2018
DOI: 10.1088/1612-202x/aad28b
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Pump-gain integrated functional laser fiber towards 10 kW-level high-power applications

Abstract: To incorporate sufficient pump energy from multi-hundred watt-level 976 nm commercial laser diodes, a new kind of (8  +  1)-type pump-gain integrated functional laser ((8  +  1)-PIFL) fiber was fabricated by our newly optimized special fiber assembly and coating techniques for the first time. This (8  +  1)-PIFL fiber allowed for 10.66 kW aggregated pump power at 976 nm from six counter-pump ports in a master oscillator power amplifier laser setup and stably presented 8.72 kW laser output at 1079.4 nm with a h… Show more

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Cited by 19 publications
(10 citation statements)
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“…In this case, if more pumping power are expected to inject, one just need to simply increase the number of pump cores. With LD pumping source, the reported maximum output power of all-fiberized LDSP is 11.23 kW [12][13][14][15]. The situation is rather complicated when considering a higher power up to 20 or 30 kW.…”
Section: Introductionmentioning
confidence: 99%
“…In this case, if more pumping power are expected to inject, one just need to simply increase the number of pump cores. With LD pumping source, the reported maximum output power of all-fiberized LDSP is 11.23 kW [12][13][14][15]. The situation is rather complicated when considering a higher power up to 20 or 30 kW.…”
Section: Introductionmentioning
confidence: 99%
“…During the past two decades, owing to the rapid development of high-brightness laser diodes (LDs) and the large mode area (LMA) double-cladding fiber fabrication technology, the average output power of fiber lasers has experienced a dramatic boost with near diffraction-limited beam quality [3][4][5]. At present, a number of high-power continuouswave (CW) fiber lasers with output power beyond 5 kW are realized through a master oscillator power amplifier (MOPA) architecture [6][7][8][9][10]. However, the MOPA system is susceptible to reflection from materials during processing, which makes it restricted in industrial applications.…”
Section: Introductionmentioning
confidence: 99%
“…Due to the far-reaching impact, mode instability in various fiber laser systems has been under extensive theoretical and experimental investigation in recent years, but most of the work belongs to fiber lasers employing end-coupled cladding-pumping (ECCP) schemes [8,9]. Sidepumping scheme, especially distributed side-coupled cladding-pumped (DSCCP) fiber or GTWave fiber, is another good choice for high power fiber laser systems [13][14][15][16][17], which is one of the important technologies to enable high power scaling of fiber lasers [18][19][20][21][22][23][24]. Impressing power results have been reported in [17,22], where signal fiber with large pump area and backward pumping scheme has been employed to suppress mode instability [17].…”
Section: Introductionmentioning
confidence: 99%
“…Sidepumping scheme, especially distributed side-coupled cladding-pumped (DSCCP) fiber or GTWave fiber, is another good choice for high power fiber laser systems [13][14][15][16][17], which is one of the important technologies to enable high power scaling of fiber lasers [18][19][20][21][22][23][24]. Impressing power results have been reported in [17,22], where signal fiber with large pump area and backward pumping scheme has been employed to suppress mode instability [17]. Recently, researchers have reported mode instability in DSCCP lasers [25,26].…”
Section: Introductionmentioning
confidence: 99%
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