NONLINEAR OPTICS: Photonic-crystal fibers are selectively filled with nonlinear liquids

The holes of a photonic-crystal fiber can be filled with optically nonlinear fluids in an arbitrary pattern, leading to versatile devices with properties such as soliton propagation and supercontinuum generation.

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MARIUS VIEWEG, TIMO GISSIBL, and HARALD GIESSEN

The holes of a photonic-crystal fiber can be filled with optically nonlinear fluids in an arbitrary pattern, leading to versatile devices with properties such as soliton propagation and supercontinuum generation.

The concept of filling the holes in a photonic-crystal fiber (PCF) to modify the fiber’s properties has gained a tremendous amount of interest in different optical fields. It is possible to use gases, metals, and liquids as filler materials.1–4 In nonlinear optics, liquids are most interesting because of their potential to generate high optical nonlinearities due to their large nonlinear coefficients. It is highly desirable to combine the structure of a PCF with the nonlinear optical properties of a liquid to gain complete control over dispersion and high nonlinearity simultaneously.5

We have developed a method to selectively fill PCFs with nonlinear liquids such as toluene or carbon tetrachloride (CCl4), and have measured solitonic spectral broadening in these fibers.6 The creation of a liquid waveguide array in a PCF shows the versatility of our technique.

Holes filled by capillary forces

A 3D direct laser-writing technique is used to selectively seal single holes.7 First, all holes are covered with an epoxy polymer (see Fig. 1). In the second step, the polymer is crosslinked by two-photon absorption of a focused femtosecond-laser pulse. The two-photon process allows 3D control over the cured volume such that the size of the voxel scales with the intensity. The challenge of this process is the correct addressing of the holes to avoid affecting the neighboring holes. To conveniently fabricate such fibers, we have automated the direct laser-writing process.

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FIGURE 1. In the fabrication process, the cleaved fiber end is first completely covered with a polymer (a). The polymer is then crosslinked hole by hole using a two-photon process (b). The fiber end is cleaned to prepare it for filling (c).

In the next step of the fabrication process, various liquids can be used to fill the fiber holes, with the choice of liquid limited only by toxicity and transparency. By using carbon disulfide, it is possible to enhance the nonlinearity by a factor of about 200 compared to fused silica. We chose toluene and CCl4 for our experiments because they present a good compromise between nonlinearity and nontoxicity. Also, the refractive indices of toluene and CCl4 are 1.48 and 1.45, respectively, which is slightly higher than the refractive index of the fiber material. Therefore we can use toluene and CCl4 in fibers with a small d/Λ ratio, where the effective refractive index of the holey region becomes similar to fused silica, without losing guiding properties. In particular, CCl4 allows for propagation of the fundamental mode in almost all cases.

The holes are filled by capillary forces. By choosing the appropriate hole diameter, hole-to-hole distance, and liquid, one can adjust the zero-dispersion wavelength for the experiment over a huge wavelength range that spans from the near IR to 600 nm. The 2D structure of a PCF can be utilized to arrange several waveguides in an arbitrary pattern to obtain discrete optical-waveguide arrays with desired properties.

Two different filling patterns

In the first experiment, we closed the holes of a PCF in a ring pattern to create a liquid-waveguide array (see Fig. 2). In a microscope picture of the fiber with the selectively closed holes, the dark open holes (which have a diameter of 2.7 µm) can clearly be seen. The open holes are subsequently filled with toluene. Light from a nanosecond microchip laser emitting at a wavelength of 1064 nm was coupled into the device, and a far-field mode image was taken at the output of the fiber. In a mode image superimposed with a schematic of the filling pattern, one can clearly see several liquid waveguides in the holey region of the fiber, as well as the light which propagates in the regular glass core of the fiber. Due to the large hole diameter and the 1064 nm wavelength, higher-order modes are excited.

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FIGURE 2. Numerous versions of selectively closed and filled PCFs have been created. A microscope image shows a PCF with selectively closed holes with the initials of the 4th Physics Institute (a). The hole diameter is 2.5 µm and the hole-to-hole distance is 2.6 µm. A similar fiber is shown but with holes closed in a checkerboard pattern (b). A scanning-electron-microscope image reveals the high-quality seal of the holes (c). A different PCF has hole diameters of 2.7 µm and a hole-to-hole distance of 5.6 µm with a ring structure (d). In a toluene-filled version of the structure shown in (d), the liquid is visible; the darker holes are closed and therefore still empty (e). A mode image of the linear propagation in the toluene waveguide array inside this fiber is superimposed with a scheme of the filling pattern (f). Blue circles indicate liquid-filled holes.

The simplest filling pattern is a single-strand structure. In this case, just one hole of the PCF is left open and this single strand is filled with the liquid. Light from a 250 fs laser source at 1030 nm was coupled into the device and propagation of the fundamental mode was observed.

To tailor the liquid-filled PCF such that propagation takes place in the anomalous-dispersion regime (meaning in this case that the zero-dispersion wavelength is smaller than 1030 nm), we used the highly nonlinear liquid CCl4, which has a nonlinear refractive-index coefficient six times higher than that of fused silica. Output spectra were measured as a function of input intensity (see Fig. 3). For low pump powers, the spectral broadening is mainly caused by self phase modulation, while for higher pump powers, supercontinuum generation due to soliton formation, fission, and Raman processes takes place.

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FIGURE 3. Output spectra of a 26-cm-long selectively filled PCF were measured for different pump powers. A single strand of the fiber is filled with CCl4 (the second-order coefficient n2 = 15 × 10-20 W/m2). The pump source generates pulses with a 250 fs pulse duration at a 1030 nm wavelength. The device is pumped in the anomalous-dispersion regime; as a result, solitons can form at higher pump powers.

Applications of the selectively filled PCF include spatio-temporal nonlinear propagation with specific tailored properties such as nonlinear all-optical switching, as well as the generation of spatio-temporal solitons (“light bullets”).8,9 Highly interesting effects arise due to the time-delayed response of the liquid, which stems from delayed reorientation of the liquid molecules.10–12 Furthermore, purely nonlinear lattices can be created.13 Additionally, the method is suited for selective filling of several different liquids, or for creation of highly birefringent liquid-filled PCFs using (for example) liquid crystals. Another possibility is to selectively infiltrate different gases for higher-harmonic generation. Several approaches are applicable to the field of biosensing.14

REFERENCES

1. F. Benabid et al., Science, 298, 399 (2002).
2. M.A. Schmidt et al., Phys. Rev. B, 77, 033417 (2008).
3. B.T. Kuhlmey et al., J. Lightwave. Technol., 27, 1617 (2009).
4. P.D. Rasmussen et al., Opt. Exp., 16, 5878 (2008).
5. R. Zhang et al., Opt. Exp., 14, 6800 (2006).
6. M. Vieweg et al., Opt. Exp., 18, 25232 (2010).
7. S. Maruo et al., Opt. Lett., 22, 132 (1997).
8. F. Ye et al., Opt. Exp., 17, 11328 (2009).
9. S. Minardi et al., Phys. Rev. Lett., 105, 263901 (2010).
10. R. Raja et al., J. Opt. Soc. Am. B, 27, 1763 (2010).
11. S. Pricking and H. Giessen, Opt. Exp., 19, 2895 (2011).
12. C. Conti et al., Phys. Rev. Lett., 105, 263902 (2010).
13. Y. Kartashov et al., Opt. Lett., 34, 770 (2009).
14. T. Euser et al., Opt. Lett., 34, 3674 (2009).

Marius Vieweg,Timo Gissibl, and Harald Giessen are at the 4th Physics Institute, University of Stuttgart, Pfaffenwaldring 57, 70569 Stuttgart, Germany; e-mail: m.vieweg@physik.uni-stuttgart.de.

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