2013
DOI: 10.1117/12.2003999
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Optimization of fiber coupling in ultra-high power pump modules at λ = 980 nm

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Cited by 13 publications
(8 citation statements)
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“…This is a long-known technique, with W ~ 3...5 µm used to ensure laterally single mode operation (e.g. in [3]). As discussed in [19], W = 30 µm enables BPP ≤ 2 mm×mrad to be sustained to P op ~ 8 W, enabled by the use of advanced vertical layer designs (to sustain high η E to high current densities) and facet passivation (for reliability at high output power densities).…”
Section: Status Of Distributed-feedback Narrow-stripe Ba Lasers (Dfb-mentioning
confidence: 99%
See 1 more Smart Citation
“…This is a long-known technique, with W ~ 3...5 µm used to ensure laterally single mode operation (e.g. in [3]). As discussed in [19], W = 30 µm enables BPP ≤ 2 mm×mrad to be sustained to P op ~ 8 W, enabled by the use of advanced vertical layer designs (to sustain high η E to high current densities) and facet passivation (for reliability at high output power densities).…”
Section: Status Of Distributed-feedback Narrow-stripe Ba Lasers (Dfb-mentioning
confidence: 99%
“…This corresponds to a lateral (slow-axis) linear brightness, B lin = P op / BPP = 3.3 W/mm×mrad [2], where BPP = 3 mm×mrad is given by BPP = 0.25 × Θ L 95% × W 95% and W 95% is the emission aperture at 95% power content. The brightness of these devices is comparable to laterally single mode lasers, which operate at P op ~ 1 W and diffraction limited BPP ~ 0.3 mm×mrad [3].…”
Section: Introductionmentioning
confidence: 99%
“…We have optimized laser diodes in the 1060 nm wavelength range for improved chip and fiber coupling efficiency, output power and linearity in pulsed operation utilizing the design rules recently reported for 980 nm pump lasers [3] . Processed as spatial single mode lasers using a ridge waveguide process those devices are capable to deliver in excess of 3 W ex facet output power in CW mode and 1.8 W when fiber coupled, reaching the 1 W level at 1.35 A.…”
Section: Seed Laser At 1060 Nmmentioning
confidence: 99%
“…In the fast axis, the divergence is very large because of the small modal size perpendicular to the active layers. Plenty of designs were reported to reduce the vertical far-field angle such as the asymmetric waveguide [10], the large optical cavity (LOC) structure [11], [12], the passive far-field reduction layer [13], the longitudinal PBC waveguide [14] and the plasmonic collimators [15]. Vertical divergence of less than 10°at full-width at half-maximum (FWHM) has been reported by the LOC [16] and longitudinal PBC design [17], with powers over 1 W in CW mode.…”
Section: Introductionmentioning
confidence: 99%