1 March 2011 All-optical diode with photonic multilayers based on asymmetric light localization
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Abstract
An all-optical diode (AOD) with structure (AB)m(BA)n(BBAA)k is proposed based on asymmetric light localization, and its optical bistability are numerically investigated by the nonlinear transfer matrix method. Research results show that the behavior of the AOD strongly depends on the period number m, n, and k, the transmission direction of the AOD is related to the values of m and n, while k affects the transmission contrast of the AOD. It is a significant reference for the design of all-optical signal processing devices.
Jin, Zhou, Yang, Xue, and He: All-optical diode with photonic multilayers based on asymmetric light localization

1.

Introduction

An all-optical diode (AOD) is a spatially nonreciprocal device and plays an important role in all optical signal processing. In recent years, various structures of AOD have been designed with different materials, such as metamaterials,1, 2, 3 and the efficiency of AOD is characterized by the transmission contrast C = (TLeftTRight)/(TLeft + TRight).4 To obtain a high transmission contrast in the structure of photonic multilayer, one way is to use the nonreciprocal reflection caused by nonlinear absorption of metal,5, 6 another way is to use the spatial asymmetry of the structure (e.g., Thue–Morse structure) with Kerr nonlinear dielectric materials.7, 8 However, the transmission of the AOD in the first way is relatively low because of the absorption of metal, and although high transmission can be reached in the spatial Thue–Morse structure with the second way, the structure is comparatively complicated when the generation number of the Thue–Morse structure becomes large, which limits its application in practical.

In this work, an AOD is designed with a simple photonic multilayers (AB)m(BA)n(BBAA)k. In comparison to the mirror-symmetric structure (AB)m(BA)m, which cannot realize nonreciprocal transmission, the spatially asymmetric structure (AB)m(BA)n(BBAA)k (with m = n) possesses not only the high transmission but also the nonreciprocal transmission due to asymmetric light localization. Furthermore, when different materials are assigned to represent A and B [i.e., the structures of the form (AB)m(BA)n(BBAA)k and (BA)m(AB)n(AABB)k whose linear properties have been studied in Ref. 9], the nonlinear performances of both forms are examined and a better assignment is suggested for designing the AOD.

2.

Simulation and Discussion

The linear and nonlinear material parameters of the photonic multilayer structure (AB)m(BA)n(BBAA)k are selected as those in Ref. 7, where A and B denote polydiacetylene 9-BCMU organic material and TiO2 material with linear refractive indices nA = 1.55, nB = 2.3, thickness dA = 92 nm, dB = 62 nm, nonlinear Kerr refractive indices n2(9-BCMU) ≈ 2.5 × 10−11 cm2/W, and n2(TiO2) ≈ 10−14 cm2/W, respectively. Thus, the resonant wavelength λres of the structure satisfies the relationship nAdA = nBdB = λres/4.

The nonlinear transmission of the structure is calculated by using the nonlinear transfer matrix method.10 As an example, the nonlinear transmission spectra of the structure (AB)6(BA)6(BBAA)6 for left and right incidence are shown in Fig. 1. In region II (between two straight dashed-dotted lines) of Fig. 1, the transmission of the left incident light locates at the upper branches because its intensity is beyond bistability threshold, while the transmission of the right incident light stays at the lower branches for its intensity is below bistablitiy threshold. Thus, an AOD whose direction is left is realized by using the nonreciprocal transmitted character in region II. Then to explore the mechanism of the AOD action, Fig. 1 shows the different field distributions for both directions. Thus, it is because the asymmetric light localization caused by combing with part (BBAA)6 that the bistability thresholds for both directions of photonic multilayer (AB)6(BA)6(BBAA)6 are differentiated.

Fig. 1

(a) Nonreciprocal transmission behavior depending on the in-put intensity Iin at incident wavelength λ = 576 nm under normal inci-dence for left and right directions. An AOD is realized with Tleft = 0.958,Tright = 0.230, Iin = 0.448 MW/cm2. (b) The electric field intensity distributions for both incident directions at wavelength λ = 576nm.

030503_1_1.jpg

To investigate the influence of the material assignment to the action of the AOD, the properties of the photonic multilayers (BA)m(AB)n(AABB)k and (AB)m(BA)n(BBAA)k are examined. As shown in Fig. 2 with an example m = n = k = 6, though both structures can realize perfect transmission, the bandwidth of the resonant mode of the former structure is narrower than that of the latter structure. Then with our calculation, the upper branches of optical bistability of the former structure falls faster than that of the latter structure. As demonstrated by comparing Figs. 2 and 1, with a rapid falling of the upper branches, the transmission and transmission contrast of (BA)6(AB)6(AABB)6 is lower than that of (AB)6(BA)6(BBAA)6 at wavelength λ = 576 nm. Moreover, as can be seen from Fig. 2, for the structure (BA)6(AB)6(AABB)6, the shorter the incident light wavelength is, the lower the difference is between the forward and backward bistability thresholds. Hence, the assignment with the form (AB)m(BA)n(BBAA)k is better to design the AOD with high transmission and high-transmission contrast.

Fig. 2

(a) Linear transmission of structures (AB)6(BA)6(BBAA)6 (solid line) and (BA)6(AB)6(AABB)6 (dashed line) and (b) nonlinear transmission of structure (BA)6(AB)6(AABB)6 for two incident directions at wavelength λ1 = 576 nm and λ2 = 572 nm corresponding the arrows 1 and 2 in (a), respectively.

030503_1_2.jpg

In the following, the influences of the period numbers m, n, and k to the behavior of the forward/backward bistability of the structure (AB)m(BA)n(BBAA)k are discussed. Figure 3 shows the nonlinear transmission spectra at wavelength λ = 576 nm under normal incidence. Several interesting conclusions are obtained. First, as shown in Figs. 3 and 3, the bistability threshold enhances for left incidence but reduces for right incidence as m increases. Therefore, the direction of the AOD strongly depends on period number m. For example, the nonreciprocal transmission of AOD is left when m = 6, whereas it is right when m > 6. In fact, the direction of the AOD also strongly depends on period number n, whereas the action of n nearly equals that of m (for simplicity, the case of n is not shown here). Second, as seen from Figs. 3 and 3, a trade-off is found between the nonreciprocity and the maximum transmission. As k increases, the maximum transmission increases while the nonreciprocity decreases. For example, for m = 7 and n = 6, when k = 6, Tmax = 0.897, the direction of the AOD is right, but when k = 8, Tmax = 0.947, the nonreciprocal transmission disappears. Third, when m = n, as k increases, besides the reduction of the bistability threshold of the AOD, another trade-off is found between the transmission and the transmission contrast. As shown in Figs. 3 and 3, the transmission contrast increases while the transmission decreases. For example, for m = 6, when k = 6, Tleft = 0.958, Tright = 0.230, and C = 0.61; but when k = 8, Tleft = 0.893, Tright = 0.185, and C = 0.65. The dependence of the optical bistability on the period numbers is useful to adjust the functions of AOD.

Fig. 3

Influences of the period numbers m, n, and k to the behavior of bistability for two directions at wavelength λ = 576 nm. (a,c,e) The light incidents from left and (b,d,f) from the right.

030503_1_3.jpg

Furthermore, it is known that the nonreciprocal transmission behavior of the structure (AB)m(BA)n(BBAA)k also depends on the wavelength of incident light due to the dynamic shift mechanism of the defect mode in nonlinear medium. Figures 4 and 4 show the effects of the incident wavelength to the behavior of forward/backward bistability, respectively. It is obtained that the bistability thresholds for both directions enhance as the wavelength of light increases.

Fig. 4

Influences of the incident wavelength to the behavior of bistability for two directions. (a) The light incidents from left and (b) from the right.

030503_1_4.jpg

3.

Conclusions

In summary, a nonlinear AOD with the structure (AB)m(BA)n(BBAA)k is realized based on asymmetric light localization. Transmission of 98.5% is reached at the input intensity 0.448 MW/cm2 with the photonic multilayer structure, which is nearly the same as that of the Thue–Morse structure, but the thickness of our structure (7.392 μm) is much thinner than that of the Thue–Morse structure (12.096 μm). Moreover, the performance of the AOD can be tuned by varying the period numbers in our structure. Therefore, the photonic multilayer structure provides significant reference for the design of all-optical signal processing devices.

Acknowledgments

This work was supported by the National Natural Science Foundation of China (Grant Nos. 60977048 and 61078046), the Natural Science Foundation of Ningbo (Grant No. 2008A610001), the International Collaboration Project of Ningbo (Grant No. 2010D10018), and the K. C. Wong Magna Fund in Ningbo University, China.

References

1.  M. W. Feise, I. V. Shadrivov, and Y. S. Kivshar, “Bistable diode action in left-handed periodic structures,” Phys. Rev. E 71(3), 037602 (2005). 10.1103/PhysRevE.71.037602 Google Scholar

2.  R. Philip, M. Anija, C. S. Yelleswarapu, and D. V. G. L. N. Rao, “Passive all-optical diode using asymmetric nonlinear absorption,” Appl. Phys. Lett. 91(14), 141118 (2007). 10.1063/1.2794015 Google Scholar

3.  A. Alberucci and G. Assanto, “All-optical isolation by directional coupling,” Opt. Lett. 33(15), 1641–1643 (2008). 10.1364/OL.33.001641 Google Scholar

4.  K. Gallo, G. Assanto, K. R. Parameswaran, and M. M. Fejer, “All-optical diode in a periodically poled lithium niobate waveguide,” Appl. Phys. Lett. 79(3), 314–316 (2001). 10.1063/1.1386407 Google Scholar

5.  G.-q. Du, H.-t. Jiang, Z.-s. Wang, and H. Chen, “Optical nonlinearity enhancement in heterostructures with thick metallic film and truncated photonic crystals,” Opt. Lett. 34(5), 578–580 (March 2009). 10.1364/OL.34.000578 Google Scholar

6.  C. Xue, H. Jiang, and H. Chen, “Highly efficient all-optical diode action based on light-tunneling heterostructures,” Opt. Express 18(7), 7479–7487 (March 2010). 10.1364/OE.18.007479 Google Scholar

7.  F. Biancalana, “All-optical diode action with quasiperiodic photonic crystals,” J. Appl. Phys. 104(9), 093113 (November 2008). 10.1063/1.3010299 Google Scholar

8.  V. Grigoriev and F. Biancalana, “Bistability, multistability and non-reciprocal light propagation in Thue-Morse multilayered structures,” New J. Phys. 12(5), 053041 (May 2010). 10.1088/1367-2630/12/5/053041 Google Scholar

9.  S. V. Zhukovsky, “Perfect transmission and highly asymmetric light localization in photonic multilayers,” Phys. Rev. A 81(5), 053808 (May 2001). 10.1103/PhysRevA.81.053808 Google Scholar

10.  P. Yeh, Optical Waves in Layered Media, Wiley, Hoboken, NJ (1988). Google Scholar

Li Jin, Jun Zhou, Mingyang Yang, Chunhua Xue, Miao He, "All-optical diode with photonic multilayers based on asymmetric light localization," Optical Engineering 50(3), 030503 (1 March 2011). https://doi.org/10.1117/1.3558733
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