Investigation on performance of all optical buffer with large dynamical delay time based on cascaded double loop optical buffers

Optical buffers are critical for optical signal processing in future optical packet-switched networks. In this paper, a theoretical study as well as an experimental demonstration on a new optical buffer with large dynamical delay time is carried out based on cascaded double loop optical buffers (DLOBs). It is found that pulse distortion can be restrained by a negative optical control mode when the optical packet is in the loop. Noise analysis indicates that it is feasible to realise a large variable delay range by cascaded DLOBs. These conclusions are validated by the experiment system with 4-stage cascaded DLOBs. Both the theoretical simulations and the experimental results indicate that a large delay range of 1--9999 times the basic delay unit and a fine granularity of 25 ns can be achieved by the cascaded DLOBs. The performance of the cascaded DLOBs is suitable for the all optical networks.     

Mechanism and enhancement of photoluminescence from silicon nanocrystals implanted in SiO2 matrix

Photoluminescence (PL) spectra of Si nanocrystals (NCs) prepared by 130 keV Si ions implantation onto SiO₂ matrix were investigated as a function of annealing temperature and implanted ion dose. PL spectra consist of two PL peaks, originated from smaller Si NCs due to quantum confinement effect (QCE) and the interface states located at the surface of larger Si NCs. The evolution of number of dangling bonds (DBs) on Si NCs was also investigated. For hydrogen-passivated samples, a monotonic increase in PL peak intensity with the dose of implanted Si ions up to 3× 10¹⁷ ions /cm² is observed. The number of DBs on individual Si NC, the interaction between DBs at the surface of neighbouring Si NCs and their effects on the efficiency of PL are discussed.     

Sr2CoO4-δ薄膜中的自旋玻璃态的磁性质研究

用脉冲激光沉积方法(PLD)在铝酸镧衬底上制备了c取向的高氧空位含量的锶钴氧薄膜.X射线衍射分析表明薄膜单一取向且没有明显杂相.原位的高气压反射式高能电子衍射仪(RHEED)监测显示,薄膜为层状生长.通过对薄膜磁化强度随温度、磁场及时间的变化曲线进行测量,发现零场冷曲线上可能存在两个特征温度:T_f和T_a.T_f为对应玻璃态的冻结温度而T_a对应少量的不缺     

非稳腔主动式直接获取纳秒近似无衍射贝塞尔绿光

通过对基于轴棱锥的贝塞尔谐振腔和贝塞尔-高斯谐振腔的研究,设计了一台腔内倍频Nd:YAG纳秒近似无衍射贝塞尔绿光激光器. 非稳激光器谐振腔由轴棱锥和凸面镜组成. 实验采用单灯脉冲抽运激光增益介质Nd:YAG晶体,倍频晶体选用KTP. 当抽运电压为350 V时,由主动式直接产生纳秒近似零阶贝塞尔绿光,其脉冲宽度为55.1 ns,波长为532 nm,线宽为0.8 nm,近似无衍射零阶贝塞尔绿光的中心光斑直径为192 μm. 利用Fresnel-Kirchhoff 衍射积分和Fox-Li迭代法,通过数值计算得出     

完全非线性孤立波的稳态解

报道了应用边界积分方法模拟完全非线性孤立波的传播,给急剧记解的波形,流束和数值计算结果。结果表明,本模型对计算孤立波的传播是有铲的。当ａ／ｈ〉０．３时,自由液面上的水平流速、底部流速和垂向平均流速之间的差别是明显的。三阶Ｂｏｕｓｓｉｎｅｓｑ方程的孤立波解比低阶方程的孤立波解更接近本文完全非线性的数值解。     

五种海藻对虹鲍的诱食作用

采用自由择食和非自由择食实验的方法,研究５种海藻Ｌｅｓｓｏｎｉａ ｖａｒｉｅｇａｔｑ,Ｄａｒｖｉｌｌａｅａ ａｕｌａｒｃｔｉｎａ,Ｐｏｒｐｈｙｒａ ｃｏｌｕｍｂｉｎａ,Ｍａｃｒｏｃｙｓｔｉｓ ｐｙｒｉｆｅｒａ,Ｅｃｋｌｏｎｉａ ｒａｄｉａｔａ对实验虹鲍Ｈａｌｉｏｔｉｓ ｉｒｉｓ的诱食作用。结果表明,５种海洋藻类的诱食作用呈显著性差异。     

胶州湾中国对虾资源的生态特征

胶州湾是我囻黄海南部对虾的重要产卵场之一,每年4月中国对虾(Penaeus chinensis)亲体陆续进人胶州湾,进行产卵活动。繁殖的幼对虾生长迅速,至8月下旬虾群平均体长可达13cm左右,成为秋汛渔业的重要捕捞对象。近年由于捕捞力量加强等诸多因素,湾内对虾的年渔获量由70年代的2-5t,减至80年代的1-2t。虽然1984年以来有关部门实施对虾增殖放流,对虾资源量有所回升,但是因春季洄游的亲体(雌虾)数量锐减,7-8月间又使用各种网具违捕幼虾,因而极大地损害了幼虾资源。刘瑞玉等(1992)曾调查研究了胶州湾对虾生物资源。本文根据作者1991年以来5月和8月的对虾拖网调査资料,对胶州湾对虾资源的生态分布及其变动原因进行了分析研究,对加强管理和保护幼虾资源,以及提高对虾产量有极其重要的意义。     

中华鳖气单胞菌疖疮病的研究

气单胞菌疖疮病是中华鳖的主要病害之一,其发病对象主要是稚鳖。将病鳖进行细菌分离,获得的菌株经人工感染、毒力测试和细菌学鉴定,确定致病菌为嗜水气单胞菌Ａｅｒｏｍｏｎａｓｈｙｄｒｏｐｈｉｌａ与豚鼠气单胞菌Ａ．ｃａｖｉａｅ。此两种致病菌不仅对健康鳖表现出较强的致病力,出现与自然病鳖相同的症状,且对健康小鼠亦有较强的致死力,半致死量ＬＤ５０分别为４．５×１０６个菌／只和１．５８×１０６个菌／只。此外,测定了病原菌对抗生素的敏感性,为科学防治提供依据。     

利用综合评分方法评估CMIP5模式对北极海冰的模拟能力

北极海冰冰盖自20世纪以来经历了前所未有的缩减,这使得北极海冰异常对大气环流的反馈作用日益显现。尽管目前的气候模式模拟北极海冰均为减少的趋势,但各模式间仍然存在较大的分散性。为了评估模式对于北极海冰变化及其气候效应的模拟能力,我们将海冰线性趋势和年际异常两者结合起来构造了一种合理的衡量指标。我们还强调巴伦支与卡拉海的重要性,因为前人研究证明此区域海冰异常是近年来影响大尺度大气环流变异的关键因子。根据我们设定的标准,CMIP5模式对海冰的模拟可被归为三种类型。这三组多模式集合平均之间存在巨大的差异,验证了这种分组方法的合理性。此外,我们还进一步探讨了造成模式海冰模拟能力差别的潜在物理因子。结果表明模式所采用的臭氧资料集对海冰模拟能力有显著的影响。     

Dissolved inorganic carbon (DIC) and its carbon isotopic composition in sediment pore waters from the Shenhu area,northern South China Sea

The Shenhu area is one of the most favorable places for the occurrence of gas hydrates in the northern continental slope of the South China Sea. Pore water samples were collected in two piston cores (SH-A and SH-B) from this area, and the concentrations of sulfate and dissolved inorganic carbon (DIC) and its carbon isotopic composition were measured. The data revealed large DIC variations and very negative δ ¹³C-DIC values. Two reaction zones, 0–3 mbsf and below 3 mbsf, are identified in the sediment system. At site SH-A, the upper zone (0–3 mbsf) shows relatively constant sulfate and DIC concentrations and δ ¹³C-DIC values, possibly due to bioturbation and fluid advection. The lower zone (below 3 mbsf) displays good linear gradients for sulfate and DIC concentrations, and δ ¹³C-DIC values. At site SH-B, both zones show linear gradients, but the decreasing gradients for δ ¹³C-DIC and SO₄ ²⁻ in the lower zone below 3 mbsf are greater than those from the upper zone, 0–3 mbsf. The calculated sulfate-methane interface (SMI) depths of the two cores are 10.0 m and 11.1 m, respectively. The depth profiles of both DIC and δ ¹³C-DIC showed similar characteristics as those in other gas hydrate locations in the world oceans, such as the Blake Ridge. Overall, our results indicate an anaerobic methane oxidation (AMO) process in the sediments with large methane flux from depth in the studied area, which might be linked to the formation of gas hydrates in this area.