共查询到17条相似文献,搜索用时 468 毫秒
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非线性Bragg微腔的双稳态研究 总被引:2,自引:0,他引:2
研究了一维Bragg微腔中的光学增强效应,并对F-P腔中Kerr介质的双稳态特性进行了理论分析,并得到相应的数学表达式.研究表明,对聚焦型Kerr介质(χ(3)>0),要产生双稳态特性必须给入射光波预置一定的红移量,若是散焦型介质(χ(3)<0)则要预置一定的蓝移量.红移量(或蓝移量)的临界值与光子晶体的介质折射率、周期数、F-P腔长度、缺陷模的线宽(FWHM)等因素密切相关,它随介质折射率比、周期数、F-P腔长的增大而减小,随缺陷模的线形变窄而降低.要有效地降低非线性介质的双稳态开关阈值,除了尽可能选择较小的合适红移(或蓝移)量外,还要选择|χ(3)|较大的Kerr介质以增强腔内的非线性光学效应. 相似文献
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介质层厚对含负折射率介质Bragg微腔的影响 总被引:1,自引:0,他引:1
研究了介质层厚对含负折射率介质一维光子晶体Bragg微腔的缺陷模和双稳态的影响.在中心频率附近将传输矩阵各矩阵元采用泰勒级数展开并取一级近似,得到了缺陷模频率与介质层厚的关系式及品质因子公式.研究结果表明:一级近似法能很好地解释中心频率附近介质层厚对缺陷模频率的影响.理想Bragg微腔结构的缺陷模品质因子最大;递增正折射率介质层厚和增大缺陷层介质层厚、递减负折射率介质层厚及同时等量递减正和负折射率介质层厚,均可使缺陷模红移,双稳态阈值降低. 相似文献
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《中国光学与应用光学文摘》2006,(4)
O437 2006043105含负折射率介质非线性Bragg腔的双稳态特性=Bistableproperties of nanlinear Bragg cavity containing negative re-fractive index materials[刊,中]/蒋美萍(南京理工大学材料科学与工程系.江苏,南京(210094)) ,陈光…∥光子学报.—2006 ,35(4) .—535-539研究了含负折射率介质一维光子晶体非线性Bragg腔的透射特性、光学增强和双稳态特性、对负折射率介质无色散和有色散非线性Bragg腔及由两种正折射率介质构成的非线性Bragg腔的透射谱、光学增强、缺陷模的线宽、入射光的红移量、双稳态开关阈值进行了比较。含负折射率… 相似文献
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含色散与非线性媒质的光子晶体的简正耦合模 总被引:7,自引:3,他引:4
利用传输矩阵方法及对色散媒质采用洛伦兹振子模型,研究了一维含色散媒质的光子晶体的简正耦合模,并计算了该结构的复有效折射率。在光学双稳态中,与仅含非线性媒质的光子晶体相比,得到了低得多的阈值入射光强。 相似文献
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《中国光学与应用光学文摘》2005,(1)
O437 2005010223 一维非均匀Kerr介质的传输矩阵算法=Transfer matrix algorithm of one-dimensional inhomogeneous Kerr medium [刊,中]/陈历学(哈尔滨工业大学应用物理系.黑龙江,哈尔滨(150001)),丁卫强….∥光子学报.-2004,33 (4).-497-500 研究了一维非均匀Kerr介质的子层逆向递推传输矩阵算法,给出了数值实现方案。此方法可以方便而精确地模拟非均匀Kerr介质的传输行为。应用此算法模拟一维 Kerr缺陷光子晶体的光学双稳开关过程时,得出了和非线性时域有限差分方法相一致的结果。图2参6(于晓光) 相似文献
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Suryanto A. van Groesen E. Hammer M. Hoekstra H.J.W.M. 《Optical and Quantum Electronics》2003,35(4-5):313-332
We present a simple numerical scheme based on the finite element method (FEM) using transparent-influx boundary conditions to study the nonlinear optical response of a finite one-dimensional grating with Kerr medium. Restricting first to the linear case, we improve the standard FEM to get a fourth order accurate scheme maintaining a symmetric-tridiagonal structure of the finite element matrix. For the full nonlinear equation, we implement the improved FEM for the linear part and a standard FEM for the nonlinear part. The resulting nonlinear system of equations is solved using a weighted-averaged fixed-point iterative method combined with a continuation method. To illustrate the method, we study a periodic structure without and with defect and show that the method has no problem with large nonlinear effect. The method is also found to be able to show the optical bistability behavior of the ideal and the defect structure as a function of either the frequency or the intensity of the input light. The bistability of the ideal periodic structure can be obtained by tuning the frequency to a value close to the bottom or top linear band-edge while that of the defect structure can be produced using a frequency near the defect mode or near the bottom of the linear band-edge. The threshold value can be reduced by increasing the number of layer periods. We found that the threshold needed for the defect structure is much lower then that for a strictly periodic structure of the same length. 相似文献
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We present a detailed study of the dispersive medium’s normal coupled modes in a symmetric one-dimensional photonic crystals (1D PCs). The splitting, homogeneous broadening effect, and the detuning effect of the normal coupled modes can be well controlled by adjusting the parameters of the dispersive medium. The bistable behavior of the PCs with Kerr medium is also investigated and it is found that the threshold intensity of nonlinear optical bistability (OB) of 1D PCs with dispersive medium is much lower than that of structure without dispersive medium. The threshold intensity is strikingly sensitive to the coupling strength of the dispersive medium. 相似文献
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Transmission properties of one-dimensional photonic crystal with two nonlinear defects were investigated based on the nonlinear transfer matrix method. From the inspection of the optical bistabilities around different defect modes, it was found that the threshold of bistability for the bonding mode is always lower than that for the anti-bonding mode. When intensity of the incident wave increases bistability could happen at any wavelength larger than the resonance wavelength of the linear anti-bonding mode in the gap. The threshold of bistability increases initially with the wavelength, then decreases sharply in reaching the resonance wavelength of the linear bonding mode. The coupling behavior of the two defects was also discussed, and it was found that the threshold of bistability increases with the distance between the two defects. A flat spectrum similar to that formed in the photonic crystal molecules was obtained under certain incident intensity. 相似文献
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Dong Zhao Zhou-qing Wang Hua Long Kai Wang Bing Wang Pei-xiang Lu 《Optical and Quantum Electronics》2017,49(4):163
We study the optical bistability (OB) in photonic multilayers doped by graphene sheets, stacking two Bragg reflectors with a defect layer between the reflectors. OB stems from the nonlinear effect of graphene, so the local field of defect mode (DM) could enhance the nonlinearity and reduce the thresholds of bistability. The structure achieves the tunability of bistability due to that the DM frequency and transmittance could be modulated by the chemical potential. Bistability thresholds and interval of the two stable states could be remarkably reduced by decreasing the chemical potential. A lager Bragg periodic number could increase the localizing of field, but the graphene loss may decrease the intensity of transmission light. We have concluded an appropriate periodic number to achieve OB. The study suggests that the tunable bistability of the structure could be used for all-optical switches in optical communication systems. 相似文献
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Low-threshold bistable reflection assisted by oscillating wave interaction with Kerr nonlinear medium 下载免费PDF全文
Yingcong Zhang 《中国物理 B》2021,30(8):84203-084203
Owing to the enormously enhanced oscillating wave, a minute variation of the incident light intensity will give rise to a change in the dielectric constant of the Kerr nonlinear medium and lead to a bistable reflection with an ultra-low threshold intensity, which is closely related to the angle of incidence and the thickness of the Kerr nonlinear medium. The criterion for the existence of optical bistability is derived. Our bistability scheme is simple and not limited to the TM-polarization. 相似文献
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The transmission spectra of two-period metal-dielectric structure are studied through the transfer matrix method. When the dielectric is nonlinear material, an optical bistability has been found. The upper threshold value is insensitive to incident frequency, while the lower threshold value increases with the incident frequency decreasing. The effect of loss from the metal layers on the optical bistability is also considered. 相似文献
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基于传递矩阵方法和光局域化原理, 本文研究了一维反铁磁光子晶体共振频率附近光学双稳态效应随电磁波入射角、 外磁场强度及电介质层数的变化.研究发现, 当外磁场为1.0 kG(1 G=10-4 T)、电磁波小角度入射时, 反铁磁材料高低共振频率附近均可探测到光学双稳态效应; 当电磁波大角度入射时, 仅在高共振频率附近探测到光学双稳态效应. 然而, 当外磁场强度增加到2.0 kG时, 由于反铁磁材料的高低共振频率向两侧移动, 低共振频率附近缺失的光学双稳态频率窗口又被有效激发. 此外, 电磁波小角度入射时, 电介质层数在低共振频率附近对双稳态效应影响较明显. 相似文献