共查询到18条相似文献,搜索用时 171 毫秒
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为了研究石墨烯器件在中红外波段的光限幅机理,采用化学气相沉积法制备出层数可控的石墨烯薄膜CaF2镜片,并基于MgO∶PPLN周期极化晶体搭建了全固态中红外光学参量振荡器,利用3 m~5 m波长可调谐的闲频光开展了石墨烯薄膜散射实验,测量了石墨烯薄膜的散射信号与入射光强度变化的归一化曲线。当闲频光能量超过1 J/cm2时,石墨烯被迅速汽化,电离形成的微小等离子体和石墨烯微片对入射闲频光产生多重非线性散射,散射能量信号呈现出快速非线性增长趋势,并且散射能量信号值的增长率与闲频光的入射波长成反比,与石墨烯的层数成正比关系,从而验证了石墨烯对中红外波段激光较强的非线性散射使其具有光限幅效应。 相似文献
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以咔唑为电子供体,苯并噻唑为电子受体,合成了两种新型咔唑-苯并噻唑衍生物3-(2-苯并噻唑-2-基乙烯基)-N-乙基咔唑和3,6-二(2-苯并噻唑-2-基乙烯基)-N-乙基咔唑,通过核磁共振和分光光度计对其结构进行表征.利用刮刀法制备质量分数为4%的衍生物/聚酰亚胺的复合薄膜.采用透射光谱法和单光束Z-扫描技术分别测试了衍生物的线性和三阶非线性光学特性.Z扫描实验结果表明3-(2-苯并噻唑-2-基乙烯基)-N-乙基咔唑薄膜的非线性吸收系数和非线性折射系数分别为β1=-2.118 9×10-10 cm/W、r1=2.285 2×10-14 cm2/W,具有反饱和吸收特性和自聚焦效应;同时3,6-二(2-苯并噻唑-2-基乙烯基)-N-乙基咔唑薄膜的非线性吸收系数与非线性折射系数分别为β2=-1.275 6×10-9 cm/W、r2=-7.039 9×10-14 cm2/W,具有反饱和吸收特性和自散焦效应. 相似文献
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采用紧束缚模型分别描述单层、双层石墨烯的能带结构, 利用光子-电子相互作用的二阶微扰理论分别计算单光子和双光子吸收系数.计算结果表明: 单层石墨烯单光子吸收系数为常数, 约为6.8×107 m-1, 即单层石墨烯对入射光的吸收率约为2.3%; 双层石墨烯的单光子吸收比单层石墨烯的单光子吸收强, 且随入射光波长呈分段性变化.单层石墨烯的双光子吸收系数与波长λ4成正比; 双层石墨烯双光子吸收系数在红外波段(~ 3100 nm处)有一个很强的共振吸收峰. 研究结果可为石墨烯材料在光电子器件的研究和制作方面提供指导.
关键词:
石墨烯
光学吸收
紧束缚模型 相似文献
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《光子学报》2015,(1)
以咔唑为电子供体,苯并噻唑为电子受体,合成了两种新型咔唑-苯并噻唑衍生物3-(2-苯并噻唑-2-基乙烯基)-N-乙基咔唑和3,6-二(2-苯并噻唑-2-基乙烯基)-N-乙基咔唑,通过核磁共振和分光光度计对其结构进行表征.利用刮刀法制备质量分数为4%的衍生物/聚酰亚胺的复合薄膜.采用透射光谱法和单光束Z-扫描技术分别测试了衍生物的线性和三阶非线性光学特性.Z扫描实验结果表明3-(2-苯并噻唑-2-基乙烯基)-N-乙基咔唑薄膜的非线性吸收系数和非线性折射系数分别为β1=-2.118 9×10-10 cm/W、r1=2.285 2×10-14 cm2/W,具有反饱和吸收特性和自聚焦效应;同时3,6-二(2-苯并噻唑-2-基乙烯基)-N-乙基咔唑薄膜的非线性吸收系数与非线性折射系数分别为β2=-1.275 6×10-9 cm/W、r2=-7.039 9×10-14 cm2/W,具有反饱和吸收特性和自散焦效应. 相似文献
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采用微球自组装及倾斜真空热蒸镀技术制作了三维手性壳状银纳米结构,采用Z扫描技术研究了该样品在532nm波长、4ns脉宽的Nd:YAG激光入射下的非线性饱和吸收特性。研究结果表明,当入射激光强度达到2.5×10~9 W/cm~2时,其非线性吸收系数可达-1.45×10~(-5) cm/W,该结果比文献报道的悬浮液中的胶体银纳米颗粒的非线性吸收系数(-1.5×10~(-9) cm/W)大四个数量级。实验还发现,该样品的非线性吸收系数随着入射激光的偏振方向改变而出现明显的变化。文中对其非线性吸收的增强机理及偏振依赖性进行了分析讨论。 相似文献
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利用氧化钕和盐酸为原料制得Nd(phen)2Cl3(三氯二邻菲罗啉合钕),测得其光谱特性并以稀土氧化钕、苯甲酸和邻菲罗啉为原料制得绿色液体激光介质钕离子的配合物——NdB3phen(三苯甲酸—邻菲罗啉合钕).利用飞秒激光器,采用单光束Z-扫描法研究了NdB3phen的三阶非线性光学特性.结果表明:当入射飞秒激光脉冲波长为400 nm,峰值功率密度为2.94×1014 W/m2,脉宽为117 fs时,测得样品NdB3phen的非线性折射率为-2.84×10-18 cm2/W|NdB3phen在开孔条件下呈现反饱和吸收现象,测出双光子吸收系数的值为9.11×10-12 m/W.实验结果表明,NdB3phen的双光子吸收系数和非线性折射率随着光强的增强而增大. 相似文献
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应用Z扫描技术,在波长为532nm、脉宽为8ns条件下,对一种新型亚酞菁配合物三-α-(2,4-二甲基-3-戊氧基)溴硼亚酞菁的三阶非线性光学特性进行了研究,结果发现,该新化合物有较强的反饱和吸收(β=3.7×10-10 m/W)效应和非线性自聚焦折射效应(n2=7.2×10-11esu),其三阶非线性极化率χ(3)=1.1×10-11esu.分析了溴硼亚酞菁配合物特殊的锥形分子结构和重原子溴的轴向配位等因素对其三阶非线性光学性质的重要影响.
关键词:
亚酞菁
Z扫描
三阶光学非线性 相似文献
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N. Venkatram D. Narayana Rao L. Giribabu S. Venugopal Rao 《Applied physics. B, Lasers and optics》2008,91(1):149-156
We report our results on the nonlinear optical and optical limiting properties of two alkoxy phthalocyanines namely 2,3,9,10,16,17,23,24-octakis-(heptyloxy)
phthalocyanine and 2,3,9,10,16,17,23,24-octakis-(heptyloxy) phthalocyanine zinc(II) studied at a wavelength of 532 nm using
6 ns pulses. Using the standard Z-scan technique we observed that both the phthalocyanines exhibited negative nonlinearity
as revealed by the signature of closed aperture data. The magnitude of the nonlinear refractive index n2 evaluated from the closed aperture data was ∼ 1.61×10-11 cm2/W for the free-base phthalocyanine and ∼ 1.56×10-11 cm2/W for the metallic phthalocyanine. Open aperture Z-scan data indicates strong nonlinear absorption in both the phthalocyanines
with measured nonlinear coefficients of ∼ 1650 cm/GW and ∼ 1850 cm/GW respectively. We also report optical limiting properties
of these phthalocyanines with limiting thresholds (I1/2) of ∼ 0.5 J/cm2. Our studies suggest that these phthalocyanines are one of the best molecules for nonlinear optical applications studied
recently.
PACS 42.65.-k; 42.70.Jk, 42.65.Jx 相似文献
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Under strong laser illumination, few-layer graphene exhibits both a transmittance increase due to saturable absorption and a nonlinear phase shift. Here, we unambiguously distinguish these two nonlinear optical effects and identify both real and imaginary parts of the complex nonlinear refractive index of graphene. We show that graphene possesses a giant nonlinear refractive index n(2)?10(-7) cm(2) W(-1), almost 9 orders of magnitude larger than bulk dielectrics. We find that the nonlinear refractive index decreases with increasing excitation flux but slower than the absorption. This suggests that graphene may be a very promising nonlinear medium, paving the way for graphene-based nonlinear photonics. 相似文献
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偶氮分散红聚合物薄膜的Z扫描研究 总被引:3,自引:0,他引:3
采用单光束Z扫描技术对新型光学存储材料偶氮分散红聚合物的薄膜样品进行了测量。实验结果表明 ,该样品的非线性折射率为负值。为消除非线性吸收的影响 ,将实验所得有孔Z扫描曲线除以开孔Z扫描曲线进行了处理。从Z扫描曲线的实验数据处理得到这种新型偶氮分散红聚合物薄膜材料的非线性折射率为 :- 5 .5× 10 -6cm2 /W ,其值比常见无机非线性光学材料大 8~ 9个数量级 ,是一种很有应用前景的新型光学存储材料。最后 ,对这种偶氮聚合物薄膜具有大的非线性折射率的物理机制进行了分析。初步认为 :在线偏振光照射下 ,偶氮分子变为各向异性。这些类似液晶相的分子很好地关联在一起 ,分子的取向对外界扰动的响应是一种集体的效果 ,所以他们具有很大的非线性响应。 相似文献
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利用Heck反应合成了一种新型的共轭长链的芴类衍生物,研究了它的线性和非线性光学特性。测试了它在石油醚、二氯甲烷、乙酸乙酯和二甲基甲酰胺(DMF)四种不同极性溶剂中的紫外吸收和荧光光谱特性,结果表明溶剂极性对新物质紫外吸收光谱和荧光光谱有一定程度的影响,随着溶剂极性的增加,吸收光谱和荧光光谱均红移。在激发波长为1064nm皮秒激光器作用下,测试了新物质的光学非线性——光限幅效应,结果显示其透射率随入射光强的变化呈现非线性降低,限幅效应明显。根据分析得出,此光限幅效应是由三光子吸收引起。通过数据拟合,得出了新物质的三光子吸收系数γ为5.4×10-21 cm3/W2及相应的三光子吸收截面σ′3为7.3×10-77 cm6.s2。 相似文献
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H. Manaa A. Tuhl J. Samuel A. AL-Mulla N.A. AL-Awadi S. Makhseed 《Optics Communications》2011,284(1):450-454
Photophysical and nonlinear optical properties of zinc phthalocyanines (ZnPc) bearing peripheral phenoxy substituents containing different functionalized groups were studied. Fluorescence spectra corresponding to the optical transition S1 → S0 are found to be appeared at 684 or 686.4 nm. Z-scan technique reveals large nonlinearities, where the absorptive and refractive effects are separately evaluated. Saturation absorption of ZnPc-1 was observed at 632.8 nm, with a very large nonlinear absorption coefficient β = −1.36 × 10−2 cm/W. However a strong nonlinear refractive effect was found in all ZnPcs (1-4). Transmitted versus incident irradiance measurements carried out on ZnPc-1 and ZnPc-2, showed a very clear optical limiting behavior with irradiance thresholds around be 44 W/cm2 and 90 W/cm2 respectively. 相似文献
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The nonlinear optical properties of thin films of LaEr(MoO4)3 were studied using a ∼30 ps Nd:YAG laser at 532 nm with a repetition rate of 250 Hz. Closed aperture Z-scan measurement revealed
a negative nonlinearity in the LaEr(MoO4)3. The nonlinear refractive index γ=1.38×10-10 cm2/W and nonlinear absorption coefficient β=16.8×10-6 cm/W were calculated from the Z-scan data. The fluorescent upconversion spectra were recorded with 980 nm excitation. An
optical switching mechanism based on nonlinear absorption is also presented experimentally.
PACS 81.15.Fg; 77.84.Bw; 33.50.Dq; 42.70.Mp 相似文献