubly resonant optical parametric oscillator
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0002703518
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4 with double refraction
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16
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0000184273
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Spatiotemporal dynamics of optical parametric oscillators
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17
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84919696421
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Staliunas, K.1
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18
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0000991774
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Traveling-wave states and secondary instabilities in optical parametric oscillators
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Longhi, S.1
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19
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0001032529
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Order parameter description of walk-off effect on pattern selection in degenerate optical parametric oscillators
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21
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0003434416
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University Science, Mill Valley, Calif.
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A. E. Siegman, Lasers (University Science, Mill Valley, Calif., 1986).
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Lasers
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Siegman, A.E.1
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22
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-
84893993467
-
-
note
-
⊥.
-
-
-
-
23
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-
30244570429
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Improvement of optical parametric oscillators by nonresonant pump reflection
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Bjorkholm, J.1
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24
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21844490112
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81% conversion efficiency in frequency-stable continuous-wave parametric oscillation
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0026263188
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Algorithm 698: DCUHRE: An adaptive multidimensional integration routine for a vector of integrals
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26
-
-
84893985607
-
-
note
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i) presents small high-frequency components. Each time this criterion is not satisfied, we decrease the step size by a factor of 2 by keeping alreadycomputed points and evaluating only the intermediate points.
-
-
-
-
27
-
-
84894011192
-
-
note
-
z) directly after the backward fast Fourier transform. This interpolation is necessary for obtaining an accurate value of the desired maximum.
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