共查询到20条相似文献,搜索用时 156 毫秒
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单个波长到多个波长的变换实验 总被引:3,自引:1,他引:2
报道一种波长变换的新方法.采用此方法不需要任何泵浦光便能够直接将信号光变换成在特定谱宽内的任意多个任意波长的变换光,这对于将来的波分复用光网络提供了较大的方便.此波长变换的原理是利用色散位移光纤的非线性效应产生超连续光谱(SC)信号,由于这种SC信号携带有变换光信号,对这种连续谱进行滤波便能够得到所需要的任意频率的变换信号.此变换方式具有变换频带宽,偏振不敏感的优点。 相似文献
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针对偏振复用相位调制信号的全光波长变换特性问题,基于半导体光放大器中四波混频效应,建立了对偏振复用正交相移键控信号的全光波长变换理论模型.根据理论分析,建立了仿真系统,仿真结果表明:泵浦光与信号光之间的频率间隔、偏振复用信号中的一个信号与一号泵浦光的偏振夹角对系统转换效率和信号质量有影响;波长转换过程中交叉相位调制产生的相位噪音会对信号质量有影响,且当泵浦光功率较大、泵浦光功率远大于信号光功率时,交叉相位调制效应的影响较小,仿真结果与理论分析一致.本文研究方法和相关结论对其它偏振复用信号基于半导体光放大器四波混频效应的波长变换研究有一定的参考价值. 相似文献
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《光学学报》2010,(11)
提出了一种基于低速信号注入法布里-珀罗型激光二极管(FP-LD)的无本振全光混频技术,利用FP-LD的一个纵模和外部注入信号光的四波混频作用生成的边带锁定纵模产生光载射频信号。通过改变FP-LD的注入光信号强度和偏振态实现副载波频率可变,并根据FP-LD注入锁定特性分析实验结果得到的不同边模抑制比。实验中采用2.7,2.5,1.25 Gb/s非归零(NRZ)码注入FP-LD实现副载波频率分别为16.2,10.0,18.2和20.0 GHz的全光混频,测量16.2 GHz的副载波得到了10 kHz偏移处单边带相位噪声为-81.2,-87.7 dBc/Hz。 相似文献
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研究了基于半导体光放大器平行双抽运对光正交频分复用信号进行全光波长变换的系统.信号光源经2Gb/s电信号直接调制后再和双抽运光耦合,经半导体光放大器后,由于四波混频效应而产生新的波长的信号光.实验结果显示,经半导体光放大器四波混频效应后,产生新的波长的信号光将携带OFDM信号且偏振不敏感,转换效率与双抽运光之间的波长间隔,抽运与信号光波长间距,信号光与泵浦光之间的偏振夹角等有关.同时也测量了转换的OFDM信号的功率-误码曲线和接收星座图. 相似文献
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基于半导体光放大器的交叉增益调制效应实现2.5Gb/s归零码的全光波长变换 总被引:2,自引:0,他引:2
采用半导体光放大器的交叉增益调制进杆了2.SGb/s的归零码光脉冲的波长变换。向下波长变换间距大于20nm,向上波长变换间距大于10nm.对变换信号测量了接收机入纤功率和误码率的关系。对实验结果进行了分析,实验表明采用半导体光放大器的交叉增益调制效应对归者吗进行波长变换时存在着一些问题。 相似文献
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基于周期极化铌酸锂波导,提出了一种采用和频产生与差频产生级联的全光单光子波长变换方案.在海森堡绘景下,通过非线性变换过程的哈密顿量求解了目标单光子信号的湮灭算子,进而根据变换前后的光子数算符之比得到了单光子波长变换的效率.分析了和频产生过程以及差频产生过程中单光子的转换效率与泵浦功率之间的关系,证明了存在最佳泵浦功率使得量子态能够完全转移.数值分析结果表明,当上变换(和频产生)泵浦光功率为65 mW、下变换(差频产生)泵浦光功率为150 mW时,由1550 nm到1530 nm的单光子波长变换可达到61%的转换效率.给出了级联单光子波长变换的实验装置,包括周期极化铌酸锂波导、泵浦激光、准单光子信号源、滤波等光学元器件、单光子探测器和同步线路. 相似文献
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A. H. Taub 《General Relativity and Gravitation》1979,10(12):1009-1009
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Ugeda MM Fernández-Torre D Brihuega I Pou P Martínez-Galera AJ Pérez R Gómez-Rodríguez JM 《Physical review letters》2011,107(11):116803
Understanding the coupling of graphene with its local environment is critical to be able to integrate it in tomorrow's electronic devices. Here we show how the presence of a metallic substrate affects the properties of an atomically tailored graphene layer. We have deliberately introduced single carbon vacancies on a graphene monolayer grown on a Pt(111) surface and investigated its impact in the electronic, structural, and magnetic properties of the graphene layer. Our low temperature scanning tunneling microscopy studies, complemented by density functional theory, show the existence of a broad electronic resonance above the Fermi energy associated with the vacancies. Vacancy sites become reactive leading to an increase of the coupling between the graphene layer and the metal substrate at these points; this gives rise to a rapid decay of the localized state and the quenching of the magnetic moment associated with carbon vacancies in freestanding graphene layers. 相似文献
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We study the relation between the centro-affine geometry of star-shaped planar curves and the projective geometry of parametrized maps into RP1. We show that projectivization induces a map between differential invariants and a bi-Poisson map between Hamiltonian structures. We also show that a Hamiltonian evolution equation for closed star-shaped planar curves, discovered by Pinkall, has the Schwarzian KdV equation as its projectivization. (For both flows, the curvature evolves by the KdV equation.) Using algebro-geometric methods and the relation of group-based moving frames to AKNS-type representations, we construct examples of closed solutions of Pinkall’s flow associated with periodic finite-gap KdV potentials. 相似文献
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In this note we use some of the results of [3] to derive a general duality theorem for the cohomologies of foliated structures on a manifold. The result is applied to the special case of a symplectic manifold M on which the foliation is given by a complex polarization F in the sense of geometric quantization. We obtain, for example, a rigorous proof of the fact that for a smooth function ƒ on M whose Hamiltonian vector field leaves F invariant, the spectrum of the corresponding prequantization operator v(ƒ) coincides with the spectrum of its transpose, under the above duality. This latter result was obtained by Simms in [12] under certain hypotheses. Proofs of the validity of those hypotheses are now available in the literature; cf. [3] and [7]. 相似文献
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Valfells A. Verboncoeur J.P. Lau Y.Y. 《IEEE transactions on plasma science. IEEE Nuclear and Plasma Sciences Society》2000,28(3):529-536
Analyzes the effects of space charge shielding on the steady state of a multipactor discharge on a dielectric. Analytic methods are used to obtain an exact function for the potential in the discharge, assuming a Maxwellian distribution of emitted electrons. An equation for the amount of power deposited on the dielectric by the multipactoring electrons, for a given saturation level, is given. A simple method for obtaining the saturation level, for a given material, is obtained 相似文献
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Kopeikin SM 《Physical review letters》2007,98(22):229001; discussion 229002
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基于密度泛函理论的第一性原理计算方法,研究了Pt原子在五边形石墨烯(PG)上的吸附与动力学行为.研究结果表明,单个Pt原子在PG上虽然具有较大的吸附能及较高的扩散势垒,却不能够在衬底形成均匀分散的单原子.这是因为,随Pt原子数增加,Ptn(n=1, 2, 3)在PG上的平均结合能也逐渐增加,更倾向于形成团簇,该发现有效否定了之前的报道称Pt能在PG上形成稳定的单原子催化剂这一结论(Phys. Chem. Chem. Phys. 21, 12201 (2019)).基于此,我们考虑对PG施加双轴应变,随着拉伸应力增加,Pt金属原子间的平均结合能逐渐降低,当拉伸应变施加至12%左右时,单个Pt在衬底上的结合能与Pt2在衬底上的平均结合能相等,从而实现PG上均匀分散的Pt单原子催化剂.该结果对五边形石墨烯基材料应变调控实现单原子催化剂提供理论借鉴. 相似文献