2014
DOI: 10.7567/jjap.53.042502
|View full text |Cite
|
Sign up to set email alerts
|

Wide-range temperature dependences of Brillouin scattering properties in polymer optical fiber

Abstract: We investigate the temperature dependences of the Brillouin scattering properties in a perfluorinated graded-index (PFGI-) polymer optical fiber (POF) in a wide temperature range from −160 to 125 °C. The temperature dependences of the Brillouin frequency shift, linewidth, and Stokes power are almost linear at lower temperature down to −160 °C; while they show nonlinear dependences at higher temperature. These behaviors appear to originate from the partial glass transition of the polymer material.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

4
18
0

Year Published

2014
2014
2024
2024

Publication Types

Select...
3
3
1

Relationship

2
5

Authors

Journals

citations
Cited by 33 publications
(22 citation statements)
references
References 21 publications
4
18
0
Order By: Relevance
“…As shown in the inset of Fig. 3(b), the BFS decreased with increasing temperature, with a proportionality constant of -3. of the heated section), which agrees well with a previously reported value [17]. The BFS fluctuations along the nonheated sections showed a standard deviation of approximately ±3.0 MHz, corresponding to strain and temperature measurement errors of around ±0.02% and ±0.9 °C, respectively.…”
Section: Methodssupporting
confidence: 91%
See 3 more Smart Citations
“…As shown in the inset of Fig. 3(b), the BFS decreased with increasing temperature, with a proportionality constant of -3. of the heated section), which agrees well with a previously reported value [17]. The BFS fluctuations along the nonheated sections showed a standard deviation of approximately ±3.0 MHz, corresponding to strain and temperature measurement errors of around ±0.02% and ±0.9 °C, respectively.…”
Section: Methodssupporting
confidence: 91%
“…Then, a partial reflection point can be automatically created at the butt-coupled interface between the POF and the silica SMF (the pigtail of an optical circulator) [15], at which Fresnel-reflected light with a reflectivity of 0.2% (calculated The key to the solution of the second problem is the BFS hopping phenomenon [21], in which the BFS in the POF (BFS: ~2.8 GHz) can be irreversibly upshifted by ~300 MHz only by applying a large strain of >7.3%. Unless cryogenic sensing is the intended application, the BFS "upshift" is preferable because the BFS in a POF decreases with increasing applied strain [16] and temperature [16], [17]). Thus, instead of inserting different fibers around the butt-coupled part, we have only to pull the POF for a length sufficiently longer than half of the spatial resolution (i.e., the width of the 0th correlation peak).…”
Section: Principlesmentioning
confidence: 99%
See 2 more Smart Citations
“…The experimental setup is simpler, and it is possible to choose and change the stimulation point. Furthermore, the Brillouin spectroscopy is a powerful tool for investigating acoustic properties under various measurement conditions, such as temperature, 6,16,17) and pressure, 18) during a phase transition. 19,20) Noncontact stimulation allows one to change these conditions without affecting the transducer used for the induction of phonons.…”
Section: Introductionmentioning
confidence: 99%