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专业英语论文

Recent Progress in Brillouin Scattering Based Fiber Sensors

Abstract:This review paper is an attempt to summarize the evolution of the distributed sensor based on Brillouin scattering, and the milestones of the distributed sensor in terms of sensing range, spatial resolution, and temperature/strain resolutions, so that readers will have a glimpse of the advantages, limitations and realized potential of this technology. Keywords: Fiber optic sensors; Brillouin scattering; Polarization mode dispersion; Strain; Temperature;

1 FDM-Based BOTDA

One approach to increase the sensing length is to use non-uniform fibers, which were originally proposed for SBS slow light applications to reduce pulse distortion1. The effective fiber length2 will be reduced to the resonant Brillouin frequency section, rather than the entire sensing length. So that, the limitation of the sensing length is the fiber loss instead of the Brillouin gain saturation. The trade-off is the larger scan range, as different fiber sections represent different Brillouin frequency shifts. The choice of the fiber types and their order along the entire sensing length are critical in obt aining the highest SNR and the longest sensing length.

The following table gives the parameters of the three types of fibers used in the experiment.

Figure 1 shows a 75 km optical fiber strain measuring usage. Through two waveforms similar pulse width can reach 1.1 meters Brillouin spectrum fitting, given the uncertainty of a Brillouin frequency shift of 1 MHz spatial resolution is 1℃temperature resolution and 17μεstrain resolution3.

Conclusion:

The performance of FDM-BOTDA is even higher than TDM-BOTDA, because different Brillouin frequencies in different fiber sections have reduced Brillouin interaction length, and hence lower the impact of SPM. The Brillouin gain of the pump signal at different sections cannot be added as in TDM-BOTDA, where the fiber is the same along the entire sensing length.

2 Combining Brillouin Gain and Loss

If the DPP-BOTDA measurement4time is doubled, it can significantly improve the spatial resolution by optical parametric amplification differential5, based on Brillouin gain6and loss of the coherent interaction7, we explore a single differential measurement and realization Bridgend a method for deep gain. In the frequency domain analysis, the Brillouin gain and loss of interaction can be used to reduce the influence of the optical pumping8. We are not using two continuous-wave performance Brillouin gain and loss process. On the other hand, ODPA-BOTDA sensor9signal directly and ODPA-BOTDA sensor detects the signal differences. Thus, the detector may even have a longer length in the sensing ODPA-BOTDA sensor. Due to large-scale application of pulse Brillouin gains and losses in the process, this process remains low saturation ODPA gain, low-loss loss, therefore, the sensor length may exceed the normal BOTDA sensor.

《专业英语》研究生课程论文

These figures show the binding of the Brillouin gain and loss in the process, double pulse Stokes and anti-Stokes width 20/15 ns results in different waves. This is reflected in the signal from 10% to 90% of the peak value of the time, results in a spatial resolution of about 0.5 m, is much smaller than the spatial resolution of 2 m and a 20 ns pulse sensor. Because the Brillouin gain increased acoustic wave generating process is very slow, 5 nanosecond pulse in BOTDA sensor can only get a very small Brillouin gain. However, in the optical fiber 20/15 ns pulses can interact longer, two acoustic waves

《专业英语》研究生课程论文

can build up greater differential gain10.

3 The Brillouin Grating as a Point Sensor

Figure 4 shows the grating by Brillouin frequency shift and Brillouin frequency difference form a double pump waves. Figure 2 illustrates the spectral width of the Brillouin scattering grating. In the X-axis, double-pump pulse generating raster TP1 and TP211.

Figure 5 direct proof, moving and stationary Brillouin optical fiber gratings, fiber Bragg grating follow the same basic theory12. Another important feature of the Brillouin scattering grating or grating sound wave attenuation relaxation. Brillouin grating by electrostrictive effect can only rely on the creation of dual pump pulse is maintained13.

《专业英语》研究生课程论文

4.Advantages and disadvantages

1.Brillouin peak frequency measurements. Polarization scrambler special introduction of the price gain to eliminate polarization dependence and at least 1 MHz peak Brillouin frequency measurement uncertainty, further raising the temperature and strain accuracy requirements of new technologies.

2.Remote Sensing of dynamic measurement speed and centimeter spatial resolution long length.

3.In order to make cost-effective distributed sensing system should explore new measurement parameters, in particular chemical or biological relevant monitoring option can be very attractive.

参考文献:

1 Kalosha, V., Chen, L. & Bao, X. Slow light of subnanosecond pulses via stimulated Brillouin scattering in nonuniform fibers.

Physical Review A75, 021802 (2007).

2 Li, W., Bao, X., Kalosha, V., Chen, L. & Li, M.-J. Using nonuniform fiber to generate slow light via SBS. International

Journal of Optics2008 (2008).

3 Dong, Y., Chen, L. & Bao, X. High-spatial-resolution time-domain simultaneous strain and temperature sensor using Brillouin

scattering and birefringence in a polarization-maintaining fiber. Photonics Technology Letters, IEEE22, 1364-1366 (2010).

4 Horiguchi, T. & Tateda, M. Optical-fiber-attenuation investigation using stimulated Brillouin scattering between a pulse and a

continuous wave. Optics Letters14, 408-410 (1989).

5 Kurashima, T., Horiguchi, T. & Tateda, M. Distributed-temperature sensing using stimulated Brillouin scattering in optical

silica fibers. Optics Letters15, 1038-1040 (1990).

6 Bao, X., Webb, D. J. & Jackson, D. A. 22-km distributed temperature sensor using Brillouin gain in an optical fiber. Optics

letters18, 552-554 (1993).

7 Bao, X., Dhliwayo, J., Heron, N., Webb, D. J. & Jackson, D. A. Experimental and theoretical studies o n a distributed

temperature sensor based on Brillouin scattering. Lightwave Technology, Journal of13, 1340-1348 (1995).

8 Tateda, M., Horiguchi, T., Kurashima, T. & Ishihara, K. First measurement of strain distribution along field-installed optical

fibers using Brillouin spectroscopy. Lightwave Technology, Journal of8, 1269-1272 (1990).

9 Horiguchi, T., Kurashima, T. & Tateda, M. Tensile strain dependence of Brillouin frequency shift in silica optical fibers.

Photonics Technology Letters, IEEE1, 107-108 (1989).

10 Horiguchi, T., Kurashima, T., Tateda, M., Ishihara, K. & Wakui, Y. Brillouin characterization of fiber strain in bent slot-type

optical-fiber cables. Lightwave Technology, Journal of10, 1196-1201 (1992).

11 Erdogan, T. Fiber grating spectra. Lightwave Technology, Journal of15, 1277-1294 (1997).

12 Song, K. Y. & Yoon, H. J. Observation of narrowband intrinsic spectra of Brillouin dynamic gratings. Optics letters35,

2958-2960 (2010).

13 Dong, Y., Chen, L. & Bao, X. Characterization of the Brillouin grating spectra in a polarization-maintaining fiber. Optics

express18, 18960-18967 (2010).

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