2012
DOI: 10.1117/12.908421
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Advances in performance and beam quality of 9xx-nm laser diodes tailored for efficient fiber coupling

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Cited by 19 publications
(11 citation statements)
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“…A common figure of merit for high power lasers is the so-called linear brightness, which is defined as lasing power divided by the half-width of the near field and the halfwidth of the far field [11]. In our case, the slow axis linear brightness at 2A rises by 55% from 0.9 to 1.4 W/mm*mrad after implementation of the air gap.…”
mentioning
confidence: 77%
“…A common figure of merit for high power lasers is the so-called linear brightness, which is defined as lasing power divided by the half-width of the near field and the halfwidth of the far field [11]. In our case, the slow axis linear brightness at 2A rises by 55% from 0.9 to 1.4 W/mm*mrad after implementation of the air gap.…”
mentioning
confidence: 77%
“…Modern BALDs with 100µm stripe-width are capable of achieving ~20W CW operation [16], [17]. These LDs are multimode along their slow axis direction and Gaussian-like single mode along their fast axis which is perpendicular to the p-n junction plane.…”
Section: Two-photon Absorption Coefficientmentioning
confidence: 99%
“…At high powers the increase in threshold current and droop in differential efficiency became big factors in lowering laser wall-plug efficiency. In diode pumped fiber lasers where high fiber coupling efficiency is required, the biggest obstacles to higher power scaling was the rise in the slow axis divergence due to internal heating [4] which limited the number of LDs that could be coupled into a fiber. To maintain good laser performance in future systems, new cooling concepts need to be explored.…”
Section: Introductionmentioning
confidence: 99%