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Optics Express

Optics Express

  • Editor: Michael Duncan
  • Vol. 10, Iss. 14 — Jul. 15, 2002
  • pp: 609–613
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Demonstration of ultra-flattened dispersion in photonic crystal fibers

W.H. Reeves, J.C. Knight, P.St.J. Russell, and P.J. Roberts  »View Author Affiliations


Optics Express, Vol. 10, Issue 14, pp. 609-613 (2002)
http://dx.doi.org/10.1364/OE.10.000609


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Abstract

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

1. Introduction

Photonic crystal fiber (PCF) is formed from a strand of silica glass with an array of microscopic air channels running along its length [1

1. J.C. Knight, T.A. Birks, P.St.J. Russell, and D.M. Atkin, “All-silica single-mode optical fiber with photonic crystal cladding,” Opt. Lett. 21, 1547 (1996) [CrossRef] [PubMed]

]. 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

2. W.J. Wadsworth, A. Ortigosa-Blanch, J.C. Knight, T.A. Birks, T-P.M. Man, and P.St.J. RussellSupercontinuum generation in photonic crystal fibers and optical fiber tapers – A novel light source,” J. Opt. Soc. Am. B in press, (2002). [CrossRef]

,3

3. J.C. Knight, J. Arriaga, T.A. Birks, A. Ortigosa-Blanch, W.J. Wadsworth, and P.St.J Russell, “Anomalous dispersion in photonic crystal fiber,” IEEE Photon. Technol. Lett. 12, 807–809 (2000) [CrossRef]

].

PCFs with zero dispersion wavelengths around the 1.5 μm communications window have also recently been demonstrated [4

4. K.P. Hansen, J.R. Jensen, C. Jacobsen, H.R. Simonsen, J. Broeng, P.M.W. Skovgaard, A. Peterson, and A. Bjarklev, “Highly Nonlinear Photonic Crystal Fiber with Zero-Dispersion at 1.55μm,” in Optical Fiber Commenication 2002, Vol. 70 of OSA Trends in Optics and Photonics Series (Optical Society of America, Washington, D.C., 2002), paper FA9.

]. 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 [5

5. J. Hansryd and P.A. Andrekson, “Broad-Band Continuous-Wave-Pumped Fiber Optical Parametric Amplifier with 49-dB Gain and Wavelength-Conversion Efficiency,” IEEE Photon. Technol. Lett. 13, 194 (2001) [CrossRef]

] and supercontinuum generation in the infrared [6

6. Y. Takushima and K Kikuchi, “10-GHz, Over 20-Channel Multiwavelength Pilse Source by Slicing Super-Continuum Spectrum Generated in Normal-Dispersion Fiber”, IEEE Photon. Technol. Lett. 11, 322, (1999) [CrossRef]

].

2. PCF With Near Zero Flattened Dispersion

PCF with ultra-flattened dispersion is investigated numerically in two papers by Ferrando et al. [7

7. A. Ferrando, E. Silvestre, J.J. Miret, and P. Andres, “Nearly zero ultraflattened dispersion in photonic crystal fibers,” Opt. Lett. 25, 790 (2000) [CrossRef]

,8

8. A. Ferrando, E. Silvestre, and P. Andres, “Designing the properties of dispersion-flattened photonic crystal fiber,” Opt. Express 9, 687 (2001) http://www.opticsexpress.org/abstract.cfm?URI=OPEX-9-13-687 [CrossRef] [PubMed]

]. 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 [1

1. J.C. Knight, T.A. Birks, P.St.J. Russell, and D.M. Atkin, “All-silica single-mode optical fiber with photonic crystal cladding,” Opt. Lett. 21, 1547 (1996) [CrossRef] [PubMed]

] 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 [9

9. M. Tateda, N. Shibata, and S. Seikai, “Interferometric method for chromatic dispersion measurement in a single-mode optical fiber,” IEEE J. Quantum Electron. QE-17, 404 (1981) [CrossRef]

]. Figure 1 shows electron micrographs of one of the fibers.

Fig. 1 A photonic crystal fiber with 7 periods in the cladding and with Λ ≈ 2.5μm and d ≈ 0.5μm.

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).

Fig. 2. Measured dispersion for a selection of 7-period PCFs. Although the theoretical ideal fiber parameters were almost reached, the experimental and theoretical results did not match.

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.

Fig. 3. Ultra-flattened dispersion photonic crystal fiber with 11 periods. Λ = 2.47μm and an average d of 0.57μm.

Fig. 4. Measured dispersion plots for ultra flattened dispersion PCF similar to the fiber shown in figure 3. Red curve: d = 0.58, Λ = 2.59, dark blue curve: d= 0.57, Λ=2.47.

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 [12

12. T.A. Birks, J.C. Knight, and P.St.J. Russell, “Endlessly single-mode photonic crystal fiber,” Opt. Lett. 22, 961 (1997) [CrossRef] [PubMed]

].

Fig. 5. (a) shows the value of dispersion for variation of hole radius and pitch for a wavelength of 1500 nm. The black line represents zero dispersion. For the same fiber parameters (b) shows the value of the dispersion slope for a wavelength of 1500 nm. The black line represents zero slope. In both graphs the “×” shows the fiber parameters of the PCF with Λ = 2.47 μm and an average d of 0.57 μm and the “+” shows the PCF with Λ = 2.59 μm and an average d of 0.58 μm.

4. Conclusions

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

1.

J.C. Knight, T.A. Birks, P.St.J. Russell, and D.M. Atkin, “All-silica single-mode optical fiber with photonic crystal cladding,” Opt. Lett. 21, 1547 (1996) [CrossRef] [PubMed]

2.

W.J. Wadsworth, A. Ortigosa-Blanch, J.C. Knight, T.A. Birks, T-P.M. Man, and P.St.J. RussellSupercontinuum generation in photonic crystal fibers and optical fiber tapers – A novel light source,” J. Opt. Soc. Am. B in press, (2002). [CrossRef]

3.

J.C. Knight, J. Arriaga, T.A. Birks, A. Ortigosa-Blanch, W.J. Wadsworth, and P.St.J Russell, “Anomalous dispersion in photonic crystal fiber,” IEEE Photon. Technol. Lett. 12, 807–809 (2000) [CrossRef]

4.

K.P. Hansen, J.R. Jensen, C. Jacobsen, H.R. Simonsen, J. Broeng, P.M.W. Skovgaard, A. Peterson, and A. Bjarklev, “Highly Nonlinear Photonic Crystal Fiber with Zero-Dispersion at 1.55μm,” in Optical Fiber Commenication 2002, Vol. 70 of OSA Trends in Optics and Photonics Series (Optical Society of America, Washington, D.C., 2002), paper FA9.

5.

J. Hansryd and P.A. Andrekson, “Broad-Band Continuous-Wave-Pumped Fiber Optical Parametric Amplifier with 49-dB Gain and Wavelength-Conversion Efficiency,” IEEE Photon. Technol. Lett. 13, 194 (2001) [CrossRef]

6.

Y. Takushima and K Kikuchi, “10-GHz, Over 20-Channel Multiwavelength Pilse Source by Slicing Super-Continuum Spectrum Generated in Normal-Dispersion Fiber”, IEEE Photon. Technol. Lett. 11, 322, (1999) [CrossRef]

7.

A. Ferrando, E. Silvestre, J.J. Miret, and P. Andres, “Nearly zero ultraflattened dispersion in photonic crystal fibers,” Opt. Lett. 25, 790 (2000) [CrossRef]

8.

A. Ferrando, E. Silvestre, and P. Andres, “Designing the properties of dispersion-flattened photonic crystal fiber,” Opt. Express 9, 687 (2001) http://www.opticsexpress.org/abstract.cfm?URI=OPEX-9-13-687 [CrossRef] [PubMed]

9.

M. Tateda, N. Shibata, and S. Seikai, “Interferometric method for chromatic dispersion measurement in a single-mode optical fiber,” IEEE J. Quantum Electron. QE-17, 404 (1981) [CrossRef]

10.

R.F. Cregan, J.C. Knight, P.St.J. Russell, and P.J. Roberts, “Distribution of spontaneous emission from an Er3+-doped photonic crystal fiber,” 1999, J. Lightwave Tech. 172138–41 [CrossRef]

11.

M.J. Steel, T.P. White, C.M. de Sterke, R.C. McPhedran, and L.C. Botten, “Symmetry and degeneracy in microstructured optical fibers,” 2001, Opt. Lett. 26, 488 [CrossRef]

12.

T.A. Birks, J.C. Knight, and P.St.J. Russell, “Endlessly single-mode photonic crystal fiber,” Opt. Lett. 22, 961 (1997) [CrossRef] [PubMed]

OCIS Codes
(060.2270) Fiber optics and optical communications : Fiber characterization
(060.2280) Fiber optics and optical communications : Fiber design and fabrication
(060.2430) Fiber optics and optical communications : Fibers, single-mode

ToC Category:
Research Papers

History
Original Manuscript: June 7, 2002
Revised Manuscript: June 27, 2002
Published: July 15, 2002

Citation
William Reeves, J. Knight, P. Russell, and P. Roberts, "Demonstration of ultra-flattened dispersion in photonic crystal fibers," Opt. Express 10, 609-613 (2002)
http://www.opticsinfobase.org/oe/abstract.cfm?URI=oe-10-14-609


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References

  1. J.C. Knight, T.A. Birks, P. St.J. Russell, and D.M. Atkin, �??All-silica single-mode optical fiber with photonic crystal cladding,�?? Opt. Lett. 21, 1547 (1996) [CrossRef] [PubMed]
  2. W.J. Wadsworth, A. Ortigosa-Blanch, J.C. Knight, T.A. Birks, T-P.M. Man and P.St.J. Russell, �??Supercontinuum generation in photonic crystal fibers and optical fiber tapers �?? A novel light source,�?? J. Opt. Soc. Am. B in press, (2002). [CrossRef]
  3. J.C. Knight, J. Arriaga, T.A. Birks, A. Ortigosa-Blanch, W.J. Wadsworth, and P.St.J Russell, �??Anomalous dispersion in photonic crystal fiber,�?? IEEE Photon. Technol. Lett. 12, 807-809 (2000) [CrossRef]
  4. K.P. Hansen, J.R. Jensen, C.Jacobsen, H.R. Simonsen, J.Broeng, P.M.W. Skovgaard, A.Peterson and A. Bjarklev, �??Highly Nonlinear Photonic Crystal Fiber with Zero-Dispersion at 1.55µm,�?? in Optical Fiber Commenication 2002, Vol. 70 of OSA Trends in Optics and Photonics Series (Optical Society of America, Washington, D.C., 2002), paper FA9.
  5. J. Hansryd and P.A. Andrekson, �??Broad-Band Continuous-Wave-Pumped Fiber Optical Parametric Amplifier with 49-dB Gain and Wavelength-Conversion Efficiency,�?? IEEE Photon. Technol. Lett. 13, 194 (2001) [CrossRef]
  6. Y. Takushima, and K Kikuchi, �??10-GHz, Over 20-Channel Multiwavelength Pilse Source by Slicing Super- Continuum Spectrum Generated in Normal-Dispersion Fiber,�?? IEEE Photon. Technol. Lett. 11, 322, (1999) [CrossRef]
  7. A. Ferrando, E. Silvestre, J.J. Miret, and P. Andres, �??Nearly zero ultraflattened dispersion in photonic crystal fibers,�?? Opt. Lett. 25, 790 (2000) [CrossRef]
  8. A. Ferrando, E. Silvestre, and P. Andres, �??Designing the properties of dispersion-flattened photonic crystal fiber,�?? Opt. Express 9, 687 (2001) <a href="http://www.opticsexpress.org/abstract.cfm?URI=OPEX-9-13-687">http://www.opticsexpress.org/abstract.cfm?URI=OPEX-9-13-687</a> [CrossRef] [PubMed]
  9. M. Tateda, N. Shibata, and S. Seikai, �??Interferometric method for chromatic dispersion measurement in a single-mode optical fiber,�?? IEEE J. Quantum Electron. QE-17, 404 (1981) [CrossRef]
  10. R.F. Cregan, J.C. Knight, P.St.J. Russell and P.J. Roberts, �??Distribution of spontaneous emission from an Er3+- doped photonic crystal fiber,�?? J. Lightwave Tech. 17 2138-41 (1999) [CrossRef]
  11. M.J. Steel, T.P. White, C.M. de Sterke, R.C. McPhedran and L.C. Botten, �??Symmetry and degeneracy in microstructured optical fibers,�?? Opt. Lett. 26, 488 (2001) [CrossRef]
  12. T.A. Birks, J.C. Knight, and P.St.J. Russell, �??Endlessly single-mode photonic crystal fiber,�?? Opt. Lett. 22, 961 (1997) [CrossRef] [PubMed]

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