We demonstrate photonic crystal fibers with ultra-flattened, near zero dispersion. Two micro-structured fibers showing dispersion of 0 ± 0.6 ps/nm.km from 1.24 μm-1.44 μm wavelength and 0 ± 1.2 ps/nm.km over 1 μm-1.6 μm wavelength have been measured.
© 2002 Optical Society of America
Photonic crystal fiber (PCF) is formed from a strand of silica glass with an array of microscopic air channels running along its length . A guiding core can be created by filling one channel with glass. In conventional step-index fibers, group velocity dispersion (GVD) is usually dominated by the dispersion of the bulk silica. In PCF, however, the additional design parameters of hole diameter, d, and hole-to-hole spacing, Λ, enable much greater flexibility in the design of dispersion to suit the required application. For example, PCFs have been reported with zero GVD point shifted to the green – in conventional step-index fibers the zero dispersion wavelength is at ~1.3 μm. These unusual fibers have very small cores and are very efficient at generating supercontinuum light from fsec Ti:Sapphire laser pulses [2,3].
PCFs with zero dispersion wavelengths around the 1.5 μm communications window have also recently been demonstrated . However, these fibers have significant higher-order dispersion (around 0.25 ps/nm2.km). Here we present PCF that has flattened, near zero, dispersion over a very much wider wavelength range – from 1 μm to 1.6 μm. These fibers have many potential uses such as optical parametric amplification  and supercontinuum generation in the infrared .
2. PCF With Near Zero Flattened Dispersion
PCF with ultra-flattened dispersion is investigated numerically in two papers by Ferrando et al. [7,8]. By optimizing d and Λ, they predicted that it is possible to create a PCF with a dispersion of ±1 ps/nm.km over a wavelength range of 543 nm centered at approximately 1.52 μm (d ≈ 0.73 μm, Λ ≈ 3.02 μm). Alternatively, a dispersion of D = ±0.5 ps/nm.km could be achieved over a wavelength range of 428 nm (d ≈ 0.63μm, Λ ≈ 2.64μm).
The fabrication of this type of PCF is non-trivial because the required hole diameters are sub-micron. Standard PCF fabrication  involves stacking silica capillaries into a hexagonal close packed structure, and replacing the central capillary with a glass rod to form a solid core. The unwanted holes between the capillaries tend to deform the structure when they collapse – normally a negligible effect with large-hole PCF. In fibers with ultra-low dispersion, however, precise control of hole shape, size, pitch and core diameter is essential.
3. Experimental Results
In our first fiber we targeted a hole diameter of d ≈ 0.63 μm and a pitch Λ ≈ 2.64 μm, these values being suggested by the numerical modeling. It contained 186 holes, and the target values were attained using an iterative fabrication process. After each draw d and Λ were determined using scanning electron microscopy and the dispersion measured using a low coherence interferometric technique . Figure 1 shows electron micrographs of one of the fibers.
Figure 2 shows the measured dispersion for a selection of different PCFs. Even though the hole size and pitch were within a few percent of the ideal dimensions (d ≈ 0.63 μm, Λ ≈ 2.55 μm), the experimental results did not match those predicted by Ferrando et al (figure 2).
Our explanation for the discrepancy in GVD is that the guided mode was not sufficiently well confined. Modeling showed that in order for the fiber dispersion to converge towards that of a fiber with infinite cladding at least 8 periods would be required. Another fiber was therefore made, this time with 455 holes (corresponding to 11 complete periods between the core and the external jacket). Fig. 3 shows an electron micrograph of this second PCF.
Figure 4 shows the dispersion plots for two 235 mm sections of fiber from this preform. The first fiber had Λ = 2.47 μm and an average d of 0.57 μm (standard deviation 0.06 μm) and the second had Λ = 2.59 μm and an average d of 0.58 μm (standard deviation 0.05 μm). Compared to bulk silica, which has a dispersion of -40 ps/nm.km at 1000 nm and 25 ps/nm.km at 1600 nm, the measured dispersion is exceptionally low over a very broad band of wavelengths. The dispersion slope is also very low. At 1000 nm the slope is 0.017 ps/nm2.km (bulk silica, 0.22 ps/nm2.km) and at 1550 nm it is -0.003 ps/nm2.km (bulk silica, 0.065 ps/nm2.km). Measuring the GVD up to 1640 nm was easy even with significant bending of the fiber, and bend loss in the wavelength range 400 nm to 1750 nm was not measurable down to a radius of curvature of 17.5 mm. The numerical apertures (NA) of the fibers were measured to be approximately 0.23 at 1500 nm, confirming that the modal confinement was relatively good. Losses at 1500 nm were measured to be of the order of 2 dB/m. Numerical modeling by the multipole method [10, 11] predicted that a PCF with Λ = 2.59 μm and d of 0.59 μm would have a non-linear effective area of 44μm2, a NA of 0.21 and a confinement loss of 0.57 dB/m for 11 periods at 1500 nm. This loss reduces by a factor of 2.8 for each extra ring of holes.
Small, slow fluctuations in fiber diameter occur unavoidably during the draw, so that the interhole spacing will vary along the length. Typically, in an optimized fiber draw we find that these variations are of the order of 1%, and that the primary result is a simple scaling of the size of the structure. The dispersion and dispersion slope at 1500nm were calculated for a range of fiber parameters (pitch from 2.1 μm to 2.7 μm and d/Λ from 0.8 to 1.6). Figure 5a shows the dispersion and figure 5b the dispersion slope, both for a wavelength of 1500 nm.
Assuming a 5% variation in pitch along the length of the fiber (with an average Λ=2.59μm, an average d of 0.59 and keeping the ratio d/Λ constant), the average dispersion was found to be D = - 0.56 ps/nm.km. This becomes negligible for a deviation of the order of 1%. For the same 5% variation, the average dispersion slope is found to be 9.98×10-4 ps/nm2.km. Additionally, as the hole diameter to pitch ratio is less than 0.4, the fiber is predicted to be endlessly single mode .
We have reported numerical and experimental results on two photonic crystal fibers with ultra-flattened GVD, the first with D = 0 ± 0.6 ps/nm.km over the range 1.24 μm to 1.44 μm and the second with D = 0 ± 1.2 ps/nm.km over the range 1 μm to 1.6 μm range. With further optimisation of the structure and better control of the fluctuations in fiber diameter, we expect these dispersion values to be reduced still further.
References and Links
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