Table 1 Simulation parameters Title Author1, Author2 School of Physics and The MOE Key Laboratory of Weak Light Nonlinear Photonics, Nankai University, Tianjin 300457, China bb@email.cn, zg@nankai.edu.cn 1. INTRODUCTION Table 1 Simulation parameters λ (nm) ω0 (mm) tp (ns) n0 n2 (m2/W) α (cm-1) τD L 600 0.5 1.0 1.65 5e-8 14 0.1 ~1.0 The easiest way to follow the format is to simply substitute your text with the corresponding sections of this template. This template was made using Microsoft Wo Fig. 3 Time delay and amplitude of the signal pulse versus the position of F-P cavity. The simulation parameters, except for z, are the same as those of fig. 2. The time delay and the amplitude of the signal pulse can be tuned by scanning the position of the cavity, thereby the light intensity in the cavity, with only nonlinear medium (red markers, n2=5e-8 m2/W), but not linear medium (blue markers, n2=0) filled. In addition, we can not observe obvious time delay when the relatively weak laser pulse pass through a free nonlinear medium, either. These phenomena can be ascribe to the combination of the photonic structure resonance and the transverse phase modulation effect. 2. XXXX Fig. 1 Experimental setup. laser lens aperture detector Nonlinear F-P cavity beam splitter mirror The easiest way to follow the format is to simply substitute your text with the corresponding sections of this template. This template was made using Microsoft Word.[5] Fig. 4 Time delay and signal intensity versus the length of the nonlinear (red markers) and linear (blue markers) F-P cavity. The easiest way to follow the format is to simply substitute your text with the corresponding sections of this template. This template was made using Microsoft Word.[5] The easiest way to follow the format is to simply substitute your text with the corresponding sections of this template. This template was made using Microsoft Word. 4. CONCLUSIONS Assumptions: The easiest way to follow the format is to simply substitute your text with the corresponding sections of this template. This template was made using Microsoft Word. The easiest way to follow the format is to simply substitute your text with the corresponding sections of this template. This template was made using Microsoft Word. 3. XXXX 5. REFERENCE [1] T. F. Krauss, “Why do we need slow light?” Nat. Photon. 2(8), 448 (2008). [2] “Slow light now and then,” Nat. Photon. 2(8), 454 (2008). [3] I.Guedes, L. Misoguti, and S. Zilio, “Precise control of superluminal and slow light propagation by transverse phase modulation,” Opt. Express 14(13), 6201(2006). [4] L. Xu, G. Zhang, N. Xu, F. Bo, F. Gao, W. Fan, J. Xu, K. Lor, and K. Chiang, “Active chromatic control on the group velocity of light at arbitrary wavelength in benzocyclobutene polymer,” Opt. Express 17(20),18292 (2009). [5] T. Bischofberger and Y. R. Shen, "Theoretical and experimental study of the dynamic behavior of a nonlinear Fabry-Perot interferrometer." Phys. Rev. A 19(3), 1169 (1979). [6] M. Sheik-Bahae, A. Said, T. Wei, D. Hagan, and E. Van Stryland, “Sensitive measurement of optical nonlinearities using a single beam,” IEEE J. Quantum Electron. 26(4), 760 (1990). Fig. 2 reference and signal pulses. Iin the maximum light intensity on axis at focus point is set to be 20 W/m2. The position of the cavity z=0, in other words, the cavity was put at the focal point of the laser beam. The amplitude transmittance T of the cavity mirror is 0.1. Other parameters are listed in table 1. It is clearly seen that the signal pulse (red curve) was delayed. The 2nd Materials Science Student Innovation Forum November , 2018, National Institute for Advanced Materials