Abstract

Stimulated Brillouin scattering in optical fibers can be used to measure strain or temperature in a distributed manner. Brillouin optical time domain analysis (BOTDA) is the most common sensor system based on the Brillouin scattering. To improve the spatial resolution of these measurements, shorter pulses must be used, resulting in reduced signal powers causing a decrease of the dynamic range. In this paper, a double-pulse technique was proposed to enhance the spatial resolution of BOTDA. Experimental results showed that the ability to resolve two adjacent events could be enhanced, about twice, by using a double-pulsed pump light without decreases in the dynamic range.

©2004 Optical Society of America

Full Article  |  PDF Article
OSA Recommended Articles
Efficient dynamic events discrimination technique for fiber distributed Brillouin sensors

Carlos A. Galindez, Francisco J. Madruga, and Jose M. Lopez-Higuera
Opt. Express 19(20) 18917-18926 (2011)

Pulse width dependence of Brillouin frequency in single mode optical fibers

Seok-Beom Cho, Young-Gyu Kim, Jin-Seok Heo, and Jung-Ju Lee
Opt. Express 13(23) 9472-9479 (2005)

Monitoring the propagation of mechanical waves using an optical fiber distributed and dynamic strain sensor based on BOTDA

Yair Peled, Avi Motil, Iddo Kressel, and Moshe Tur
Opt. Express 21(9) 10697-10705 (2013)

More Recommended Articles

References

  • View by:
  • Article Order
  • |
  • Year
  • |
  • Author
  • |
  • Publication
  1. B. Culshaw and J. P. Dakin, Eds., Optical Fiber Sensors (Boston, London, Artech House, 1989), I and II.
  2. M. K. Barnoski and S. M. Jensen, “Fiber waveguides: A novel technique for investigating attenuation characteristics,” Appl. Opt. 15, 2112–2115, (1976).
    [Crossref] [PubMed]
  3. T. Horiguchi and M. Tateda, “Optical fiber attenuation investigation using stimulated Brillouin scattering between a pulse and a continuous wave,” Opt. Lett. 14, 408–410, (1989).
    [Crossref] [PubMed]
  4. T. Horiguchi and M. Tateda, “BOTDA-Nondestructive measurement of single-mode optical fiber attenuation characteristics using Brillouin interaction: Theory,” J. Lightwave Technol. 7, 1170–1176 (1989).
    [Crossref]
  5. W. Kaiser and M. Maier, “Stimuilated Rayleigh, Brillouin and Raman Sectroscopy,” in Laser Handbook, F. T. Arecchi and E. O. Schulz-Dubois, eds. (North-Holland, 1972),  2, 1077–1150.
  6. G. P. Agrawal, Nonlinear Fiber Optics, (Academic Press, Boston, 1989), chap. 9.
  7. M. Niklès, L. Thévenaz, and P. A. Robert, “Brillouin gain spectrim characterization in single-mode optical fibers,” J. Lightwave Technol. 15, 1842–1851 (1997).
    [Crossref]

1997 (1)

M. Niklès, L. Thévenaz, and P. A. Robert, “Brillouin gain spectrim characterization in single-mode optical fibers,” J. Lightwave Technol. 15, 1842–1851 (1997).
[Crossref]

1989 (2)

T. Horiguchi and M. Tateda, “Optical fiber attenuation investigation using stimulated Brillouin scattering between a pulse and a continuous wave,” Opt. Lett. 14, 408–410, (1989).
[Crossref] [PubMed]

T. Horiguchi and M. Tateda, “BOTDA-Nondestructive measurement of single-mode optical fiber attenuation characteristics using Brillouin interaction: Theory,” J. Lightwave Technol. 7, 1170–1176 (1989).
[Crossref]

1976 (1)

1972 (1)

W. Kaiser and M. Maier, “Stimuilated Rayleigh, Brillouin and Raman Sectroscopy,” in Laser Handbook, F. T. Arecchi and E. O. Schulz-Dubois, eds. (North-Holland, 1972),  2, 1077–1150.

Agrawal, G. P.

G. P. Agrawal, Nonlinear Fiber Optics, (Academic Press, Boston, 1989), chap. 9.

Barnoski, M. K.

Horiguchi, T.

T. Horiguchi and M. Tateda, “BOTDA-Nondestructive measurement of single-mode optical fiber attenuation characteristics using Brillouin interaction: Theory,” J. Lightwave Technol. 7, 1170–1176 (1989).
[Crossref]

T. Horiguchi and M. Tateda, “Optical fiber attenuation investigation using stimulated Brillouin scattering between a pulse and a continuous wave,” Opt. Lett. 14, 408–410, (1989).
[Crossref] [PubMed]

Jensen, S. M.

Kaiser, W.

W. Kaiser and M. Maier, “Stimuilated Rayleigh, Brillouin and Raman Sectroscopy,” in Laser Handbook, F. T. Arecchi and E. O. Schulz-Dubois, eds. (North-Holland, 1972),  2, 1077–1150.

Maier, M.

W. Kaiser and M. Maier, “Stimuilated Rayleigh, Brillouin and Raman Sectroscopy,” in Laser Handbook, F. T. Arecchi and E. O. Schulz-Dubois, eds. (North-Holland, 1972),  2, 1077–1150.

Niklès, M.

M. Niklès, L. Thévenaz, and P. A. Robert, “Brillouin gain spectrim characterization in single-mode optical fibers,” J. Lightwave Technol. 15, 1842–1851 (1997).
[Crossref]

Robert, P. A.

M. Niklès, L. Thévenaz, and P. A. Robert, “Brillouin gain spectrim characterization in single-mode optical fibers,” J. Lightwave Technol. 15, 1842–1851 (1997).
[Crossref]

Tateda, M.

T. Horiguchi and M. Tateda, “Optical fiber attenuation investigation using stimulated Brillouin scattering between a pulse and a continuous wave,” Opt. Lett. 14, 408–410, (1989).
[Crossref] [PubMed]

T. Horiguchi and M. Tateda, “BOTDA-Nondestructive measurement of single-mode optical fiber attenuation characteristics using Brillouin interaction: Theory,” J. Lightwave Technol. 7, 1170–1176 (1989).
[Crossref]

Thévenaz, L.

M. Niklès, L. Thévenaz, and P. A. Robert, “Brillouin gain spectrim characterization in single-mode optical fibers,” J. Lightwave Technol. 15, 1842–1851 (1997).
[Crossref]

Appl. Opt. (1)

J. Lightwave Technol. (2)

T. Horiguchi and M. Tateda, “BOTDA-Nondestructive measurement of single-mode optical fiber attenuation characteristics using Brillouin interaction: Theory,” J. Lightwave Technol. 7, 1170–1176 (1989).
[Crossref]

M. Niklès, L. Thévenaz, and P. A. Robert, “Brillouin gain spectrim characterization in single-mode optical fibers,” J. Lightwave Technol. 15, 1842–1851 (1997).
[Crossref]

Opt. Lett. (1)

Other (3)

B. Culshaw and J. P. Dakin, Eds., Optical Fiber Sensors (Boston, London, Artech House, 1989), I and II.

W. Kaiser and M. Maier, “Stimuilated Rayleigh, Brillouin and Raman Sectroscopy,” in Laser Handbook, F. T. Arecchi and E. O. Schulz-Dubois, eds. (North-Holland, 1972),  2, 1077–1150.

G. P. Agrawal, Nonlinear Fiber Optics, (Academic Press, Boston, 1989), chap. 9.

Cited By

OSA participates in Crossref's Cited-By Linking service. Citing articles from OSA journals and other participating publishers are listed here.

Alert me when this article is cited.


Figures (10)

Fig. 1.
Fig. 1. Locations of a single pulse (left) and its corresponding scattering power (right) at fixed frequency modulation of probe light.

Download Full Size | PPT Slide | PDF

Fig. 2.
Fig. 2. Locations of a double-pulse (left) and its corresponding scattering power (right) at fixed frequency modulation of probe light.

Download Full Size | PPT Slide | PDF

Fig. 3.
Fig. 3. Experimental setup for Brillouin gain spectrum measurements. (ISO = isolator, PC = polarization controller, PS = polarization scrambler, DET = detector, ATT = attenuator, CIR = circulator.)

Download Full Size | PPT Slide | PDF

Fig. 4.
Fig. 4. Configuration of the fiber under test. (section 1 and section 3: strained sections, section 2: free fiber section.)

Download Full Size | PPT Slide | PDF

Fig. 5.
Fig. 5. BGS of 80 ns single pulse (left) and BGS’s of single pulses (right) at the position of 1800 m

Download Full Size | PPT Slide | PDF

Fig. 6.
Fig. 6. BGS’s of single and double-pulses. (S: single pulse, D: double-pulse, D_A-B ns: A = pulse width, B = separation width)

Download Full Size | PPT Slide | PDF

Fig. 7
Fig. 7 Normalized backscattering power of 80 ns single pulse (left) and 40-20 ns double-pulse (right) along the fiber. (with 2 m strained fiber section.)

Download Full Size | PPT Slide | PDF

Fig. 8
Fig. 8 Normalized backscattering power of 80 ns single pulse (left) and 40-20 ns double-pulse (right) along the fiber. (section 1 and section 3 = 2 m, section 2 = 2 m.)

Download Full Size | PPT Slide | PDF

Fig. 9.
Fig. 9. Normalized backscattering power of 80 ns single pulse (left) and 40-20 ns double-pulse (right) along the fiber. (section 1 and section 3 = 2 m, section 2 = 4 m.)

Download Full Size | PPT Slide | PDF

Fig. 10.
Fig. 10. BGS’s of single and double-pulses. (S: single pulse, D: double-pulse, D_A-B ns: A = pulse width, B = separation width)

Download Full Size | PPT Slide | PDF

Equations (3)

Equations on this page are rendered with MathJax. Learn more.

ν B = 2 n V a λ p
g B ( ν ) = g B ( ν B ) ( Δ ν B 2 ) 2 ( ν − ν B ) 2 + ( Δ ν B 2 ) 2
g B ( ν B ) = g 0 = 2 π n 7 p 12 2 c λ p 2 ρ 0 V a Δ ν B

Metrics