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Journal articles on the topic 'Erbium-Doped Fibre'

Author: Grafiati

Published: 11 December 2022

Last updated: 27 January 2023

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1

Khudyakov, M. M., A. E. Levchenko, V. V. Vel’miskin, K. K. Bobkov, S. S. Aleshkina, M. M. Bubnov, M. V. Yashkov, A. N. Guryanov, L. V. Kotov, and M. E. Likhachev. "Optimisation of the efficiency of tapered erbium-doped optical fibre." Quantum Electronics 51, no. 12 (December 1, 2021): 1056–60. http://dx.doi.org/10.1070/qel17651.

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Abstract We have developed a cladding pumped tapered erbium-doped fibre with a record-high core diameter for erbium-doped fibres (100 mm) and a near diffraction-limited beam quality (μ 2 ∼ 1.3). Optimisation of the tapered fibre parameters provided a high (18 %) efficiency of pump radiation conversion at a wavelength of 976 nm into signal radiation at a wavelength of 1560 nm.

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2

Lavrinovica, I., A. Supe, and J. Porins. "Experimental Measurement of Erbium-Doped Optical Fibre Charecteristics for Edfa Performance Optimization." Latvian Journal of Physics and Technical Sciences 56, no. 2 (April 1, 2019): 33–41. http://dx.doi.org/10.2478/lpts-2019-0011.

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Abstract The paper presents experimental study of the major erbium-doped fibre amplifier (EDFA) features such as gain at low signal and gain saturation by an application of different erbium-doped optical fibres (EDFs). The main objective of the research is to estimate how the performance of EDFA varies depending on the length of doped fibre, pumping configuration scheme, as well as excitation source power. It is shown that a high gain coefficient of 16–20 dB can be practically achieved.

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3

Pettitt, M. J., A. Hadjifotiou, and R. A. Baker. "Crosstalk in erbium doped fibre amplifiers." Electronics Letters 25, no. 6 (1989): 416. http://dx.doi.org/10.1049/el:19890286.

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4

Zotov, K. V., M. E. Likhachev, A. L. Tomashuk, M. M. Bubnov, M. V. Yashkov, and A. N. Gur'yanov. "Radiation-resistant erbium-doped silica fibre." Quantum Electronics 37, no. 10 (October 31, 2007): 946–49. http://dx.doi.org/10.1070/qe2007v037n10abeh013660.

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5

Kasik, I., O. Podrazky, J. Mrazek, J. Cajzl, J. Aubrecht, J. Probostova, P. Peterka, P. Honzatko, and A. Dhar. "Erbium and Al2O3 nanocrystals-doped silica optical fibers." Bulletin of the Polish Academy of Sciences Technical Sciences 62, no. 4 (December 1, 2014): 641–46. http://dx.doi.org/10.2478/bpasts-2014-0070.

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Abstract. Fibre lasers and inherently rare-earth-doped optical fibers nowadays pass through a new period of their progress aiming at high efficiency of systems and their high power. In this paper, we deal with the preparation of silica fibers doped with erbium and Al2O3 nanocrystals and the characterization of their optical properties. The fibers were prepared by the extended Modified Chemical Vapor Deposition (MCVD) method from starting chlorides or oxide nanopowders. Conventional as well as modified approaches led to a nanocrystalline mullite phase formation in the fiber cores in which erbium is dissolved. The proposed modified approach based on starting nanopowders led to improved geometry of preforms and fibers and consequently to the improvement of their background attenuation. Such nanocrystal -doped fibers can be used for ASE sources. Further improvement of fiber optical properties can be expected.

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6

CHU, P. L., and Y. L. XUE. "NONLINEAR EFFECTS IN ERBIUM-DOPED FIBRES." Journal of Nonlinear Optical Physics & Materials 02, no. 03 (July 1993): 401–13. http://dx.doi.org/10.1142/s0218199193000243.

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Theoretical and experimental investigations of the nonlinear refractive index in an Erbium-doped fibre is presented. The transient response of this fibre is also examined. The switching speed can be improved by using a signal power at a wavelength close to the resonant wavelength between the excited state and the ground state.

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7

Harun, Sulaiman Wadi, Mukul C. Paul, Shyamal Das, Anirban Dhar, and Harith Ahmad. "Mode-locked Thulium Ytterbium co-Doped Fiber Laser with Graphene Saturable Absorber." Photonics Letters of Poland 8, no. 4 (December 31, 2016): 104. http://dx.doi.org/10.4302/plp.2016.4.05.

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A passively mode-locked Thulium Ytterbium co-doped fiber laser (TYDFL) is demonstrated using a graphene polyvinyl alcohol saturable absorber as the mode-locker. With 980 nm multimode pumping, the laser operates at 1942.95 nm with repetition rate of 11.76 MHz. The pulse width is calculated to be around 52.85 ps. The maximum pulse energy of 1190.5 pJ is achieved at pump power of 1750 mW. Full Text: PDF ReferencesJ. Sotor et al., "Ultrafast thulium-doped fiber laser mode locked with black phosphorus", Opt. Lett. 40, 3885-3888 (2015) CrossRef J. Wang et al., "152 fs nanotube-mode-locked thulium-doped all-fiber laser", Nature Scientific Reports 6, 28885 (2016) CrossRef I. M. Babar et al., "Double-clad thulium/ytterbium co-doped octagonal-shaped fibre for fibre laser applications", Ukr. J. Phys. Opt. 15, 173-183 (2014) CrossRef Harun et al., "Mode-locked bismuth-based erbium-doped fiber laser with stable and clean femtosecond pulses output", Laser Phys. Lett. 8, 449-452 (2011) CrossRef M. A. Ismail et al., "Nanosecond soliton pulse generation by mode-locked erbium-doped fiber laser using single-walled carbon-nanotube-based saturable absorber", Applied Optics 51, 8621-8624 (2012) CrossRef G. Sobon et al., "Graphene Oxide vs. Reduced Graphene Oxide as saturable absorbers for Er-doped passively mode-locked fiber laser", Opt. Express 20, 19463-19473 (2012) CrossRef G. Sobon et al., "Thulium-doped all-fiber laser mode-locked by CVD-graphene/PMMA saturable absorber", Opt. Express 21, 12797-12802 (2013) CrossRef

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8

Seikai, S., T. Tohi, and Y. Kanaoka. "Erbium-doped fibre amplifier circuit having a subsidiary erbium-doped fibre useful for bidirectional optical transmission systems." Electronics Letters 30, no. 22 (October 27, 1994): 1877–78. http://dx.doi.org/10.1049/el:19941296.

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9

Wade, S. A., D. I. Forsyth, Q. Guofu, X. Chen, T. S. Chuan, W. Yong, T. Sun, and K. T. V. Grattan. "Dual Measurement of Strain and Temperature Using the Combination of Er3+ -Doped Fibre Fluorescence Lifetime and a Fibre Bragg Grating." Measurement and Control 34, no. 6 (July 2001): 175–78. http://dx.doi.org/10.1177/002029400103400606.

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Fibre optic sensing devices have been produced for the dual measurement of strain and temperature using the combined properties of fibre Bragg gratings and the fluorescence lifetime of erbium-doped fibre. Two different sensors were constructed with the fibre Bragg grating written in normal fibre and also written directly in the Er3+-doped fibre. Results obtained indicate that this technique can be used to measure strains and temperatures with accuracies of approximately 1.2°C and 20.4 με

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10

Popov, S. M., O. V. Butov, A. O. Kolosovskii, V. V. Voloshin, I. L. Vorob’ev, V. A. Isaev, D. V. Ryakhovskii, et al. "Optical fibres with an inscribed fibre Bragg grating array for sensor systems and random lasers." Quantum Electronics 51, no. 12 (December 1, 2021): 1101–6. http://dx.doi.org/10.1070/qel17659.

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Abstract We report the latest results on inscribing extended fibre Bragg grating (FBG) arrays upon fibre drawing, obtained at the Kotelnikov Institute of Radioengineering and Electronics of RAS. The properties of these structures are considered, and examples of their application in sensor systems of microwave dense wavelength multiplexing and as a basis for designing single-frequency fibre lasers are considered. The optical and laser characteristics of FBG arrays, inscribed (using 248-nm UV laser radiation) both in standard single-mode telecommunication fibres of the SMF-28 type and in erbium-doped active fibres, are investigated.

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11

Lai, Y. C., G. F. Qiu, W. Zhang, L. Zhang, I. Bennion, and K. T. V. Grattan. "Simultaneous Measurement of Temperature and Strain by Combining Active Fibre with Fibre Gratings." Measurement and Control 34, no. 6 (July 2001): 172–74. http://dx.doi.org/10.1177/002029400103400605.

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This paper reports on a novel optical fiber-based sensing system for conducting simultaneous measurement of temperature and strain. The sensor design is based on the combination of active fibre and fibre gratings. Addressing smart structure applications erbium/ytterbium co-doped fibre is used to meet the requirements for both high temperature responsivity and small sensor size. The temperature dependence of ASE power under different pump wavelengths is investigated. An optical reference is induced to enhance the measurement resolution. The feasibility of this technique for simultaneous measurement of temperature and strain is demonstrated.

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12

Sheng-Hai, Zhang, and Shen Ke. "Controlling hyperchaos in erbium-doped fibre laser." Chinese Physics 12, no. 2 (January 20, 2003): 149–53. http://dx.doi.org/10.1088/1009-1963/12/2/305.

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13

Kurkov, Andrei S., Vladimir M. Paramonov, M. V. Yashkov, S. E. Goncharov, and I. D. Zalevskii. "Multimode cladding-pumped erbium-doped fibre laser." Quantum Electronics 37, no. 4 (April 30, 2007): 343–44. http://dx.doi.org/10.1070/qe2007v037n04abeh013471.

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14

Zyskind, J. L., V. Mizrahi, D. J. DiGiovanni, and J. W. Sulhoff. "Short single frequency erbium-doped fibre laser." Electronics Letters 28, no. 15 (1992): 1385. http://dx.doi.org/10.1049/el:19920881.

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15

Abraham, D., R. Nagar, M. N. Ruberto, G. Eisenstein, J. L. Zyskind, D. Digiovanni, U. Koren, and G. Raybon. "Intracavity-diode-pumped erbium doped fibre laser." Electronics Letters 28, no. 19 (1992): 1830. http://dx.doi.org/10.1049/el:19921167.

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16

Teyo, T. C., P. Poopalan, and H. Ahmad. "Regenerative erbium-doped fibre ring laser-amplifier." Electronics Letters 35, no. 17 (1999): 1471. http://dx.doi.org/10.1049/el:19990981.

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17

Kimura, Y., and M. Nakazawa. "Gain characteristics of erbium-doped fibre amplifiers with high erbium concentration." Electronics Letters 28, no. 15 (1992): 1420. http://dx.doi.org/10.1049/el:19920903.

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18

Rühl, F. F. "Prediction of optimum fibre lengths for erbium doped fibre amplifiers." Electronics Letters 27, no. 9 (1991): 769. http://dx.doi.org/10.1049/el:19910478.

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19

Sergeyev, Sergey V. "Fast and slowly evolving vector solitons in mode-locked fibre lasers." Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences 372, no. 2027 (October 28, 2014): 20140006. http://dx.doi.org/10.1098/rsta.2014.0006.

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We report on a new vector model of an erbium-doped fibre laser mode locked with carbon nanotubes. This model goes beyond the limitations of the previously used models based on either coupled nonlinear Schrödinger or Ginzburg–Landau equations. Unlike the previous models, it accounts for the vector nature of the interaction between an optical field and an erbium-doped active medium, slow relaxation dynamics of erbium ions, linear birefringence in a fibre, linear and circular birefringence of a laser cavity caused by in-cavity polarization controller and light-induced anisotropy caused by elliptically polarized pump field. Interplay of aforementioned factors changes coherent coupling of two polarization modes at a long time scale and so results in a new family of vector solitons (VSs) with fast and slowly evolving states of polarization. The observed VSs can be of interest in secure communications, trapping and manipulation of atoms and nanoparticles, control of magnetization in data storage devices and many other areas.

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20

Chen, D. R., Z. W. Yu, S. Qin, and S. L. He. "Switchable dual-wavelength Raman erbium-doped fibre laser." Electronics Letters 42, no. 4 (2006): 202. http://dx.doi.org/10.1049/el:20064019.

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21

Rosolem, J. B., A. A. Juriollo, and M. A. Romero. "S-band EDFA using standard erbium-doped fibre." Electronics Letters 43, no. 22 (2007): 1186. http://dx.doi.org/10.1049/el:20072385.

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22

Millar, C. A., T. J. Whitley, and S. C. Fleming. "Thermal properties of an erbium-doped fibre amplifier." IEE Proceedings J Optoelectronics 137, no. 3 (1990): 155. http://dx.doi.org/10.1049/ip-j.1990.0027.

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23

Kim, J. S., C. Codemard, J. Nilsson, and J. K. Sahu. "Erbium-ytterbium co-doped hollow optical fibre laser." Electronics Letters 42, no. 9 (2006): 515. http://dx.doi.org/10.1049/el:20060186.

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24

Lees, G. P., M. J. Cole, and T. P. Newson. "Narrow linewidth, Q-switched erbium doped fibre laser." Electronics Letters 32, no. 14 (1996): 1299. http://dx.doi.org/10.1049/el:19960874.

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25

Li, Shenping, Hao Ding, and K. T. Chan. "Erbium-doped fibre lasers for dual wavelength operation." Electronics Letters 33, no. 1 (1997): 52. http://dx.doi.org/10.1049/el:19970001.

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26

Olshansky, R. "Noise figure for erbium-doped optical fibre amplifiers." Electronics Letters 24, no. 22 (1988): 1363. http://dx.doi.org/10.1049/el:19880933.

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27

Ainslie, B. J., K. J. Blow, A. S. Gouveia-neto, P. G. J. Wigley, A. S. B. Sombra, and J. R. Taylor. "Femtosecond soliton amplification in erbium doped silica fibre." Electronics Letters 26, no. 3 (1990): 186. http://dx.doi.org/10.1049/el:19900126.

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28

Bellemare, Antoine. "Continuous-wave silica-based erbium-doped fibre lasers." Progress in Quantum Electronics 27, no. 4 (January 2003): 211–66. http://dx.doi.org/10.1016/s0079-6727(02)00025-3.

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29

Kolegov, A. A., G. S. Sofienko, L. A. Minashina, and A. V. Bochkov. "Narrow-band erbium-doped fibre linear–ring laser." Quantum Electronics 44, no. 1 (January 31, 2014): 13–16. http://dx.doi.org/10.1070/qe2014v044n01abeh015281.

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30

Teyo, T. C., V. Sinivasagam, M. K. Abdullah, and H. Ahmad. "An injection-locked erbium-doped fibre ring laser." Optics & Laser Technology 31, no. 7 (October 1999): 493–96. http://dx.doi.org/10.1016/s0030-3992(99)00103-6.

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31

Jarabo, Sebastián. "Analytical theoretical model of erbium-doped fibre amplifiers." Optics Communications 181, no. 4-6 (July 2000): 303–11. http://dx.doi.org/10.1016/s0030-4018(00)00771-9.

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32

Greer, E. J., D. J. Lewis, and W. M. Macauley. "Polarisation dependent gain in erbium-doped fibre amplifiers." Electronics Letters 30, no. 1 (January 6, 1994): 46–47. http://dx.doi.org/10.1049/el:19940048.

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33

Davey, R. P., N. Langford, and A. I. Ferguson. "Subpicosecond pulse generation from erbium doped fibre laser." Electronics Letters 27, no. 9 (1991): 726. http://dx.doi.org/10.1049/el:19910451.

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34

Rühl, F. F. "Implicit analytical solution for erbium doped fibre amplifier." Electronics Letters 28, no. 5 (1992): 465. http://dx.doi.org/10.1049/el:19920293.

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35

Mori, A., Y. Ohishi, and S. Sudo. "Erbium-doped tellurite glass fibre laser and amplifier." Electronics Letters 33, no. 10 (1997): 863. http://dx.doi.org/10.1049/el:19970585.

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36

Singh, B. P. "Characteristics of regenerative erbium-doped fibre ring amplifier." Electronics Letters 36, no. 12 (2000): 1013. http://dx.doi.org/10.1049/el:20000736.

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37

Xia, G., Z. Wu, Y. Lin, J. Chen, and S. Tao. "A simple model of erbium-doped fibre amplifiers." Journal of Optics 29, no. 4 (August 1998): 298–301. http://dx.doi.org/10.1088/0150-536x/29/4/009.

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38

Mond, M., D. Albrecht, H. M. Kretschmann, E. Heumann, G. Huber, S. K�ck, V. I. Levchenko, et al. "Erbium Doped Fibre Amplifier Pumped Cr2+:ZnSe Laser." physica status solidi (a) 188, no. 4 (December 2001): R3—R5. http://dx.doi.org/10.1002/1521-396x(200112)188:43.0.co;2-i.

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39

Lester, Christian, Karsten Rottwitt, Jørn Hedegaard Povlsen, and Anders Bjarklev. "Raman effect in transparent distributed erbium-doped fibre." Optics Communications 106, no. 4-6 (March 1994): 183–86. http://dx.doi.org/10.1016/0030-4018(94)90318-2.

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40

Perry, I. R., A. C. Tropper, and J. R. M. Barr. "Micro-fluorescence profiling of erbium-doped fibre preforms." Journal of Luminescence 59, no. 1-2 (February 1994): 39–49. http://dx.doi.org/10.1016/0022-2313(94)90020-5.

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41

Frisken, S. J., C. A. Telford, R. A. Betts, and P. S. Atherton. "Passively mode-locked erbium-doped fibre laser with nonlinear fibre mirror." Electronics Letters 27, no. 10 (May 9, 1991): 887–89. http://dx.doi.org/10.1049/el:19910556.

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42

Dung, Jeng-Cherng, Sien Chi, and Senfar Wen. "Gain flattening of erbium-doped fibre amplifier using fibre Bragg gratings." Electronics Letters 34, no. 6 (1998): 555. http://dx.doi.org/10.1049/el:19980446.

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43

Krylov, A. A., A. V. Gladyshev, A. K. Senatorov, A. N. Kolyadin, A. F. Kosolapov, M. M. Khudyakov, M. E. Likhachev, and I. A. Bufetov. "1.56-to-2.84 μm SRS conversion of chirped pulses of a high-power erbium fibre laser in a methane-filled hollow-core revolver fibre." Quantum Electronics 52, no. 3 (March 1, 2022): 274–77. http://dx.doi.org/10.1070/qel18003.

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Abstract Single-cascade 1.56-to-2.84 μm SRS conversion is demonstrated in a hollow-core revolver fibre filled with methane at a pressure of 25 atm under pumping by positively chirped pulses of a high-power erbium-doped all-fibre laser. At a maximum pump pulse energy of 34 μJ (average power 3.74 W) and a pump pulse duration of about 260 ps, ultrashort pulses (USPs) with a duration of 110 ps and an energy of 1.33 μJ (average power 133 mW) are achieved at the centre wavelength of 2.84 μm. The gas fibre Raman lasers based on hollow-core fibres with pumping by high-power fibre sources are promising for producing all-fibre systems emitting USPs in the mid-IR range.

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44

Takada, K., T. Kitagawa, M. Shimizu, and M. Horiguchi. "High-sensitivity low coherence reflectometer using erbium-doped superfluorescent fibre source and erbium-doped power amplifier." Electronics Letters 29, no. 4 (1993): 365. http://dx.doi.org/10.1049/el:19930246.

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45

Ponosova, A. A., I. S. Azanova, N. K. Mironov, M. V. Yashkov, K. E. Riumkin, O. L. Kel', Yu O. Sharonova, and M. A. Melkumov. "Erbium-doped optical fibre with enhanced radiation resistance for superluminescent fibre sources." Quantum Electronics 49, no. 7 (July 15, 2019): 693–97. http://dx.doi.org/10.1070/qel16833.

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46

Patrick, H. J., A. D. Kersey, W. K. Burns, and R. P. Moeller. "Erbium-doped superfluorescent fibre source with long period fibre grating wavelength stabilisation." Electronics Letters 33, no. 24 (1997): 2061. http://dx.doi.org/10.1049/el:19971376.

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47

De Souza, K., D. O. Culverhouse, and T. P. Newson. "Dual-operation Q-switched erbium-doped fibre laser for distributed fibre sensing." Electronics Letters 33, no. 24 (1997): 2040. http://dx.doi.org/10.1049/el:19971391.

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48

Rahman, M. F. A., P. H. Reddy, A. Ahmad, A. A. Latiff, M. F. Baharom, and S. W. Harun. "Q-switched Ytterbium-doped fibre laser using an 8 cm long Hafnium bismuth erbium co-doped fibre saturable absorber." Journal of Physics: Conference Series 2075, no. 1 (October 1, 2021): 012020. http://dx.doi.org/10.1088/1742-6596/2075/1/012020.

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Abstract In this paper, we present a Q-switched fibre laser at 1069 nm which is induced by an 8 cm long Hafnium bismuth erbium co-doped fibre (HBEDF) saturable absorber (SA). The pulsating laser has a maximum repetition rate of 67 kHz at 175 mW pump power. We obtained the narrowest pulse width of 3.48 μs, the maximum pulse energy of 70.2 nJ, the maximum output power of 4.7 mW and the maximum peak power of 20.1 mW. The Q-switched laser is simple and may found practical applications in medicine and remote sensing.

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49

Sulaiman, A., M. Muhammad, H. Ahmad, and S. Harun. "Erbium-doped fibre ring laser based on microfibre coupler." Ukrainian Journal of Physical Optics 14, no. 4 (2013): 196. http://dx.doi.org/10.3116/16091833/14/4/196/2013.

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50

Xin-Huan, Feng, Liu Yan-Ge, Sun Lei, Yuan Shu-Zhong, Kai Gui-Yun, and Dong Xiao-Yi. "A Polarization Controlled Switchable Multiwavelength Erbium-Doped Fibre Laser." Chinese Physics Letters 21, no. 4 (March 17, 2004): 659–61. http://dx.doi.org/10.1088/0256-307x/21/4/019.

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