Abstract
We present a 2.2 GHz modulated, 1.27 kW output power, monolithic fiber amplifier based on pseudo-random binary sequence (PRBS) phase modulation. The spectral line spacing of maximizing the threshold enhancement factor (plateau of trend) was found by theoretical simulation. The spectral line spacing was adjusted to 12.7 MHz by a pattern length of n = 9, which is close to the plateau of trend in the proposed architecture. A 2.2 GHz low-pass radio frequency filter was used to control the FWHM of the seed. A four-stage Yb-doped fiber amplifier chain was established to boost a distributed Bragg reflector (DBR) laser and a distributed feedback (DFB) diode laser to 1.2 kW and 1.27 kW with a backward reflectively of <1‰, which shows a good suppression of SBS effect.
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Introduction
Stimulated Brillouin scattering (SBS) is one of the leading nonlinear impairments in high-power narrow-linewidth continuous-wave (CW) fiber amplifiers1. In SBS process, optical power is transferred from the signal light and into the backscattered Stokes light2. Sufficiently high optical power initiates backscattered pulsation, which can severe damage the fiber amplifier. In order to suppress SBS and achieve higher laser power, phase modulation techniques have been implemented by fiber-coupled LiNbO3 electro-optic modulators. Phase modulation techniques include driving the phase modulator with a sine wave3, a flat-top spectrum radio frequency (RF) signal4,5, or a white noise source (WNS)6 etc. Among these linewidth broadening methods, >20 GHz linewidth can be generally obtained. Unfortunately, such linewidth may cause harmful effects for many fields, such as the beam quality degradation in spectral beam combining due to dispersion. To further suppress SBS at a much narrow level, a PRBS phase modulation technique has been theoretically and experimentally studied7,8. The advantage of PRBS has been proven in the long-distance optical communication systems9. PRBS generates an equally spaced discrete optical power spectral density, and the spectral line spacing is a function of the modulation frequency and pattern length, which can make the spectral line spacing adjustment flexible10. In the narrow linewidth fiber amplifier configuration, a proper spectral line spacing improves the SBS suppression for a given linewidth11. When the spectral line spacing is large enough, each discrete spectral component separately seeds the SBS process likes sine-wave modulation format12, and the SBS threshold is determined by the component with the highest spectral power. As the spectral line spacing is reduced, the greater overlap between the gain spectra of adjacent lines, and the concomitant enhancement of cross-interactions is demonstrated11. For a given linewidth, the number of spectral line is inversely proportional to the spectral line spacing. Enhancement of the SBS threshold cannot be achieved by simply increasing the number of spectral line. Therefore, exploring the proper spectral line spacing is key points to further scale laser power at a much narrow linewidth.
In this paper, we applied PRBS phase modulation with a 2.2 GHz low-pass RF filter to control the longitudinal mode spacing of the single frequency master oscillator, aimed to equilibrate spectral homogenization and Brillouin gain-spectrum overlap in the narrow linewidth fiber amplifier. The spectral line spacing of the phase modulated seed is chosen to be 12.7 MHz, which approach the plateau of the SBS threshold. A four-stage, 1.2 kW monolithic fiber amplifier is proposed by using a 7 m-long non-polarization maintaining 20/400 μm Yb-doped fiber, which is used to boost a DFB diode laser and a DBR fiber laser to 1.27 kW and 1.2 kW, respectively. The backward reflectively is measured to be <1‰. To the best of our knowledge, this is the highest power level for narrow linewidth fiber amplifier based on phase control under 5 GHz spectral linewidth.
Results
We established a PRBS modulated, low pass filtered, kilowatt-class, monolithic fiber amplifier. The proposed architecture is shown in Fig. 1. Reflectivity versus output power with DBR and DFB laser seed are shown in Fig. 2(a). As shown, signal power of 1.27 kW and 1.2 kW were attained at DFB and DBR laser seeding with near diffraction-limited beam quality (M2 < 1.2), respectively. In both cases, the reflectivity was much less than 1‰ of the previous amplifiers1,13,14, there is potential room for further power scaling. This work demonstrates the highest output power in <5 GHz regime based on phase-modulated approach. The DFB diode laser seed provided superior SBS suppression (lower reflectivity) in the same amplifier. Figure 2(c) shows that a characteristic of relative intensity of backward Rayleigh and Stokes light was utilized to identify the SBS threshold (with the former lower ~3 dB) in our experiment. The DFB laser-seeded amplifier obtained a weaker backward Stokes light than Rayleigh light at pump full power output as plotted in Fig. 2(d). The forward spectral content for fiber amplifier configurations were measured as shown in Fig. 2(e,f), the DBR laser-seeded amplifier provided an ASE suppression of more than 40 dB at full power output, while the DFB laser-seeded amplifier was characterized by an obviously ASE noise. The single frequency threshold of ~24 W was measured by using the same SBS threshold criterion, and the enhancement factor of ~53 was attained at maximum power in our experiment.
A 1.2 kW four-stage fiber amplifier was used to explore proper spectral line spacing under PRBS modulation. The self-heterodyne technique15 was applied to characterize the Brillouin gain spectrum, and the measured spectral data of the amplifier were fitted with a Lorentzian lineshape to be a FWHM bandwidth of ~23.2 MHz, which is shown in Fig. 3. The estimated result of the Brillouin gain spectrum bandwidth is expectedly less than the Brillouin spontaneous bandwidth (~40–50 MHz) due to gain narrowing1,7. Figure 6(b) compares the measurement results of the amplifier SBS threshold when PRBS signal generator at eleven different spectral line spacings. The SBS threshold increases as the spectral line spacing decreases due to the spectral homogenization as presented in Fig. 7, and the saturation characteristic is reached when the spectral line spacing is reduced to about 10 MHz.
Discussion
A triply coupled, set of nonlinear partial differential equations can be used to characterize the evolution of laser fields in the SBS suppression system4,11,16. In these equations, optical fibers are seeded with phase-modulated light, and the three-wave interaction among the pump (AL), the Stokes (AS), and acoustic (ρ) fields is described as following:
here γe is the electrostrictive constant, ГB is the Brillouin bandwidth, ΩB is the resonant acoustic frequency, c is the speed of light, n is the refractive index of fiber, ω is the optical frequency (ω ≈ ωL ≈ ωS), ωL is the frequency of the pump light, which is the signal light of amplifier, ωS is the frequency of the Stokes light, ρ0 is the mean density of the fiber medium, ε0 is the vacuum permittivity, and f is a Gaussian random variable which initiates SBS. These equations can be solved via the initial conditions of the phase modulated pump wave7,11,12. When the optical spectrum of the pump laser is modulated to generate a series of equidistant spectral lines, the effective Brillouin gain Geff is expressed as17
where Leff is the effective length of the fiber; g0 = γe2ω2/ρ0nc3νSГB; ωL,j = ωL,0 + jΔυ, ωS,j = ωS,0 + jΔυ; ωL,0 is the central frequency of the pump light, Ωa is the frequency of the acoustic wave resonant with the laser mode oscillating at ωL,0; IL,m is the intensity of the pump light. The phase modulation is implemented by using a PRBS signal to drive the electro-optic modulator. The spectral line spacing depends on modulation frequency and pattern length,
where, υpm is the modulation frequency of PRBS, n is the pattern length. The spectrum of PRBS presents sinc2-function envelope and the linewidth of the pump laser is determined by the modulation frequency7. Based on Eq. (5) continuously adjusting the spectral line spacing can only be achieved by controlling the modulation frequency of PRBS signal generator. Therefore, a special spectral line spacing and a narrow pump linewidth becomes a dilemma due to the correlation of the modulation frequency of the unfiltered PRBS RF signal. One attractive approach to manipulate pump linewidth is to filter the PRBS signal with a low-pass filter. In Fig. 4(a), the modulated pump linewidth is determined by the bandwidth of the low-pass filter (ΔυF). The spectrum of modulated pump laser presents a frequency comb with the envelope of
where A is the modulation coefficient. Substituting Eq. (6) to Eq. (4), the Brillouin gain modulated by PRBS is
where N is equal to ΔυF/2Δυ. The intensity distribution of optical modes has been normalized, the Geff is a convolution of the laser spectrum and the spontaneous Brillouin linewidth12. Therefore, a certain value of n can be found to derive a maximum Brillouin gain
Generating the strongest Stokes light, the maximum Brillouin gain determines the SBS threshold. Consequently, the SBS threshold enhancement factor can be expressed by
where Geff, 0 = 2g0Leff/ГB is the Brillouin gain of a single-frequency pump laser12.
In order to calculate the SBS threshold enhancement factor based on Eq. (9), we measured the Brillouin gain spectrum of the fiber amplifier, as drawn in Fig. 3. The normalized enhancement factors were simulated with ГB = 1.46 × 108 rad/s (corresponds to Brillouin gain bandwidth of 23.2 MHz), ΔυF = 2.2 GHz, and υpm = 6.5 GHz. Subsequently, the Brillouin gain bandwidth was expanded to different bandwidths varying from 10 MHz to 60 MHz is shown in Fig. 5. As is shown, the threshold enhancement factor is in an inverse proportion to the spectral line spacing and appears to a saturation character, and there is a strong dependence on the Brillouin gain bandwidth for the saturation values and the plateaus (maximizing threshold enhancement factor). For a given linewidth, the number of spectral line (N) is inversely proportional to the spectral line spacing, as shown in Fig. 4(a). More spectral lines make the optical spectral shape homogeneous as presented in Fig. 7, which will improve the SBS threshold. When the spectral line spacing is further reduced, the convolution of the Brillouin gain spectrum and the spectral line is increased according to the number of the spectral line N in the Eq. (9), which ultimately offsets the threshold enhancement caused by spectral homogenization and reaches plateau. Thus, a certain spectral line spacing can be found to maximize threshold enhancement factor. Simultaneously, a large Brillouin gain bandwidth causes the plateau occur at a large spectral line spacing due to the extension in the overlap range.
Based on the above analysis, we simulated the normalized enhancement factor for different filter bandwidths varying from 1 GHz to 5 GHz, as plotted in Fig. 6(a). The Brillouin gain bandwidth and PRBS modulation frequency were maintained at 23.2 MHz and 6.5 GHz, respectively. As is shown, the saturation values have a strong dependence on the filter bandwidth, and there is an apparent irrelevance in the filter bandwidth for the plateaus. A wider filter bandwidth transmits more spectral lines with a same spectral line spacing, which more effectively homogenizes the spectrum and enhances the SBS threshold. For different filter bandwidths, the overlap range of the Brillouin gain spectrum and the spectral line almost stays a constant since the Brillouin gain bandwidth is much smaller than the filter bandwidth, as shown in Fig. 7. In this case, the spectral line spacing of the plateaus is also constant. Based on 1.2 kW four-stage monolithic fiber amplifier shown in Fig. 1, we measured the SBS thresholds in the case of 2.2 GHz filter bandwidth, and compared with the simulated data in Fig. 6(b). In our experiment, the intensity of the separated spectral line was controlled to be nearly the same level. The SBS threshold decline trend represent good agreement with the simulation. When the spectral line spacing was reduced to about 10 MHz, the SBS threshold slightly fluctuated with varying the spectral line spacing. This result adjacent to the estimate (9.6 MHz) of the plateau in Fig. 6(a). Similar results had been demonstrated in4,11.
We chose a spectral line spacing (12.7 MHz) close to the plateau to modulate DFB diode laser and DBR laser seeds, respectively. Due to the inherent current noise, the linewidth of DFB laser is generally wider than that of DBR laser18,19. The spectrum of DFB laser is broadened relative to DBR laser. For current noise broadened DFB laser with a linewidth less than the spectral line spacing, the spectral broadening resulting from PRBS phase modulation and current noise is independent of each other. This is expected, a more homogenous spectrum will be obtained by driving two spectral broadening mechanisms, while the SBS threshold is also enhanced. As is shown in Fig. 2, the SBS threshold was further enhanced when the amplifier was seeded with a DFB laser. However, significant ASE was observed with 1082 nm DFB diode laser wavelength due to the strong emission cross section of the Yb-doped fiber around 1070 nm.
Methods
The schematic diagram of PRBS modulated, low pass filtered, Yb-doped monolithic fiber amplifier is shown in Fig. 1. DFB diode laser (1075 nm) and DBR laser (1082 nm) were used to seed the amplifier, respectively. A PRBS generator and a low-pass RF filter served to generate pseudo-random binary sequence signal of a specific bandwidth and arbitrary spectral line spacing. Subsequently, RF signals were magnified by a ~25 dB RF amplifier. The effective linewidth of the seed was broadened via a fiber-coupled LiNbO3 electro-optic modulator. Thereafter, a third-stages amplifier was implemented to amplify the broadened seed to ~12 W. In the main amplifier stage, six 300 W (976 nm) fiber-coupled laser diodes were combined by a (6 + 1) × 1 pump/signal combiner, a 7 m-long non-polarization maintaining 20/400 μm Yb-doped fiber (manufactured by nLight) was utilized to be the gain medium. A high power cladding stripper (CPS) was installed to eliminate the redundant light in the cladding. At the amplifier output, the pigtail fiber was cleared to 8° to avoid unexpected end reflection. The circulator was applied between pre amplifier stage and main amplifier stage to protect the preceding stage and monitor backward scatting light. Different spectral line spacings were implemented while maintaining the filter bandwidth of 2.2 GHz. For each spectral line spacings, the intensity of each phase modulated signal was maintained to be the same level as drawn in Fig. 4(b,c). The seed was amplified to 1.2 kW by driving a phase modulated signal with modulation frequency of 6.5 GHz and pattern length of 9, the modulation linewidth of the modulated signal was limited by a low-pass RF filter with 3 dB bandwidth of 2.2 GHz.
The single-frequency laser (1075 nm) operated in the amplifier without phase modulation in order to measure single-frequency SBS threshold. The output power of amplifier was measured through 1.5 kW range thermal power meter. A 5 W range integrating sphere power meter was used to measure the power of backward scatting light. The spectral content of forward light and backward scatting light was sampled utilizing an optical spectrum analyzer (OSA) of 0.02 nm resolution bandwidth. The spectrum of the phase modulated signal was measured through a wideband (10 Hz to 26.5 GHz) spectrum analyzer (KEYSIGHT N9020A), a 5 dB coaxial attenuator was placed at the input of the spectrum analyzer for overpower protection. The beam quality of the output power at 1 kW was measured by the LQM-20 (@PRIMES Corporation) using four-sigma method. The temperature of the fiber amplifier system was maintained at 20 °C by water cooler, at the same time, the temperature of the high power CPS was kept within 60 °C by a dedicated water cooler.
References
Flores, A., Robin, C., Lanari, A. & Dajani, I. Pseudo-random binary sequence phase modulation for narrow linewidth, kilowatt, monolithic fiber amplifiers. Opt Express 22, 17735–17744 (2014).
Cui, J. W. et al. Stimulated Brillouin scattering evolution and suppression in an integrated stimulated thermal Rayleigh scattering-based fiber laser. Photonics Res 5, 233–238 (2017).
Liu., Y. K. et al. >1 kW all-fiberized narrow-linewidth polarization-maintained fiber amplifiers with wavelength spanning from 1065 to 1090 nm. Appl Optics 56, 4213–4218 (2017).
Anderson, B. M., Hui, R. Q., Flores, A. & Dajani, I. SBS suppression and coherence properties of a flat top optical spectrum in a high power fiber amplifier. In Fiber Lasers Xiv: Technology and Systems 10083, 100830V-1-100830V-8 (2017).
Harish, A. V. & Nilsson, J. Optimization of phase modulation with arbitrary waveform generators for optical spectral control and suppression of stimulated Brillouin scattering. Opt Express 23, 6988–6999 (2015).
Khitrov, V. et al. Kw level narrow linewidth Yb fiber amplifiers for beam combining. In Laser Technology for Defense and Security Vi 7686, 76860A-1 - 76860A-8 (2010).
Robin, C. et al. Pseudo-random binary sequence phase modulation in high power Yb-doped fiber amplifiers. In Fiber Lasers X: Technology, Systems, and Applications 8601, 86010Z-1-86010Z-9 (2013).
White, J. O., Young, J. T., Wei, C. L., Hu, J. & Menyuk, C. R. Seeding fiber amplifiers with piecewise parabolic phase modulation for high SBS thresholds and compact spectra. Opt Express 27, 2962–2974 (2019).
Aoki, Y., Tajima, K. & Mito, I. Input power limits of single-mode optical fibers due to stimulated brillouin-scattering in optical communication-systems. J Lightwave Technol 6, 710–719 (1988).
Anderson, B., Flores, A., Holten, R. & Dajani, I. Comparison of phase modulation schemes for coherently combined fiber amplifiers. Opt Express 23, 27046–27060 (2015).
Harish, A. V. & Nilsson, J. Optimization of Phase Modulation Formats for Suppression of Stimulated Brillouin Scattering in Optical Fibers. IEEE Journal of Selected Topics in Quantum Electronics 24, 10 (2018).
Zeringue, C., Dajani, I., Naderi, S., Moore, G. T. & Robin, C. A theoretical study of transient stimulated Brillouin scattering in optical fibers seeded with phase-modulated light. Opt Express 20, 21196–21213 (2012).
Naderi, N. A., Flores, A., Anderson, B. M. & Dajani, I. Beam combinable, kilowatt, all-fiber amplifier based on phase-modulated laser gain competition. Opt Lett 41, 3964–3967 (2016).
Naderi, N. A., Dajani, I. & Flores, A. High-efficiency, kilowatt 1034 nm all-fiber amplifier operating at 11 pm linewidth. Opt Lett 41, 1018–1021 (2016).
Hofstetter, R., Schmuck, H. & Heidemann, R. Dispersion effects in optical millimeter-wave systems using self-heterodyne method for transport and generation. IEEE Transactions on Microwave Theory and Techniques 43, 2263–2269 (1995).
Anderson, B. M., Flores, A. & Dajani, I. Filtered pseudo random modulated fiber amplifier with enhanced coherence and nonlinear suppression. Opt Express 25, 17671–17682 (2017).
Lichtman, E., Waarts, R. G. & Friesem, A. A. Stimulated brillouin-scattering excited by a modulated pump wave in single-mode fibers. J Lightwave Technol 7, 171–174 (1989).
Cook, A. L. & Hendricks, H. D. Characteristics of linewidth-narrowed distributed-bragg-reflector laser with a fiber external-cavity formed with the vertical grating emission. J Lightwave Technol 13, 356–363 (1995).
Kimura, T. & Sugimura, A. Linewth reduction by coupled phase-shift distributed-feedback lasers. Electron. Lett. 23, 1014–1015 (1987).
Acknowledgements
This work was supported in part by the National Natural Science Foundation of China (61805261, 61705243, 61735007); The Program of Shanghai Technology Research Leader (17XD1424800); The Shanghai Sailing Programme (17YF1421200); The Shanghai Military and Military Integration Project (MRH-2018-1013).
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B.H., Jun. Z. and Yifeng. Y. conceived the project; M.L., Jingpu. Z., H.W. and Yifeng. Y. designed the experiments; M.L., L.Y., Yang. Y., G.B., X.Z. and H.S. performed the experiments and analyzed the data; M.L. wrote the main manuscript text; all authors reviewed the manuscript.
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Liu, M., Yang, Y., Shen, H. et al. 1.27 kW, 2.2 GHz pseudo-random binary sequence phase modulated fiber amplifier with Brillouin gain-spectrum overlap. Sci Rep 10, 629 (2020). https://doi.org/10.1038/s41598-019-57408-5
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DOI: https://doi.org/10.1038/s41598-019-57408-5
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