Expand this Topic clickable element to expand a topic
Skip to content
Optica Publishing Group

Design and development of a trenched optical fiber with ultra-low bending loss

Open Access Open Access

Abstract

We have designed and experimentally demonstrated a single mode optical fiber with a very low bending loss of about 0.014 dB/loop at 1550 nm for a bending radius of 5 mm.

©2009 Optical Society of America

1. Introduction

With growing interests among researchers in fiber-to-the-home (FTTH) applications driven by increasing number of internet users, the research and the development of optical fibers having bend insensitivity are in much demand [14]. In contrast to currently used single mode optical fibers (SMFs) that cause a huge power penalty due to bendings at corners of a home, bend-insensitive optical fibers (BIF) offer cost savings and compactness of fiber boxes. Specifically, two kinds of bend-insensitive optical fibers are available: (a) low-index trenched BIFs, and (b) Mode field diameter (MFD) optimized BIFs.

In the low-index trenched BIF approach, the bend insensitivity is achieved by putting a low index trench in the cladding, thereby reducing the cladding effective index and preventing the loss of power due to bendings [1,2]; the commercialization of these BIFs have been already achieved [35]. In the extended version of the low-index trenched optical fiber, the optical fiber with bending loss of 0.03 dB/loop has been reported at 1550 nm for the bending radius of 5 mm where a nano-engineered low-index ring around the core has been used [5]. Thus, this approach of adding low-trenches or low-index nano-rings in the cladding region has successfully addressed the issue of reducing the bending loss. Typical bending loss for the low-index trenched optical fiber is about 0.67 dB/loop [4] and 0.03 dB/loop [5] for the low-index trenched and nano-engineered optical fibers, respectively, at 1550 nm for the bending radius of 5 mm. In the second approach to achieve bend insensitivity in the optical fiber, the MFD of optical fiber core can be optimized such that the mode field is confined inside the optical fiber core, which then limits the bending loss upon sharp bends. Experimentally measured bending loss reported with such technique of bending loss optimization has been restricted to about 1 to 1.7 dB/loop at 1550 nm for the bending radius of 5 mm because MFD cannot be reduced below 6–7 µm, otherwise incompatibility of these fibers with existing single mode fibers (SMFs) arise [68].

Making the low index trench in the optical fiber needs a high skill of fiber manufacture. The low-index trench in the optical fiber can be added by co-doping silica with fluorine or boron. If we define the trench index difference as

ΔnTrench=ncladnTrench

where n Trench is the trench index and n clad is the cladding index, its typical value is around 0.002 for the fluorine doping (in the modified chemical vapor disposition (MCVD) system), but this index difference value of the trench is not sufficient to achieve the desired bend insensitivity [6]. Another way to make low refractive index of the trench is to use the boron doping, but then the control of trench width becomes an issue due to the diffusion of boron atoms in the surrounding regions. Therefore, the fluorine doping is preferred to the boron doping. Considering the skill required and cost related factors in manufacturing the low-index trenched optical fiber, we combined (a) the shallow low-index trench to be fabricated using the fluorine doping and (b) the MFD optimization to achieve the lowest bending loss for any optical fiber reported so far. It should be strongly emphasized that since the optical fiber fabricated by using the MCVD technique usually shows central dip in the core and therefore to design the experimental BIF fiber, we chose the worst case of central index dip (i.e., the dip index reaching the cladding index value). It is noted that occurrence of the worst case central index dip is usual if no measures are taken to reduce it (for example, removing the innermost layer, or additional supply of GeO2 just before sealing of the preform; that needs a skilled experimentalist). Therefore, if the current methodology is followed, no central dip removing technique is necessary; limitations on the dispersion and the MFD will be taken care by the design. In the current communication, firstly, we discuss a theoretical design of the bend-insensitive optical fiber by adopting the MFD and the trench optimization technique, and secondly, we report the development of optical fiber at tolerable limits to achieve the lowest bending loss ever reported for the single mode optical fiber.

2. Design

To theoretically design the bend-insensitive SMF, the MFD of fiber was calculated from the following relation:

MFD=22π(rE2rdr)2πrE4rdr

The macrobending loss in units of dB/km was calculated using [9,10]:

αmacro=10Loge10(πV816aRbW3)12exp(4RbΔW33aV2)[0(1g)Erdr]20E2rdr

where E is the radial field of fundamental mode, a denotes the fiber core radius, Rb is the bend radius, nmax and nmin are maximum and minimum values of the refractive index and other parameters appearing in Eq. (3) are given by:

g=n(r)2nmin2nmax2nmin2;V=k0anmax2nmin2
W=aβ2(k0nmin)2;Δ=nmax2nmin22nmax2

We used the commercial FiberCAD code to solve propagation equations and to calculate the bending loss of optical fiber. It is noted that to address the issue of a central index dip (typical for the optical fiber made with the MCVD process) the refractive index profile was modeled as:

n(r)=nmax12Δ(1ra)2

where n max is the maximum value of core refractive index, w is a width of dip region, and Δ(n 2 max-n 2 clad)/(2n 2 max). We choose 100% central dip (i.e., the dip approaching the value of cladding index; n(0)=nclad) for designing the optical fiber.

Design criteria are listed in Table 1 that followed the ITU-T recommendation for G652 for the optical fibers except that the MFD requirement was relaxed to be above 7.5 µm [8]. With regards to the cutoff wavelength of SMF, the ITU-T recommendation tells that the cable-cutoff wavelength should not be more than 1260 nm. Though there is no exact relationship available between the cable cutoff wavelength and the fiber cutoff wavelength, with our own observations it can be stated that the mentioned cable cutoff wavelength is roughly equals to 1350 nm to 1450 nm of the optical fiber cutoff wavelength. The optimum parameters that we obtained were subjected to these cutoff wavelength constraints. The design methodology adopted was as follows. Step-1: we obtained the optimum core refractive index and radial parameters of the bend-insensitive single mode optical fiber that followed the design criterion-1. Step-2: by using the core parameters obtained with Step-1, a trenched SMF was designed for various trench parameters that followed the design criterion-2. By using these two different design steps, we were able to obtain the trench parameters that resulted in the minimum bending loss possible within said limits of design criteria.

Tables Icon

Table 1. Design criteria for the bend- insensitive single mode optical fiber.

Following the design criterion-1, calculated refractive index and core radius values of the bend-insensitive single mode optical fiber without any trench are listed in Table 2(a) for the core without central index dip, and in Table 2(b) for the core with central index dip. Parameters that pose limitations on core radius values at the given index, n max, are shown in brackets. It can be observed that for the bend-insensitive single mode optical fiber to follow the design criterion-1, there is limited freedom to choose core parameters. As an example, typical curves used to get data in Table 2(b) are illustrated in Fig. 1 for the core refractive index of 1.452, where it can be observed that the MFD at 1550 nm is always more than 7.5 µm for any value of the core radius and therefore it has been mentioned as ‘Any’ in Table 2(b). It can also be noted that for parameters mentioned in Fig. 1, the bending loss decreases with increasing the core radius and therefore we need the core radius above certain value (i.e., above ‘minimum a’) to get the bending loss less than 2 dB/loop at 1550 nm and the bending radius of 5 mm.

Tables Icon

Table 2. (a). Optical parameters of the single mode optical fiber without central index dip. These parameters were obtained by following limitations on the bracketed parameter as listed in the design criterion-1.

Core radius a is in µm, Bending loss is in dB/loop at 1550 nm for 5 mm of the bending radius.

Tables Icon

Table 2. (b). Optical parameters of the single mode optical fiber with central index dip. These parameters were obtained by following limitations on the bracketed parameter as listed in the design criterion-1.

Core radius a is in µm, Bending loss is in dB/loop at 1550 nm for 5 mm of the bending radius.

 figure: Fig. 1.

Fig. 1. Dependence various parameters of the single mode fiber on its core with the central index dip. The core index was 1.452.

Download Full Size | PDF

Next, by using design values of Table 2(b), we calculated trench parameters that gave the lowest theoretical bending loss values. A trenched refractive index profile of proposed BIF is shown in Fig. 2(a). As detailed design of trench parameters for the general SMF has been already described in [6], and because our aim in this paper is to address experimental issues, the current communication has been restricted to the design of trench parameters of the bend-insensitive single mode optical fiber having the central index dip in the core.

 figure: Fig. 2.

Fig. 2. (a) A refractive index profile of the bend-insensitive single mode optical fiber. (b) Dependence of the theoretical bending loss on b at 1550 nm for 5 mm bending radius. Note that there is an optimum value of b corresponding to the lowest bending loss at the bending radius of 5 mm.

Download Full Size | PDF

To understand easily what has to be optimized to get the lowest bending loss, a typical example emphasizing a fact that the lowest theoretical bending loss can be obtained by selecting a proper value of b is shown in Fig. 2(b) where it can be observed that there exists the lowest bending loss value at the particular value of b. We carried out calculations that gave a set of optimum b values for various c, Δn Trench and the core index. Utility curves showing variations of optimum b values to obtain the lowest bending loss (at 1550 nm and 5 mm of the bending radius) are shown in Fig. 3 for various core refractive indices and c values. Corresponding values of Δn Trench that satisfy the design criterion-2 for different core indices are shown in Fig. 4. A complete set of optimized parameters can be obtained from Fig. 3 and Fig. 4.

 figure: Fig. 3.

Fig. 3. Optimized values of b and c to get the lowest bending loss at 1550 nm for the bending radius of 5 mm at various core refractive indices. The central index dip has been considered to be 100%.

Download Full Size | PDF

 figure: Fig. 4.

Fig. 4. Minimum values of the trench refractive index difference at various core index values at optimized b and c values. The central index dip has been considered to be 100%.

Download Full Size | PDF

3. Experiments

An optical fiber preform with the germano-silicate glass composition was fabricated by using the MCVD technique to follow design parameters mentioned in Section 2. The optical fiber with outer diameter of 125 µm was drawn at 2000 °C by using the draw tower. Refractive index profile of the optical fiber is illustrated in Fig. 5. Its cutoff wavelength was determined to be around 1350 nm.

 figure: Fig. 5.

Fig. 5. Refractive index profile of the optical fiber fabricated using MCVD process

Download Full Size | PDF

To measure the bending loss, we spliced two single mode fibers at two ends of the BIF and the optical power was measured by using the optical spectrum analyzer (OSA). A broadband light source (ASE source) emitting at 1300 nm to 1650 nm was used as the input. Bending losses were measured independently with one and ten loops, each having the bending radius of 5 mm. An experiment to measure the bending loss is shown in Fig. 6, where S 1 and S 2 indicate splicing points. The output power (Ps) from the BIF was measured initially when it was straight and then again when a loop of 5 mm radius was applied (Pb); the ratio Pb/Ps gave the bending loss. These measurements were repeated several times to estimate the error margin.

 figure: Fig. 6.

Fig. 6. An experimental setup to measure the bending loss of BIF.

Download Full Size | PDF

We also measured the splicing loss between our BIF and the commercially available SMF [11] having MFD of about 9.5 µm at 1550 nm. To measure the actual splicing loss, initially we fusion spliced the BIF (length=50 cm) between two SMFs (length=50 cm each) and recorded the output power (P2), the experimental setup was similar to Fig. 6 except fiber lengths. Then without changing input and output launch conditions, we removed the BIF and fusion spliced remaining SMFs and recorded the output power (P 3). The splicing loss was calculated in dB as follows:

αdB=12[10log10(P3P2)]

where αdB is the splicing loss in dB. It is noted that factor ½ in Eq. (6) has been used to average the splicing loss for a splice.

4. Results and discussion

As shown in the refractive index profile of proposed bend-insensitive single mode optical fiber (Fig. 5), we obtained c/a=2.84, Δn Trench=0.002, n max=1.456 and core radius, a=3.05 µm. It is noted that we used fluorine doping technique to obtain the low index trench and the low-index difference value was just 0.002; it was much smaller than the minimum trench index difference of 0.0028 needed to obtain the negligible bending loss at the bending radius of 5 mm [6], thus making the fabrication of optical fiber using the MCVD process much simple. A very low bending loss in spite of the low trench index difference can be attributed to our technique of optimizing the MFD and trench parameters as described earlier. We measured the maximum bending loss of about 0.014 dB/loop at 1550 nm for the bending radius of 5 mm (as listed in Table 3). Typical transmission spectra of the BIF after applying 1 and 10 loops of 5 mm radius are shown in Fig. 7. It can be observed that transmission spectra were approximately same for the straight and the bent fiber. To estimate the error, various events where the bending losses at 1550 nm were recorded are shown in Fig. 8, where it can be seen that the maximum bending loss was limited to 0.014 dB/loop at the bending radius of 5 mm and the standard deviation error was ±0.002. For our BIF, the MFD was measured by using the standard single mode fiber characterization equipment and it was found to be about 7.7 µm at 1550 nm. Thus, the BIF followed the target of MFD (to be more than 7.5 µm at 1550 nm) along with the ultra low bending loss at 1550 nm. Measured optical parameters of the bend-insensitive single mode optical fiber are listed in Table 3.

Tables Icon

Table 3. Measured optical parameters of the bend-insensitive single mode optical fiber.

 figure: Fig. 7.

Fig. 7. Comparison of spectral variations of the output power when the BIF was straight and when loops were formed with the radius of 5 mm. Top figure shows a wide band variation, while an enlarged version for the band around 1550 nm has been shown in the bottom figure.

Download Full Size | PDF

 figure: Fig. 8.

Fig. 8. Experimental results showing the bending loss measured at various events (wavelength=1550 nm; bending radius=5 mm. The maximum value of bending loss was limited to 0.014 dB.

Download Full Size | PDF

Another point to be stressed is the tolerance of design. From utility curves of Fig. 3 and Fig. 4, it can be estimated that for our fiber the optimum value of b/a should be 2.12 for the lowest bending loss at 1550 nm for the bending radius of 5 mm, while experimentally obtained b/a was 0.98. Theoretical curve indicating the bending loss that would have been obtained for our bend-insensitive single mode optical fiber at various b/a is shown in Fig. 9. From Fig. 9, it can be stated that the bending loss would have been 0.0123 dB/loop instead of 0.014 dB/loop at the bending radius of 5 mm (at 1550 nm) if theoretical design criteria were followed.

 figure: Fig. 9.

Fig. 9. Dependence of the bending loss on b/a at c/a=2.84, ΔnTrench=0.002, nmax=1.456 and core radius, a=3.05 µm (bending radius=5 mm and wavelength=1550 nm). The theoretical bending loss was adjusted with the measured bending loss at 1550 nm. Optimum b/a was 2.12, while experimentally obtained b/a was 0.98.

Download Full Size | PDF

Reason for such a small bending loss in our bend-insensitive fiber can be explained as follows. When the fiber is subjected to bend, some mode field in the core is leaked into the cladding region causing the bending loss. In our bend-insensitive single mode optical fiber: (a) confinement of the field in the optical fiber core (MFD optimization) reduced the bending loss because less power was leaked into the cladding, and (b) due to a low-index trench that was formed outside the core, the effective refractive index of the cladding was reduced, which eventually increased the coupling of cladding field to the core region when the fiber was again straight, thereby reducing the bending loss. Combination of these two effects has resulted in the ultra-low bending loss ever reported at 1550 nm for the bending radius of 5 mm.

Other parameters of the optical fiber such as the dispersion and the dispersion slope at various wavelengths are shown in Fig. 10 and Fig. 11, which show that these parameters are well within the ITU-T recommendations. A comparison of bending characteristics of our fiber with other reported results have been listed in Table 4, which illustrates that the bending loss for our BIF was much smaller than the similar category of MFD optimized fibers [7].

 figure: Fig. 10.

Fig. 10. Dispersion and MFD characteristics of the fabricated bend insensitive optical fiber.

Download Full Size | PDF

 figure: Fig. 11.

Fig. 11. Calculated bending loss and dispersion slope characteristics of the bend insensitive optical fiber at the bending radius of 5 mm. The theoretical bending loss was adjusted with the maximum value of measured bending loss at 1550 nm.

Download Full Size | PDF

Tables Icon

Table 4. A comparison of bending losses of different bend-insensitive single mode optical fibers. Bending loss has been computed for one loop of 5 mm radius.

Finally commenting on the splicing loss of BIF, it can be stated that the utility of BIF depends on how well it can be adopted in the existing fiber optics network that is composed of conventional single mode fibers. Important practical issues to be addressed for the compatibility of the BIF with the SMF are: (a) easiness of splicing and (b) splicing loss between two fibers. As illustrated in Section 3, we carried out the splicing loss measurement between our BIF and the commercially available SMF by using the experimental setup similar to one shown in Fig. 6. To fusion splice two fibers, we used a fusion-splicer and it was observed that the fusion splicing was quite easy and all our splicing events were successful as shown in the Fig. 12. Typical measurements for the splicing loss between the BIF and the SMF are shown in Fig. 13, where the splicing loss can be noted to be about 0.376 dB. Several repeated measurements showed that the maximum value of splicing loss between the BIF and the SMF was limited to 0.467 dB as shown in Fig. 14. It can be mentioned that the advantage brought by the BIF (bending loss ~0.014 dB at 5 mm of the bending radius) surpasses the slight disadvantage of increase in the splicing loss (maximum 0.467 dB).

 figure: Fig. 12.

Fig. 12. Photographs showing two successive events of the fusion splicing between two fibers; our BIF is at the left side of a viewer while the SMF is shown on the right side.

Download Full Size | PDF

 figure: Fig. 13.

Fig. 13. Typical splicing loss between the SMF and the BIF.

Download Full Size | PDF

 figure: Fig. 14.

Fig. 14. Measured splicing loss values between the SMF and the BIF for several measurement events. The maximum splicing loss between the SMF and the BIF was limited to 0.467 dB.

Download Full Size | PDF

We further investigated the splicing loss in terms of the transverse offset (where two fibers were misaligned along the axis parallel the end face of fiber) and the longitudinal offset (where fibers were misaligned along the axis perpendicular to the end face of fiber). For the transverse splicing loss measurement, the separation between the SMF and the BIF was 5 µm. As illustrated in Fig. 15, the transverse offset and the longitudinal offset losses between the SMF and the BIF were quite high. The relative splicing loss mentioned in Fig. 15 is the splicing loss calculated with respect to the splicing loss when two fibers were perfectly aligned along the axis (for the transverse splicing loss) or when they were fused (for the longitudinal splicing loss).

 figure: Fig. 15.

Fig. 15. Losses due to the transverse offset and the longitudinal offset between the BIF and commercial SMF at 1550 nm. The transverse splicing loss was measured with the separation of 5 µm between two fibers.

Download Full Size | PDF

Before concluding, with regards to our BIF, we would like to comment on relationship between the theoretical bending loss and the experimental bending loss. It can be stated that the bending loss obtained by Eq. (2) to Eq. (5) is qualitative in nature and for the quantitative accuracy one needs some constant value to be multiplied to the theoretical value. Considering the maximum bending loss we measured at 1550 nm for the BIF (i.e., 0.014 dB/loop at 5 mm of the bending radius), we found that this multiplying constant was 271.884 at 1550 nm for 5 mm of the bending radius.

5. Summary

We have designed and developed the bend-insensitive single mode optical fiber with the MFD optimization and the low-index trench technique, which showed that the bending loss was 0.014 dB/loop at 1550 nm for a loop of 5 mm radius. The maximum value of splicing loss between the BIF and the SMF was limited to 0.467 dB at 1550 nm.

Acknowledgments

This work was supported by the Brain Korea-21 Information Technology Project, Ministry of Education and Human Resources Development, by the National Core Research Center (NCRC) for Hybrid Materials Solution of Pusan National University, by the GIST Top Brand Project (Photonics 2020), Ministry of Science and Technology, and by the Samsung Electronics Hainan Fiberoptics-Korea Co. Ltd., South Korea.

References and links

1. K. Himeno, S. Matsuo, N. Guan, and A. Wada, “Low bending loss single mode fibers for Fiber-to-the-Home,” IEEE J. Lightwave Technol. 23(11), 3494–3499 (2005). [CrossRef]  

2. P. R. Watekar, S. Ju, and W.-T. Han, “Single-mode optical fiber design with wide-band ultra low bending-loss for FTTH application,” Opt. Express 16(2), 1180–1185 (2008). [CrossRef]  

3. Sumitomo (2009), http://www.sumitomoelectric.com/news/pr/press.asp?entryid=266, http://www.sumitomoelectric.com/news/pr/press.asp?entryid=266

4. Samsung (2009), http://www.samsungfiberoptics.com/products/OF/OF_SF_BIF.asp

5. M.-J. Li, P. Tandon, D. C. Bookbinder, S. R. Bickham, M. A. McDermott, R. B. Desorcie, D. A. Nolan, J. J. Johnson, K. A. Lewis, and J. J. Englebert, “Ultra-low bending loss single-mode fiber for FTTH,” in Optical Fiber Communication Conference and Exposition and The National Fiber Optic Engineers Conference, OSA Technical Digest (CD) (Optical Society of America, 2008), paper PDP10. http://www.opticsinfobase.org/abstract.cfm?URI=OFC-2008-PDP10.

6. P. R. Watekar, S. Ju, Y. S. Yoon, Y. S. Lee, and W.-T. Han, “Design of a trenched bend insensitive single mode optical fiber using spot size definitions,” Opt. Express 16(18), 13545–13551 (2008). [CrossRef]  

7. Stokeryale bend-insensitive fiber (2007), http://www.stockeryale.com/o/fiber/products/bif-1550-l2.htm

8. ITU-T recommandations G.652, http://www2.ing.unipi.it/~d7384/HTML/AdT/ITU_G652.pdf

9. A. W. Snyder and J. D. Love, in: Optical waveguide theory, Chapman and Hall (1983).

10. D. Marcuse, “Curvature loss formula for optical fibers,” J. Opt. Soc. Am. 66(3), 216–220 (1976). [CrossRef]  

11. Samsung (2009), http://www.samsungfiberoptics.com/products/OF/OF_SF_SMF.asp

Cited By

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

Alert me when this article is cited.


Figures (15)

Fig. 1.
Fig. 1. Dependence various parameters of the single mode fiber on its core with the central index dip. The core index was 1.452.
Fig. 2.
Fig. 2. (a) A refractive index profile of the bend-insensitive single mode optical fiber. (b) Dependence of the theoretical bending loss on b at 1550 nm for 5 mm bending radius. Note that there is an optimum value of b corresponding to the lowest bending loss at the bending radius of 5 mm.
Fig. 3.
Fig. 3. Optimized values of b and c to get the lowest bending loss at 1550 nm for the bending radius of 5 mm at various core refractive indices. The central index dip has been considered to be 100%.
Fig. 4.
Fig. 4. Minimum values of the trench refractive index difference at various core index values at optimized b and c values. The central index dip has been considered to be 100%.
Fig. 5.
Fig. 5. Refractive index profile of the optical fiber fabricated using MCVD process
Fig. 6.
Fig. 6. An experimental setup to measure the bending loss of BIF.
Fig. 7.
Fig. 7. Comparison of spectral variations of the output power when the BIF was straight and when loops were formed with the radius of 5 mm. Top figure shows a wide band variation, while an enlarged version for the band around 1550 nm has been shown in the bottom figure.
Fig. 8.
Fig. 8. Experimental results showing the bending loss measured at various events (wavelength=1550 nm; bending radius=5 mm. The maximum value of bending loss was limited to 0.014 dB.
Fig. 9.
Fig. 9. Dependence of the bending loss on b/a at c/a=2.84, ΔnTrench =0.002, nmax =1.456 and core radius, a=3.05 µm (bending radius=5 mm and wavelength=1550 nm). The theoretical bending loss was adjusted with the measured bending loss at 1550 nm. Optimum b/a was 2.12, while experimentally obtained b/a was 0.98.
Fig. 10.
Fig. 10. Dispersion and MFD characteristics of the fabricated bend insensitive optical fiber.
Fig. 11.
Fig. 11. Calculated bending loss and dispersion slope characteristics of the bend insensitive optical fiber at the bending radius of 5 mm. The theoretical bending loss was adjusted with the maximum value of measured bending loss at 1550 nm.
Fig. 12.
Fig. 12. Photographs showing two successive events of the fusion splicing between two fibers; our BIF is at the left side of a viewer while the SMF is shown on the right side.
Fig. 13.
Fig. 13. Typical splicing loss between the SMF and the BIF.
Fig. 14.
Fig. 14. Measured splicing loss values between the SMF and the BIF for several measurement events. The maximum splicing loss between the SMF and the BIF was limited to 0.467 dB.
Fig. 15.
Fig. 15. Losses due to the transverse offset and the longitudinal offset between the BIF and commercial SMF at 1550 nm. The transverse splicing loss was measured with the separation of 5 µm between two fibers.

Tables (5)

Tables Icon

Table 1. Design criteria for the bend- insensitive single mode optical fiber.

Tables Icon

Table 2. (a). Optical parameters of the single mode optical fiber without central index dip. These parameters were obtained by following limitations on the bracketed parameter as listed in the design criterion-1.

Tables Icon

Table 2. (b). Optical parameters of the single mode optical fiber with central index dip. These parameters were obtained by following limitations on the bracketed parameter as listed in the design criterion-1.

Tables Icon

Table 3. Measured optical parameters of the bend-insensitive single mode optical fiber.

Tables Icon

Table 4. A comparison of bending losses of different bend-insensitive single mode optical fibers. Bending loss has been computed for one loop of 5 mm radius.

Equations (7)

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

ΔnTrench=ncladnTrench
MFD=2 2π(rE2rdr)2πrE4rdr
αmacro=10Loge10(πV816aRbW3)12exp(4RbΔW33aV2)[0(1g)Erdr]20E2rdr
g=n(r)2nmin2nmax2nmin2;V=k0anmax2nmin2
W=aβ2(k0nmin)2;Δ=nmax2nmin22nmax2
n(r)=nmax12Δ(1ra)2
αdB=12[10log10(P3P2)]
Select as filters


Select Topics Cancel
© Copyright 2024 | Optica Publishing Group. All rights reserved, including rights for text and data mining and training of artificial technologies or similar technologies.