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Multimode Graded Index Fiber with Random Array of Bragg Gratings and Its Raman Lasing Properties. / Kuznetsov, Alexey G.; Wolf, Alexey A.; Munkueva, Zhibzema E. et al.

In: Fibers, Vol. 11, No. 6, 48, 06.2023.

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Kuznetsov AG, Wolf AA, Munkueva ZE, Dostovalov AV, Babin SA. Multimode Graded Index Fiber with Random Array of Bragg Gratings and Its Raman Lasing Properties. Fibers. 2023 Jun;11(6):48. doi: 10.3390/fib11060048

Author

Kuznetsov, Alexey G. ; Wolf, Alexey A. ; Munkueva, Zhibzema E. et al. / Multimode Graded Index Fiber with Random Array of Bragg Gratings and Its Raman Lasing Properties. In: Fibers. 2023 ; Vol. 11, No. 6.

BibTeX

@article{eabdaa3255a44353ad315f6a79c12b2c,
title = "Multimode Graded Index Fiber with Random Array of Bragg Gratings and Its Raman Lasing Properties",
abstract = "Light propagation in multimode fibers is known to experience various nonlinear effects, which are being actively studied. One of the interesting effects is the brightness enhancement at the Raman conversion of the multimode beam in graded index (GRIN) fiber due to beam cleanup at Raman amplification and mode selective feedback in the Raman laser cavity based on fiber Bragg gratings (FBGs) with special transverse structure. It is also possible to explore random distributed feedback based on Rayleigh backscattering on natural refractive index fluctuations in GRIN fibers, but it is rather weak, requiring very high power multimode pumping for random lasing. Here, we report on the first realization of femtosecond pulse-inscribed arrays of weak randomly spaced FBGs in GRIN fibers and study Raman lasing at its direct pumping by highly multimode (M2~34) 940-nm laser diodes. The fabricated 1D–3D FBG arrays are used as a complex output mirror, together with the highly reflective input FBG in 1-km fiber. Above threshold pump power (~100 W), random lasing of the Stokes beam at 976 nm is obtained with output power exceeding 28 W at 174 W pumping. The beam quality parameter varies for different arrays, reaching M2~2 at the linewidth narrowing to 0.1–0.2 nm due to the interference effects, with the best characteristics for the 2D array.",
keywords = "fiber Bragg grating, fiber Raman laser, multimode fiber, random array",
author = "Kuznetsov, {Alexey G.} and Wolf, {Alexey A.} and Munkueva, {Zhibzema E.} and Dostovalov, {Alexander V.} and Babin, {Sergey A.}",
note = "This research was funded by Russian Science Foundation, grant 21-72-30024. Публикация для корректировки.",
year = "2023",
month = jun,
doi = "10.3390/fib11060048",
language = "English",
volume = "11",
journal = "Fibers",
issn = "2079-6439",
publisher = "Multidisciplinary Digital Publishing Institute (MDPI)",
number = "6",

}

RIS

TY - JOUR

T1 - Multimode Graded Index Fiber with Random Array of Bragg Gratings and Its Raman Lasing Properties

AU - Kuznetsov, Alexey G.

AU - Wolf, Alexey A.

AU - Munkueva, Zhibzema E.

AU - Dostovalov, Alexander V.

AU - Babin, Sergey A.

N1 - This research was funded by Russian Science Foundation, grant 21-72-30024. Публикация для корректировки.

PY - 2023/6

Y1 - 2023/6

N2 - Light propagation in multimode fibers is known to experience various nonlinear effects, which are being actively studied. One of the interesting effects is the brightness enhancement at the Raman conversion of the multimode beam in graded index (GRIN) fiber due to beam cleanup at Raman amplification and mode selective feedback in the Raman laser cavity based on fiber Bragg gratings (FBGs) with special transverse structure. It is also possible to explore random distributed feedback based on Rayleigh backscattering on natural refractive index fluctuations in GRIN fibers, but it is rather weak, requiring very high power multimode pumping for random lasing. Here, we report on the first realization of femtosecond pulse-inscribed arrays of weak randomly spaced FBGs in GRIN fibers and study Raman lasing at its direct pumping by highly multimode (M2~34) 940-nm laser diodes. The fabricated 1D–3D FBG arrays are used as a complex output mirror, together with the highly reflective input FBG in 1-km fiber. Above threshold pump power (~100 W), random lasing of the Stokes beam at 976 nm is obtained with output power exceeding 28 W at 174 W pumping. The beam quality parameter varies for different arrays, reaching M2~2 at the linewidth narrowing to 0.1–0.2 nm due to the interference effects, with the best characteristics for the 2D array.

AB - Light propagation in multimode fibers is known to experience various nonlinear effects, which are being actively studied. One of the interesting effects is the brightness enhancement at the Raman conversion of the multimode beam in graded index (GRIN) fiber due to beam cleanup at Raman amplification and mode selective feedback in the Raman laser cavity based on fiber Bragg gratings (FBGs) with special transverse structure. It is also possible to explore random distributed feedback based on Rayleigh backscattering on natural refractive index fluctuations in GRIN fibers, but it is rather weak, requiring very high power multimode pumping for random lasing. Here, we report on the first realization of femtosecond pulse-inscribed arrays of weak randomly spaced FBGs in GRIN fibers and study Raman lasing at its direct pumping by highly multimode (M2~34) 940-nm laser diodes. The fabricated 1D–3D FBG arrays are used as a complex output mirror, together with the highly reflective input FBG in 1-km fiber. Above threshold pump power (~100 W), random lasing of the Stokes beam at 976 nm is obtained with output power exceeding 28 W at 174 W pumping. The beam quality parameter varies for different arrays, reaching M2~2 at the linewidth narrowing to 0.1–0.2 nm due to the interference effects, with the best characteristics for the 2D array.

KW - fiber Bragg grating

KW - fiber Raman laser

KW - multimode fiber

KW - random array

UR - https://www.scopus.com/record/display.uri?eid=2-s2.0-85163748323&origin=inward&txGid=8aaf0c39039065bdf453341e60dbc02d

UR - https://www.mendeley.com/catalogue/cea114a1-7497-3aa8-bd82-ac428294009a/

U2 - 10.3390/fib11060048

DO - 10.3390/fib11060048

M3 - Article

VL - 11

JO - Fibers

JF - Fibers

SN - 2079-6439

IS - 6

M1 - 48

ER -

ID: 59251604