• Photonics Research
  • Vol. 2, Issue 2, 59 (2014)
Jin Hou1、*, Jiajia Zhao1, Chunyong Yang1, Zhiyou Zhong1, Yihua Gao2, and and Shaoping Chen1
Author Affiliations
  • 1Hubei Key Laboratory of Intelligent Wireless Communications, College of Electronics and Information Engineering, South-central University for Nationalities, Wuhan, Hubei 430074, China
  • 2Wuhan National Laboratory for Optoelectronics (WNLO), School of Physics, Huazhong University of Science and Technology, Wuhan, Hubei 430074, China
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    DOI: 10.1364/PRJ.2.000059 Cite this Article Set citation alerts
    Jin Hou, Jiajia Zhao, Chunyong Yang, Zhiyou Zhong, Yihua Gao, and Shaoping Chen. Engineering ultra-flattened-dispersion photonic crystal fibers with uniform holes by rotations of inner rings[J]. Photonics Research, 2014, 2(2): 59 Copy Citation Text show less

    Abstract

    Wepresent a novel method for engineering ultra-flattened-dispersion photonic crystal fibers with uniform air holes by rotations of inner air-hole rings around the fiber core. By choosing suitable rotation angles of each inner ring, theoretical results show that normal, anomalous, and nearly zero ultra-flattened-dispersion fibers in wide spectra ranges of interest can be obtained alternatively. Moreover, in our dispersion sensitive analysis, these types of fibers are robust to variations from optimal design parameters. The method is suitable for the accurate adjustment of fiber dispersion within a small range, which would be valuable for the fabrication of ultra-flattened-dispersion fibers and also have potential applications in wide-band high-speed optical communication systems.

    1. INTRODUCTION

    In high-speed optical communication systems, fiber dispersion is a crucial factor that has great influence on the bandwidth of information transmission. Conventionally, in order to decrease the dispersion effect, dispersion-shifted fiber and zero-dispersion single-mode fiber are designed for communication wavelengths. In recent years, photonic crystal fiber (PCF) [1], has became a preeminent method for transmitting information because of its unique optical properties and flexible designs. The variety of possible geometries in PCF offers great possibility to control its dispersion properties, particularly useful in designing dispersion flattened fibers over a wide range of wavelengths.

    Over the last decade, various PCFs have been proposed and studied to obtain ultra-flattened-dispersion property. Initially, characterized by the lattice constant and hole diameter, relative flattened dispersion can be achieved [2,3]. After that, in order to improve dispersion flatness over a wider bandwidth, more complicated design methods have been exploited, such as doping additional materials such as GeO2 in the central part of the silica core [4,5], changing the diameter of the air holes belonging to the first two or three inner rings [6,7], modifying the circular air holes into other shapes [810], selectively filling the PCF with liquids [11], designing a hybrid core region with three-fold symmetry for the fiber [12], assembling additional defected air holes in the central core region [13], or combining two or more of these methods, for instance, introducing both GeO2-or F-doped silica and also modifying the circular holes into hollow rings in the PCFs [14]. While wonderful dispersion flatness performance could be obtained, the modifications either broke the uniformity of the holes’ size or introduced additional materials, which will raise complexity during the design of fibers. In addition, minor variations of these design parameters that would be introduced in the fabrication process are likely to cause a large change of the dispersion characteristic. Therefore, the realization of ultra-flattened-dispersion PCFs with low sensitivity by a relatively simple method is still a challenge.

    In this paper, we propose a novel design approach for achieving ultra-flattened-dispersion PCFs over wide wavelength regions with low sensitivity just by rotations of two inner air-hole rings around the fiber core. The approach can obtain ultra-flattened-dispersion PCFs while maintaining the uniformity of the PCFs’ air-hole size. Numerical results show that our proposed method for control of dispersion in PCFs works well. The paper is organized as follows. In Section 2, the topology and design principle of proposed PCFs are presented. Then, in Section 3, dispersion engineering for nearly zero-dispersion PCFs, normal dispersion PCFs, and abnormal dispersion PCFs is investigated in detail. In Section 4, a sensitive analysis is performed to determine the variations of the dispersion characteristic arising from inevitable imprecision angles of the inner rings. Finally, conclusions are given in Section 5.

    2. SCHEMATIC TOPOLOGY AND DESIGN PRINCIPLE

    The schematic cross section of the proposed PCF topology structure is depicted in Fig. 1. The host material is pure silica, and the number of air-hole rings is assumed to be 11. It is composed of circular air holes arranged in a triangular array of lattice constant Λ with the central air hole missing, and all air holes have a uniform diameter d. As denoted in the right panel of Fig. 1, the central core area of the fiber is additionally modified by rotations of the innermost two air-hole rings around the fiber core with angles of α degrees and β degrees relative to their original positions to obtain ultra-flattened dispersion, respectively. And the original positions of air holes in the inner two rings are also denoted in the right panel of Fig. 1 as dashed circles.

    Schematic topology of the proposed PCFs structure. The air holes in the silica background are arranged in a triangular configuration of lattice constant Λ with the central air hole missing, and all air holes have a uniform diameter d. The first and second innermost air-hole rings (colored green and yellow, respectively) are rotated around the fiber core with angles of α degrees and β degrees relative to their original positions, respectively. And the original positions of air holes in the inner rings are denoted as dashed circles in the right panel.

    Figure 1.Schematic topology of the proposed PCFs structure. The air holes in the silica background are arranged in a triangular configuration of lattice constant Λ with the central air hole missing, and all air holes have a uniform diameter d. The first and second innermost air-hole rings (colored green and yellow, respectively) are rotated around the fiber core with angles of α degrees and β degrees relative to their original positions, respectively. And the original positions of air holes in the inner rings are denoted as dashed circles in the right panel.

    It is clear that there are four structure parameters, namely Λ, d, α, and β, which can be tuned to achieve the ultra-flattened-dispersion PCFs. Hence, our design strategy is performed in two steps. First, relatively dispersion flattened PCFs are obtained by varying parameters Λ and d [3]. Then, we try to tailor the dispersion of PCFs further by carefully adjusting both α and β. A plane-wave expansion method with a lattice resolution of 32 is employed to obtain highly accurate dispersion values of the fundamental mode of fibers in the numerical calculations [15]. And the material dispersion is directly included in the calculations through the Sellmeier equation. In order to get a highly accurate result, a minimum change step of 1° is adopted near the optimum structure parameters.

    3. DISPERSION ENGINEERING AND ANALYSIS

    In this section, we will show how to realize nearly zero-dispersion ultra-flattened PCF, normal dispersion ultra-flattened PCF, and anomalous dispersion ultra-flattened PCF through dispersion engineering by our proposed topology. We start from the achievement of nearly zero-dispersion ultra-flattened PCF. As mentioned in Section 2, first, relatively flattened zero-dispersion PCF is obtained by choosing appropriate parameters Λ and d. We know the total dispersion D is approximately equal to the sum of the geometrical dispersion Dg and material dispersion Dm, that is, D(λ)Dg(λ)+Dm(λ)Dg(λ)(Dm(λ)), and the slope of the Dm curve being fixed. Through performing a scaled Dg curve having a liner resign with the same slope as Dm, and meanwhile ensuring the wavelength region where Dm behaves linearly overlaps the wavelength region of linear behavior of Dg, we will obtain an ultra-flattened-dispersion curve D in the overlapping wavelength range. Reference [3] has given the results that, by fixing d/Λ and changing Λ, the curve of Dg is shifted, and the slope of its linear part is modified. Meanwhile, by fixing Λ and changing d the curve of Dg is shifted, but the slope of its linear part is approximately preserved. According to the above conclusion, coupled with a further calculation, Λ=2.3μm and d=0.61μm are chosen. Second, dispersion is further optimized by engineering the parameters α and β. Thus, the influence exerted by parameters α and β on the dispersion characteristic should be investigated in detail.

    Before optimizing, the tuning ranges of α and β should be determined first. Due to the geometric symmetry of the proposed PCF structure, if we only take one of the parameters α and β as the variation parameter and fix the other, a variation range with a minimum period of 30° should be enough to represent all the cases of angle variations. For example, when β is fixed with 0°, variation of α within 0° to 30° is enough. However, if we take α and β simultaneously as tuning factors, an angle variation range of 60° should be required. Specifically, when one of the parameters has a symmetric angle, it is equal to the case of variation of only one parameter. Thus, an angle variation range for the other parameter of 30° would be enough for one of the parameters maintained at the symmetric angle. For example, when β is 30°, variation of α within 0° to 30° is also enough.

    Figure 2 plots the chromatic dispersion D as a function of the wavelength λ. Figure 2(a) shows the chromatic dispersion dependence on the change of parameter α, while β is fixed with original degree. And Fig. 2(b) shows the chromatic dispersion dependence on the change of parameter β, while α is fixed. From Fig. 2, it is evident that when increasing α or β separately from 0° to 30°, the curves all shift upward. So variation of α or β will lead to a similar dispersion changing tendency. And as the curve shifts upward, the chromatic dispersion curve becomes flatter since the peak at shorter wavelength increases slower than the valley rising at longer wavelength.

    Chromatic dispersion D as a function of wavelength λ with Λ=2.3 μm and d=0.61 μm for changing one of the design parameters: (a) α is changing from 0° to 30°, while β is fixed, and (b) β is changing from 0° to 30°, while α is fixed.

    Figure 2.Chromatic dispersion D as a function of wavelength λ with Λ=2.3μm and d=0.61μm for changing one of the design parameters: (a) α is changing from 0° to 30°, while β is fixed, and (b) β is changing from 0° to 30°, while α is fixed.

    Comparing Figs. 2(a) and 2(b), while the impact of β on the chromatic dispersion in the long wavelength zone is much greater than that of α, the impact of β on the dispersion in the short wavelength zone is less sensitive. The reason can be explained as follows. Since the innermost ring is much nearer to the fiber central core than the second innermost ring, the short wavelengths at first can only have a serious influence on the innermost ring, and they have less influence on the second innermost ring. As wavelength increases, the light can penetrate the first innermost ring and could have a direct influence on the second innermost ring too. So variation of the second innermost ring will heavily affect the optical properties of fiber in the long wavelength zone. As shown in Fig. 3, it also can be explained by the transverse electric field intensity distributions of the fundamental mode for both short wavelength and long wavelength. Figure 3(a) shows the transverse electric field intensity distribution of the fundamental mode at 1.45 μm for the original PCF, which is with both α and β equal to 0°, and Figs. 3(b) and 3(c) show the electric field intensity distributions at the same wavelength for the maximum variations of α and β, respectively. Correspondingly, Figs. 3(d), 3(e), and 3(f) show the electric field intensity distributions at 1.75 μm wavelength for these three structure cases as in Figs. 3(a), 3(b), and 3(c). As wavelength increases, it is clear that variation of the second innermost ring leads to more mode-field distribution penetrating to the cladding compared to the variation of the first inner ring. Thus, the chromatic dispersion is very sensitive to β. Therefore we first use β for a coarse tuning; then, we fix β with a relative optimized value and use α for an accurate tuning to obtain wide-band ultra-flattened nearly zero dispersion. Here, we focus on the chromatic dispersion curve with the lowest fluctuation for a wavelength range from 1.25 to 1.65 μm. As shown in Fig. 2(b), through a preliminary engineering, β=20° is selected as the parameter for the proposed nearly zero-dispersion flattened PCF.

    Fundamental mode transverse electric field intensity (Et2) distributions at 1.45 μm (upper figures) and 1.75 μm (lower figures) wavelengths, for nearly zero-dispersion flattened PCFs with Λ=2.3 μm and d=0.61 μm for (a) α=0° and β=0°, (b) α=30° and β=0°, (c) α=0° and β=30°, (d) α=0° and β=0°, (e) α=30° and β=0°, and (f) α=0° and β=30°.

    Figure 3.Fundamental mode transverse electric field intensity (Et2) distributions at 1.45 μm (upper figures) and 1.75 μm (lower figures) wavelengths, for nearly zero-dispersion flattened PCFs with Λ=2.3μm and d=0.61μm for (a) α=0° and β=0°, (b) α=30° and β=0°, (c) α=0° and β=30°, (d) α=0° and β=0°, (e) α=30° and β=0°, and (f) α=0° and β=30°.

    Then we investigate the combined influence of α and β for a final optimization of nearly zero-dispersion fiber. Figure 4 shows the variations of the chromatic dispersion versus wavelength λ for changing α from 0° to 59° with optimized β=20°. While increasing α from 0° to 20°, the dispersion curve shifts down first and gets the lowest at 20°. Continuously increasing α from 20° to 50°, the dispersion curve tends to rise up and gets the highest at 50°. Finally, increasing α from 50° to 59°, the dispersion curve tends to shift downward again and gets close to its original position. This can be explained as follows. As α increases from 0° with a fixed β=20°, the difference between β and α, i.e., |βα|, first tends to be smaller, and thus its variation on dispersion becomes weaker, so the dispersion curve shifts downward before α reaches 20°. On the contrary, once |βα| gets bigger again, its variation on dispersion becomes stronger again, so the dispersion curve shifts upward again and gets to the highest extreme at α with 50°, which is equal to the maximum |βα| of 30°. Finally, the optimum dispersion curve can be obtained with α=0° and β=20°, and its dispersion variations are within 1.2±0.6ps/(km·nm) in a wavelength range of 1.25–1.65 μm. So we can see that the flatness of dispersion is finely tuned by adjusting parameters β and α.

    Chromatic dispersion D as a function of wavelength λ with Λ=2.3 μm and d=0.61 μm for changing α from 0° to 59°, while β has an optimized value of 20°.

    Figure 4.Chromatic dispersion D as a function of wavelength λ with Λ=2.3μm and d=0.61μm for changing α from 0° to 59°, while β has an optimized value of 20°.

    After the design of nearly zero ultra-flattened-dispersion PCF, normal ultra-flattened-dispersion PCF and anomalous ultra-flattened-dispersion PCF are also proposed. The suitable lattice constant and hole diameter have also been chosen for them, which have the values of Λ=2.7μm, d=0.75μm and Λ=2.2μm, d=0.54μm, respectively. The method we used to choose these parameters for the normal flattened-dispersion PCF and anomalous flattened-dispersion PCF is the same as that for zero ultra-flattened-dispersion PCF. Then based on previous experience deduced from the design of zero ultra-flattened-dispersion PCF, the optimum normal and anomalous ultra-flattened-dispersion curves are all easily achieved.

    In Fig. 5, we show the calculated chromatic dispersion for changing α or β while reserving the other parameters. In the figure, the black solid curve represents the chromatic dispersion of the initial fiber with α=0° and β=0°. The blue solid curves with various geometric shapes show the chromatic dispersion dependence on the changing α, while β is unchanged. The red dashed-dotted curves with various geometric shapes describe the chromatic dispersion dependence on the changing parameters β, while α is unchanged. The impact of structure parameters changing on chromatic dispersion shown in Fig. 5(b) is similar to what we have shown in Fig. 2. Parameter β has much greater influence on the chromatic dispersion than α does in the long wavelength zone, while in the short wavelength zone, α has comparable impact on the dispersion compared with β. However, for Fig. 5(a), the situation changes much. For the short wavelength zone, in spite of changing α and β, the chromatic dispersion is changed minimally. And when the wavelength is beyond a specific value, the dispersion curve becomes sensitive to the structure parameters. First, it is much more sensitive to the changing of the innermost ring. And as the wavelength increases to the long wavelength zone, the second innermost ring also plays an important role in controlling the fiber dispersion. The phenomena can be understood similar to what we explained for the nearly zero-dispersion PCF in the previous part. The different sensitivities found in these figures would mainly arise from the different period Λ, which we have chosen to obtain different kinds of chromatic dispersion behaviors. For Figs. 2 and 5(b), their periods are 2.3 and 2.2 μm, respectively. So, the dispersion behavior shown in these figures is similar. However, for Fig. 5(a), a large period of 2.7 μm is adopted. Therefore, only longer wavelengths are sensitive to the change of α and β.

    Chromatic dispersion D as a function of the wavelength λ, for changing structure parameters α or β from 0° to 30° while reserving the other parameters, for (a) normal ultra-flattened-dispersion PCF with Λ=2.7 μm and d=0.75 μm, and (b) abnormal ultra-flattened-dispersion PCF with Λ=2.2 μm and d=0.54 μm.

    Figure 5.Chromatic dispersion D as a function of the wavelength λ, for changing structure parameters α or β from 0° to 30° while reserving the other parameters, for (a) normal ultra-flattened-dispersion PCF with Λ=2.7μm and d=0.75μm, and (b) abnormal ultra-flattened-dispersion PCF with Λ=2.2μm and d=0.54μm.

    From the results shown in Fig. 5(a), β=16° is selected as the preliminary parameter for the proposed normal dispersion flattened PCF in a wavelength range of 1.5–2.0 μm. While from the curves shown in Fig. 5(b), β=22° is selected as the preliminary parameter for the proposed anomalous dispersion flattened PCF in a wavelength range of 1.25–1.65 μm.

    After that, a final optimizing process for normal ultra-flattened-dispersion PCF and anomalous ultra-flattened-dispersion PCF is also shown in Figs. 6(a) and 6(b). We note that when α increases from 0° to 59°, the curves changing tendency shown in Figs. 6(a) and 6(b) are similar to what we have shown in Fig. 4. In the end, the optimum parameters of α=0° and β=16° are selected for the normal ultra-flattened-dispersion PCF, and its corresponding dispersion variations are within 21.1±0.7ps/(km·nm) in the wavelength range of 1.5–2.0 μm. Also, the optimum parameters of α=57° and β=22° are selected for the anomalous ultra-flattened-dispersion PCF, and its corresponding dispersion variations are 11.1±0.8ps/(km·nm) in the wavelength range of 1.25–1.65 μm.

    Chromatic dispersion as a function of the wavelength λ, for the changing α (a) normal ultra-flattened-dispersion PCF with β=16°, Λ=2.7 μm, and d=0.75 μm, and (b) abnormal ultra-flattened-dispersion PCF with β=22°, Λ=2.2 μm, and d=0.54 μm.

    Figure 6.Chromatic dispersion as a function of the wavelength λ, for the changing α (a) normal ultra-flattened-dispersion PCF with β=16°, Λ=2.7μm, and d=0.75μm, and (b) abnormal ultra-flattened-dispersion PCF with β=22°, Λ=2.2μm, and d=0.54μm.

    4. SENSITIVE ANALYSIS

    In the previous sections, various kinds of ultra-flattened-dispersion PCFs with uniform air holes have been theoretically realized by rotations of inner two air-hole rings around the core with specific angles. But considering the inevitable imprecision that would be introduced during the fabrication process, it may affect the dispersion characteristics of the proposed PCFs. Thus, sensitive analysis regarding the impact of the fluctuation of the design parameters on the dispersion characteristics should be performed.

    Due to the fact that the PCFs can be fabricated with high lattice uniformity and with high precision to the cladding hole diameter [13,16], we only focus our sensitive analysis on the air-hole positions of the inner two rings due to inaccurate angles of the rings. Here, taking the ultra-flattened zero-dispersion PCF for example, a set of calculations is performed to show the impact of variation of α or β on the chromatic dispersion, in which either α or β or α and β is deviated ±3°, from the optimum point α=0° and β=22°. As plotted in Fig. 7, we note even in the extreme condition that α deviated 3° and β has the inverse change; the maximum variation of dispersion is still within 1.05ps/(km·nm) around the nominal dispersion value. In fact, according to the fabrication date in Ref. [16], the extreme situation will not be likely to occur in our cases. As a result, we can draw a conclusion that possible variations of the design parameters of the proposed fibers will not influence the dispersion property much.

    Chromatic dispersion D as a function of the wavelength λ with Λ=2.3 μm and d=0.61 μm; α or/ and β are varied from their optimum values of α=0° and β=20°.

    Figure 7.Chromatic dispersion D as a function of the wavelength λ with Λ=2.3μm and d=0.61μm; α or/ and β are varied from their optimum values of α=0° and β=20°.

    Further research is also carried out to figure out why the fiber is not sensitive to fluctuations of the optimum design parameters. The impact of variations of optimum parameters α and β on the effective mode area of the fundamental mode is calculated and analyzed. The design parameters that we choose are the same as in Fig. 7, and their corresponding effective mode areas at the wavelength of 1.55 μm are given in Table 1. It is easy to find the correspondence between the effective mode area and the chromatic dispersion curve. As the effective mode area increases, the chromatic dispersion shifts up. The largest variation of effective mode area and the largest variation of dispersion have the same parameters. And even in the worst condition, the maximum variation of effective mode area to the nominal value is only 0.5441μm2. Therefore, it is easy to say that the fiber is not sensitive to fluctuations of its optimum design parameters. Thus, our proposed fiber is a robust design.

    α[°]β[°]Aeff[μm2]
    02031.7186
    0+020+331.8863
    0+020331.3310
    0+320+031.5597
    0320+031.8842
    0+320331.1745
    0320+332.0136
    0+320+331.7454
    0320331.5134

    Table 1. Effective Mode Areas at λ=1.55μm for Different Parameters with Λ=2.3μm and d=0.61μm

    5. CONCLUSIONS

    In conclusion, we have demonstrated a novel method for realizing ultra-flattened-dispersion PCFs with uniform air holes by rotations of each inner air-hole ring wholly around the fiber core. It only uses four parameters, namely Λ, d, α, and β, to control the dispersion of PCFs. Λ and d take charge of the regulation of dispersion in a wide range, while α and β are responsible for the accurate adjustment of dispersion in a small range. Theoretical results show that nearly zero, normal, and anomalous ultra-flattened-dispersion fibers in wide spectra ranges of interest all can be obtained. These proposed fibers reduce the difficulty of designs compared to that with multiple different submicrometer air-hole sizes or introduce other kinds of materials. Sensitive analysis also shows that possible fluctuation of design parameters will not affect the desired dispersion property seriously. Moreover, this method can work as a companion for the existing dispersion tailoring technologies to accurately adjust dispersion within a small range. Thus, we believe our proposed fiber structure is a robust design, which would have potential applications in wide-band high-speed optical communication systems.

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    Jin Hou, Jiajia Zhao, Chunyong Yang, Zhiyou Zhong, Yihua Gao, and Shaoping Chen. Engineering ultra-flattened-dispersion photonic crystal fibers with uniform holes by rotations of inner rings[J]. Photonics Research, 2014, 2(2): 59
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