2001
DOI: 10.1016/s0030-4018(01)01584-x
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On the design of enhancement cavities for second harmonic generation

Abstract: Enhancement cavities using o -axis spherical mirrors allow the elliptical Gaussian beams from semiconductor diode lasers to be matched directly to the optimum beam pro®le for frequency conversion in a nonlinear crystal. We give a general recipe for the design of such cavities. Ó

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Cited by 17 publications
(7 citation statements)
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“…It is as small as possible to limit the astigmatism caused by the tilted curved mirrors. This geometry leads to a circular beam waist inside the crystal of 35 µm as calculated by ABCD matrix formalism [21] that is close to the optimal value for the Boyd-Kleinman factor.…”
Section: Methodssupporting
confidence: 57%
“…It is as small as possible to limit the astigmatism caused by the tilted curved mirrors. This geometry leads to a circular beam waist inside the crystal of 35 µm as calculated by ABCD matrix formalism [21] that is close to the optimal value for the Boyd-Kleinman factor.…”
Section: Methodssupporting
confidence: 57%
“…This can be obtained by second-harmonic generation ͑SHG͒ in an external enhancement cavity containing a nonlinear crystal, where a cw titanium:sapphire ͑Ti:S͒ laser provides the fundamental frequency. 4,5 SHG in an external enhancement cavity forms the basis of the laser setup used in our laboratory ͑see Ref. 6 and references therein͒.…”
Section: Introductionmentioning
confidence: 99%
“…Relation (5) for the optimum ξ = 2.84 is equivalent with obtaining a beam waist of 28 μm in the middle of the crystal. Using the ray transfer matrix analysis [20] we designed a bow tie resonator that allows us to fit the oven with the crystal in the middle of the short arm and to obtain the required beam waist in the middle of the crystal (see Fig. 5).…”
Section: Methodsmentioning
confidence: 99%