Standard

2nd-order random lasing in a multimode diode-pumped graded-index fiber. / Evmenova, Ekaterina A.; Kuznetsov, Alexey G.; Nemov, Ilya N. et al.

In: Scientific Reports, Vol. 8, No. 1, 17495, 01.12.2018, p. 17495.

Research output: Contribution to journalArticlepeer-review

Harvard

Evmenova, EA, Kuznetsov, AG, Nemov, IN, Wolf, AA, Dostovalov, AV, Kablukov, SI & Babin, SA 2018, '2nd-order random lasing in a multimode diode-pumped graded-index fiber', Scientific Reports, vol. 8, no. 1, 17495, pp. 17495. https://doi.org/10.1038/s41598-018-35767-9

APA

Evmenova, E. A., Kuznetsov, A. G., Nemov, I. N., Wolf, A. A., Dostovalov, A. V., Kablukov, S. I., & Babin, S. A. (2018). 2nd-order random lasing in a multimode diode-pumped graded-index fiber. Scientific Reports, 8(1), 17495. [17495]. https://doi.org/10.1038/s41598-018-35767-9

Vancouver

Evmenova EA, Kuznetsov AG, Nemov IN, Wolf AA, Dostovalov AV, Kablukov SI et al. 2nd-order random lasing in a multimode diode-pumped graded-index fiber. Scientific Reports. 2018 Dec 1;8(1):17495. 17495. doi: 10.1038/s41598-018-35767-9

Author

Evmenova, Ekaterina A. ; Kuznetsov, Alexey G. ; Nemov, Ilya N. et al. / 2nd-order random lasing in a multimode diode-pumped graded-index fiber. In: Scientific Reports. 2018 ; Vol. 8, No. 1. pp. 17495.

BibTeX

@article{e7a0f2ed54c34b7bab61fd9654bfa1a3,
title = "2nd-order random lasing in a multimode diode-pumped graded-index fiber",
abstract = "Raman lasing in a graded-index fiber (GIF) attracts now great deal of attention due to the opportunity to convert high-power multimode laser diode radiation into the Stokes wave with beam quality improvement based on the Raman clean-up effect. Here we report on the cascaded Raman generation of the 2nd Stokes order in the 1.1-km long GIF with 100-μm core directly pumped by 915-nm diodes. In the studied all-fiber scheme, the 1st Stokes order is generated at 950–954 nm in a linear cavity formed at GIF ends by two fiber Bragg gratings (FBGs) securing beam quality improvement from M2 ≈ 30 to M2 ≈ 2.3 due to special transverse structure of FBGs. The 2nd Stokes wave is generated either in linear (two FBGs) or half-open (one FBG) cavity with random distributed feedback via Rayleigh backscattering. Their comparison shows that the random lasing provides better beam quality and higher slope efficiency. Nearly diffraction limited beam (M2 ≈ 1.6) with power up to 27 W at maximum gain (996 nm), and 17 W at the detuned wavelength of 978 nm has been obtained, thus demonstrating that the 2nd-order random lasing in diode-pumped GIF with FBGs provides high-efficiency high-quality beam generation in a broad wavelength range within the Raman gain spectral profile.",
keywords = "BEAM, CW, DISTRIBUTED-FEEDBACK, HIGH-EFFICIENCY, LASER, RAMAN FIBER",
author = "Evmenova, {Ekaterina A.} and Kuznetsov, {Alexey G.} and Nemov, {Ilya N.} and Wolf, {Alexey A.} and Dostovalov, {Alexandr V.} and Kablukov, {Sergey I.} and Babin, {Sergey A.}",
note = "Publisher Copyright: {\textcopyright} 2018, The Author(s).",
year = "2018",
month = dec,
day = "1",
doi = "10.1038/s41598-018-35767-9",
language = "English",
volume = "8",
pages = "17495",
journal = "Scientific Reports",
issn = "2045-2322",
publisher = "Nature Publishing Group",
number = "1",

}

RIS

TY - JOUR

T1 - 2nd-order random lasing in a multimode diode-pumped graded-index fiber

AU - Evmenova, Ekaterina A.

AU - Kuznetsov, Alexey G.

AU - Nemov, Ilya N.

AU - Wolf, Alexey A.

AU - Dostovalov, Alexandr V.

AU - Kablukov, Sergey I.

AU - Babin, Sergey A.

N1 - Publisher Copyright: © 2018, The Author(s).

PY - 2018/12/1

Y1 - 2018/12/1

N2 - Raman lasing in a graded-index fiber (GIF) attracts now great deal of attention due to the opportunity to convert high-power multimode laser diode radiation into the Stokes wave with beam quality improvement based on the Raman clean-up effect. Here we report on the cascaded Raman generation of the 2nd Stokes order in the 1.1-km long GIF with 100-μm core directly pumped by 915-nm diodes. In the studied all-fiber scheme, the 1st Stokes order is generated at 950–954 nm in a linear cavity formed at GIF ends by two fiber Bragg gratings (FBGs) securing beam quality improvement from M2 ≈ 30 to M2 ≈ 2.3 due to special transverse structure of FBGs. The 2nd Stokes wave is generated either in linear (two FBGs) or half-open (one FBG) cavity with random distributed feedback via Rayleigh backscattering. Their comparison shows that the random lasing provides better beam quality and higher slope efficiency. Nearly diffraction limited beam (M2 ≈ 1.6) with power up to 27 W at maximum gain (996 nm), and 17 W at the detuned wavelength of 978 nm has been obtained, thus demonstrating that the 2nd-order random lasing in diode-pumped GIF with FBGs provides high-efficiency high-quality beam generation in a broad wavelength range within the Raman gain spectral profile.

AB - Raman lasing in a graded-index fiber (GIF) attracts now great deal of attention due to the opportunity to convert high-power multimode laser diode radiation into the Stokes wave with beam quality improvement based on the Raman clean-up effect. Here we report on the cascaded Raman generation of the 2nd Stokes order in the 1.1-km long GIF with 100-μm core directly pumped by 915-nm diodes. In the studied all-fiber scheme, the 1st Stokes order is generated at 950–954 nm in a linear cavity formed at GIF ends by two fiber Bragg gratings (FBGs) securing beam quality improvement from M2 ≈ 30 to M2 ≈ 2.3 due to special transverse structure of FBGs. The 2nd Stokes wave is generated either in linear (two FBGs) or half-open (one FBG) cavity with random distributed feedback via Rayleigh backscattering. Their comparison shows that the random lasing provides better beam quality and higher slope efficiency. Nearly diffraction limited beam (M2 ≈ 1.6) with power up to 27 W at maximum gain (996 nm), and 17 W at the detuned wavelength of 978 nm has been obtained, thus demonstrating that the 2nd-order random lasing in diode-pumped GIF with FBGs provides high-efficiency high-quality beam generation in a broad wavelength range within the Raman gain spectral profile.

KW - BEAM

KW - CW

KW - DISTRIBUTED-FEEDBACK

KW - HIGH-EFFICIENCY

KW - LASER

KW - RAMAN FIBER

UR - http://www.scopus.com/inward/record.url?scp=85057619546&partnerID=8YFLogxK

U2 - 10.1038/s41598-018-35767-9

DO - 10.1038/s41598-018-35767-9

M3 - Article

C2 - 30504776

AN - SCOPUS:85057619546

VL - 8

SP - 17495

JO - Scientific Reports

JF - Scientific Reports

SN - 2045-2322

IS - 1

M1 - 17495

ER -

ID: 17684302