2010
DOI: 10.1364/oe.18.016765
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An intra-cavity Raman laser using synthetic single-crystal diamond

Abstract: Low birefringence synthetic single-crystal diamond was used as a Raman laser medium inside a Q-switched Nd:YVO(4) laser. A maximum average output power of 375 mW was achieved at a wavelength of 1240 nm and a repetition rate of 6.3 kHz. This equates to a conversion efficiency of 4% from the diode laser to the first Stokes component at 1240 nm. Optical losses within the diamond (approximately 1% per single pass) limited the performance and are currently the main barrier to the demonstration of an efficient CW di… Show more

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Cited by 36 publications
(19 citation statements)
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“…The higher upper bound given by this technique compared to the ISO approach results from its lower accuracy, the effect of the coatings (these had some visible damage as a result of the laser experiments which may have contributed to the measured absorption), and the effect of any scattered light absorbed in the mount. Even so, an absorption coefficient of <0.006cm 1 is a significant improvement on the sample used in [8,9] where an absorption coefficient of ~0.03cm 1 was measured using the same apparatus. However, laser calorimetry is not, in general, sensitive to scatter, which may be a significant fraction of the overall loss if the absorption is small [23]: a different measurement technique would be required to determine this and hence the total loss.…”
Section: Low-loss Synthetic Diamondmentioning
confidence: 99%
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“…The higher upper bound given by this technique compared to the ISO approach results from its lower accuracy, the effect of the coatings (these had some visible damage as a result of the laser experiments which may have contributed to the measured absorption), and the effect of any scattered light absorbed in the mount. Even so, an absorption coefficient of <0.006cm 1 is a significant improvement on the sample used in [8,9] where an absorption coefficient of ~0.03cm 1 was measured using the same apparatus. However, laser calorimetry is not, in general, sensitive to scatter, which may be a significant fraction of the overall loss if the absorption is small [23]: a different measurement technique would be required to determine this and hence the total loss.…”
Section: Low-loss Synthetic Diamondmentioning
confidence: 99%
“…Recently, the use of high optical quality, single-crystal, synthetic diamond as a Raman material in external cavity [3][4][5][6] and intracavity [7][8][9] configurations has been demonstrated -made possible by the progress in diamond chemical vapour deposition (CVD) [10,11]. Diamond has a large Raman gain (64cm/GW at = 532nm [12] and between 12.5cm/GW [13] and 16.6cm/GW [5] at = 1064nm), broad transparency (0.23-2.5µm and >7µm [14]) and a large Raman shift (1332cm 1 [15]).…”
Section: Introductionmentioning
confidence: 99%
“…As the pump sources, mostly neodymium or ytterbium doped lasers generating at fundamental frequency or higher harmonics were used. The Raman laser operation at different first Stokes wavelengths was demonstrated: 275 nm [16], 573 nm [17,18], 1193 nm [19], and 1240 nm [20][21][22][23].…”
Section: Introductionmentioning
confidence: 99%
“…As a synthetic diamond prepared by a CVD method become available, Raman laser operation in intra-or external-cavity resonator configuration, and under continuous or pulsed pumping was investigated. Generation of the 1 st Stokes wavelength at 573 nm [1,2], 1193 nm [3], and 1240 nm [4,5] was demonstrated.…”
Section: Introductionmentioning
confidence: 99%