1 August 2009 Optimal design of single resonant and ultrabroadband long-period fiber grating filters
Author Affiliations +
Abstract
We propose a spectral flat-top, single resonant, and ultrabroadband-more than 180 nm in a -20-dB bandwidth-long-period fiber grating (LPG) filter. The ultrabroadband LPG is based on a thin cladding layer LPG synthesized by the Lagrange multiplier optimization (LMO) algorithm. As the bandwidth and resonant spectra cover a very wide band, both material dispersion and waveguide dispersion were included in the calculations of the LMO method. To the best of our knowledge, the bandwidth of the designed flat-top LPG filter in the -20-dB coupling is the broadest currently existing in the literature. Such designed LPG devices can be very useful for a variety of applications in broadband optical communication systems.
Lee and Han: Optimal design of single resonant and ultrabroadband long-period fiber grating filters

1.

Introduction

Long-period fiber gratings (LPGs), coupled with a guided core mode in copropagating modes in an optical fiber, have been widely used as band-rejection filters, wavelength-dependent loss filters, mode converters, and high-sensitivity sensors.1 Recently, due to the rapid development of ultrawideband ( S+ band–L-band) gain amplifiers, a broadband gain flattening device within a very wide bandwidth is needed; consequently, the LPGs appear to be good candidates for gain flattening applications.2 However, broadband LPG filters could lead to a high insertion loss as a result of the high-order cladding modes coupling in a typical LPG device. To overcome this shortcoming, Jeong and Oh theoretically presented a new LPG filter that significantly enhanced the free spectral range (FSR) by controlling the waveguide dispersion of the cladding modes in fluorine-doped-cladding LPG.3 Their model further controlled material dispersion in the cladding region using doped ions Cr3+ to change the effective indices of the cladding modes,4 thereby changing the phase-matching conditions of LPGs as well. However, the proposed methods are not very practical due to the highly difficult fabrications of such special fibers.

Another technique to enhance the FSR of LPG involves etching the fiber cladding with hydrofluoric acid (HF). Yin demonstrated that an HF-etched ultrathin LPG (with a cladding thickness of 28mm ) with first-order cladding mode coupling provides a wide tuning range of 120nm and has only a single resonant peak over a wide wavelength range (10002000nm) .5 These authors subsequently presented a highly sensitivity sensor based on an ultrathin-clad LPG, with high-order mode coupling that can be tuned for > 220nm as well as a single resonant peak in a wide range of wavelength bands;6 however, the inherent bandwidth of the resonance peaks of LPGs are narrow, at about several nanometers, because the phase-matching condition between the two optical modes is satisfied at only a specific resonant wavelength. Indeed, this is the major drawback of the bandwidth-versus-coupling strength trade-offs for practical applications when using such a narrowband LPG device.

To enhance LPGs’ performance for broadband resonance of LPG, Wang and Ramachandran 7, 8, 9 demonstrated several broadband, spectrally flat LPG-based devices in especially designed few-mode fibers, which were designed to have two coupled modes with identical group velocities in the desired spectral range of wavelength. The LPG coupling in this condition can achieve a broadband mode conversion because it occurs in the turnaround point (TAP) between the fundamental mode and a specific higher-order guided core mode (with negative chromatic dispersion). Although engineering a fiber waveguide to have identical group velocities for two modes may yield a better broadband grating if a LPG is written to couple at the TAP, the bandwidth of the proposed LPG devices cannot be > 180nm at the 20-dB coupling strength (the record bandwidth is 110nm with a flatband for the variable optical attenuator in Ref. 9). Moreover, the special dispersion-tailor fiber must be difficultly fabricated using a specially designed process.

The current paper presents another option: a spectral flat-top, single resonant, and ultrabroadband LPG (UBLPG) with a bandwidth of > 180nm at 20-dB . The proposed device is based on a thin-cladding LPG with synthesizing using the Lagrange multiplier optimization (LMO) algorithm. To the best of our knowledge, the bandwidth of the designed UBLPG at 20dB is the broadest in the existing literature. Such devices can be utilized as broadband mode converters and broadband couplers for broadband optical applications. They can also be used as a broadband all-fiber polarizer when the UBLPG is written in the birefringent fiber. Moreover, due to core and cladding coupling in the thin-clad LPG, these devices could be used as a tunable broadband filter by changing the refractive index of the surrounding. The current study examines the waveguide dispersion as well as material dispersion, calculated using the Sellmeier equation, involved in the numerical analysis for covering such a wideband wavelength range. The effective indices of the guided modes are subsequently obtained by solving the characteristic equations of the fiber. From the simulation results, the bandwidth of the resonant peak for the designed LPG can be substantially broadened when using the proposed LMO algorithm, which is a variation-based approach that has been proven to be very effective in designing different fiber grating filters for the applications of fiber optics.10, 11, 12 Furthermore, the presented UBLPG device has only a single resonant peak over a very wide wavelength range (> 600nm) . We believe that such UBLPG devices will be very useful in a variety of applications for an ultrawideband optical communications to cover the S+L bands.

2.

LMO Algorithm for UBLPG

LPGs incorporate coupling guided through the core mode into the forward propagating modes in a fiber by phase matching the two modes at resonant wavelengths. LPGs characteristics can be effectively identified using the coupled mode equations.13 As the single resonance peak of the designed UBLPG is extended over an extremely wide wavelength range, the material dispersion should be considered in the simulation processes. The dispersive characteristics of pure silica (SiO2) and silica doped with dopants such as GeO2 have been precisely calculated using the following Sellmeier equation:

1

n21=i=13Aiλ2λ2Bi2,
where Ai and Bi are Sellmeier coefficients and λ is the wavelength, measured in microns. The silica doped with GeO2 used in this designed case is shown in Table 1.14 The effective index of the guided core mode can thus be obtained using dispersion relations.13 The effective indices of cladding modes can be determined by solving the dispersion relations of three-layer optical fibers.6 Once the effective core and cladding modes are calculated, the resonant wavelengths of the LPGs can be expressed as λpm=(neffconeffclm)Λ , where neffco and neffclm are the effective indices of the core and the m -order cladding modes and Λ is the grating period of UBLPG. The detailed theoretical analysis of LMO for synthesized LPGs has been described in a previous work,11 in which the boundary conditions for the coupled equations of the Lagrange multipliers were obtained by using the variational method with the cost functional with respect to the parameters of the designed LPG. In the current study, to improve the target performance, the corresponding boundary conditions for Lagrange multipliers coupled equations at L are strategically calculated in decibel scale, as follows:

2.

2a

μco(L)=2Aco(L)(ΔtdB),

2b

μcl(L)=0,
where μco(L) and μcl(L) are the Lagrange multipliers fields for the core and cladding mode of UBLPG at L , L is the grating length, Aco(L) is the mode field of the core mode of the designed UBLPG at L , and ΔtdB={10log10[Tco(λ)]10log10[Td(λ)]} is the discrepancy between the output [Tco(λ)] and target transmission spectra [Td(λ)] in the decibel scale. On the basis of the numerical results, it is found that such a strategy using the decibel scale in the formulation of boundary condition (BC) of Lagrange multipliers equations provides a much better improvement in the convergence of the LMO algorithm (decibel-scale LMO) than those cases the BC are calculated in linear scale (linear-scale LMO).

Table 1

Sellmeier coefficients of silica glass doped with GeO2 .14

Composition SiO2 (100mol%) GeO2 (0mol%) SiO2 (96.5mol%) GeO2 (3.5mol%)
A1 0.69616630.7004080
B1 0.06840430.0684241
A2 0.40794260.4188000
B2 0.11624140.1175610
A3 0.89747940.8959635
B3 9.89616109.9642629

3.

Design Results and Discussion

This section demonstrates an ultrabroadband thin-clad LPG filter with a single resonant peak in an extremely wide range of wavelength band (600nm) optimally designed using a decibel-scale LMO algorithm. In the analysis, the fiber core was assumed to be germanosilicate glass (with doped 3.5mol% GeO2 ), as in conventional single-mode fibers. The refractive index of cladding was the pure silica, and the surrounding material was air (with a refractive index of 1). The dispersive characteristics of core and cladding were calculated, and the refractive indices are provided in Fig. 1. When the fiber core and cladding diameters are set at 8.2 and 40μm of the thin-clad LPG, respectively, the effective refractive index of the fundamental core mode can be obtained through the dispersion relation and shown in dotted line of Fig. 1. The first five odd-cladding modes determined by the dispersion relations of the three-layer optical fiber6 are shown in Fig. 1.

Fig. 1

(a) Refractive indices of core and cladding of the fiber; the dotted line is the effective index of the guided core mode. (b) The effective indices of the first five odd-cladding modes ( LP0m , m=1,3,5. ) of the proposed fiber device. (c) The phase-matching grating periods versus the coupling wavelengths for the first five odd-cladding modes.

080501_1_1.jpg

From the LPG’s phase-matched conditions of LPG, the grating period (Λ) can be calculated as a function of the wavelength (λ) , as shown in Fig. 1 for the first five odd-cladding mode couplings. If the grating period is set to 285μm , the corresponding resonant wavelength λp is 1.529μm when the core mode and first odd-cladding mode satisfy the matching coupling phase. (One can also choose high-order mode coupling for simulations.) It can be clearly seen that only one resonant peak in a very wide wavelength band emerges, regardless of which cladding mode of coupling is used in the thin-clad LPG. Figure 2 depicts the corresponding transmission spectra of nonoptimized (Gaussian apodized) and LMO-UBLPG with a grating length of 40mm . The coupling coefficients (κ) of the designed UBLPGs are shown in Fig. 2. The dashed line is the Gaussian apodized, while the solid line and dashed dotted line present real (κr) and imaginary (κi) parts of the coupling coefficient synthesized by decibel-scale LMO algorithm. From the simulation results of the dotted line of Fig. 2, the bandwidth of the designed LMO(I)-LPG can be significantly expanded by using the linear-scale LMO algorithm in Ref. 11. However, the coupling strength of the LMO(I)-LPG is only 20dB for the final convergence because the boundary conditions μco(L) and μcl(L) of the linear-scale LMO algorithm are saturated with the error of 0.01 .

Fig. 2

(a) Transmission spectra of the designed UBLPGs. The dotted line is LMO(I) method using linear scale, and the dashed line is LMO(II) method with decibel scale. (b). Real (κr) and imaginary (κi) parts of the designed coupling coefficients of UBLPG, with a grating length of 4cm .

080501_1_2.jpg

To improve the performance of the proposed filter when the target performance is in the decibel scale, the decibel-scale LMO algorithm mentioned in the previous section is utilized. The designed LPG [called LMO(II)-LPG] is depicted by the dashed line in Fig. 2, which indicates that the almost 30dB coupling strength can be achieved with a bandwidth of about 100nm and 20dB with a bandwidth of 180nm . In addition, these designed LPGs should be polarization insensitive due to the spatially symmetric modes in the cylindrical structure of optical fiber. Furthermore, the LPGs are in general significantly easier to fabricate than FBGs due to the LPG periods, which are hundreds of microns. One can use the UV-beam-scanning point-by-point exposure techniques15 to achieve a complex coupling coefficient of the gratings for practical fabrication.

4.

Conclusion

This paper presented the optimization of a spectral flat-top, ultrabroadband thin-clad LPG filter with a single resonant peak in a very wide range of wavelength band (450nm) using the decibel-scale LMO algorithm. For the first time, the spectrum in the 20-dB bandwidth of the designed UBLPG filter can be broadened beyond 180nm by using the proposed of LMO method. This proposed UBLPG also can be utilized as a broadband polarizer when the designed LPG is written in an elliptical core fiber or a birefringent fiber. We believe such a novel UBLPG device will be very useful in applications for ultrabroadband fiber-optics technology.

References

1.  A. M. Vengsarkar, P. J. Lemaire, J. B. Judkins, V. Bhatia, T. Erdogan, and J. E. Sipe, “Long-period fiber gratings as band rejection filters,” J. Lightwave Technol.0733-8724 14, 58–65 (1996). 10.1109/50.476137 Google Scholar

2.  A. M. Vengsarkar, J. R. Pedrazzani, J. B. Judkins, P. J. Lemaire, N. S. Bergano, and C. R. Davidson, “Long-period fiber-grating-based gain equalizers,” Opt. Lett.0146-9592 21, 336–338 (1996). 10.1364/OL.21.000336 Google Scholar

3.  H. Jeong and K. Oh, “Theoretical analysis of cladding-mode waveguide dispersion and its effects on the spectra of long-period fiber grating,” J. Lightwave Technol.0733-8724 21, 1838–1845 (2003). 10.1109/JLT.2003.815641 Google Scholar

4.  H. Jeong and K. Oh, “Enhancement of free spectral range of the resonance peaks in a long-period fiber grating by controlling material dispersion of cladding modes,” Opt. Commun.0030-4018 199, 103–110 (2001). 10.1016/S0030-4018(01)01570-X Google Scholar

5.  S. Yin, K.-W. Chung, and X. Zhu, “A novel all-optic tunable long-period grating using a unique double-cladding layer,” Opt. Commun.0030-4018 196, 181–186 (2001). 10.1016/S0030-4018(01)01396-7 Google Scholar

6.  K.-W. Chung and S. Yin, “Analysis of a widely tunable long-period grating by use of an ultrathin cladding layer and higher-order cladding mode coupling,” Opt. Lett.0146-9592 29, 812–814 (2004). 10.1364/OL.29.000812 Google Scholar

7.  Z. Wang and S. Ramachandran, “Ultrasensitive long-period fiber gratings for broadband modulators and sensors,” Opt. Lett.0146-9592 28, 2458–2460 (2003). 10.1364/OL.28.002458 Google Scholar

8.  S. Ramachandran, Z. Wang, and M. Yan, “Bandwidth control of long-period grating-based mode converters in few-mode fibers,” Opt. Lett.0146-9592 27, 698–700 (2002). 10.1364/OL.27.000698 Google Scholar

9.  S. Ramachandran, M. Yan, E. Monberg, F. V. Dimarcello, P. Wisk, and S. Ghalmi, “Record bandwidth, spectrally flat coupling with microbend gratings in dispersion-tailored fibers,” IEEE Photon. Technol. Lett.1041-1135 15, 1561–1563 (2003). 10.1109/LPT.2003.818625 Google Scholar

10.  C. L. Lee, R. K. Lee, and Y. M. Kao, “Design of multichannel DWDM fiber Bragg grating filters by Lagrange multiplier constrained optimization,” Opt. Express1094-4087 14, 11002–11011 (2006). 10.1364/OE.14.011002 Google Scholar

11.  C. L. Lee, R. K. Lee, and Y. M. Kao, “Synthesis of long-period fiber gratings with a Lagrange multiplier optimization method,” Opt. Commun.0030-4018 281, 61–74 (2008). 10.1016/j.optcom.2007.08.069 Google Scholar

12.  C. L. Lee, R. K. Lee, and Y. M. Kao, “Lagrange multiplier constrained optimization for designing narrowband dispersionless fiber bragg gratings,” Opt. Eng.0091-3286 47, 015005 (2008). 10.1117/1.2835461 Google Scholar

13.  T. Erdogan, “Fiber grating spectra,” J. Lightwave Technol.0733-8724 15, 1277–1294 (1997). 10.1109/50.618322 Google Scholar

14.  J. W. Fleming, “Dispersion in GeO2SiO2 glasses,” Appl. Opt.0003-6935 23(24), 4486–4493 (1984). 10.1364/AO.23.004486 Google Scholar

15.  A. I. Kalachev, D. N. Nikogosyan, and G. Brambilla, “Long-period fiber grating fabrication by high-intensity femtosecond pulses at 211nm,” J. Lightwave Technol.0733-8724 23, 2568–2578 (2005). 10.1109/JLT.2005.851335 Google Scholar

© (2009) Society of Photo-Optical Instrumentation Engineers (SPIE)
Cheng-Ling Lee, Pin Han, "Optimal design of single resonant and ultrabroadband long-period fiber grating filters," Optical Engineering 48(8), 080501 (1 August 2009). https://doi.org/10.1117/1.3194285 . Submission:
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