碳排放与资金双重约束下企业存货质押与生产决策

在碳排放许可与交易制度下,研究受资金约束的排放依赖性企业的存货质押与生产决策.以利润函数为目标函数构建决策模型,模型包括销售收入、生产成本、产成品存储费用、缺货成本、贷款利息、排放权市场交易费用和净化成本.通过求解,得出质押量、产量及对应的利润,最后对各参数进行敏感性分析.     

(E)-(5-(4-(二苯基胺)苯乙烯基)二噻吩并[2,3-b∶3′,2′-d]噻吩基)-2-亚甲基丙二腈的聚集态发光现象的研究

本文报道了对一种电子给体-受体化合物(E)-(5-(4-(二苯基胺)苯乙烯基)二噻吩并[2,3-b∶3′,2′-d]噻吩基)-2-亚甲基丙二腈(TPA-DCST)的合成与光谱学行为的研究。化合物TPA-DCST的分子结构中含有强电子给体(三苯胺)与强电子受体(二氰基乙烯)两个部分,并由二噻吩并[2,3-b∶3′,2′-d]噻吩作为共轭桥将电子给体与受体相连接。在合成方面,采用Wittig反应将三苯胺通过双键与二噻吩并[2,3-b∶3′,2′-d]噻吩相连接、醛基化,并与并二腈经Knoevenagel缩合反应合成目标产物。产物通过了核磁氢谱、碳谱、红外以及高分辨率质谱的确认。光谱方面,主要考察了该化合物的吸收与荧光行为。其最大吸收峰位在412nm左右,归属于π-π*跃迁。在非极性溶剂正己烷中表现出来自分子间聚集而形成的聚集态荧光(550nm),并通过了单分子在CTAB胶束([c]=1.02×10-2 mol/L)的发光(460nm)试验得到验证。溶剂效应表明,该化合物没有出现典型的ICT态的发光现象,其原因在于电子给体与受体相连的共轭桥单元,即二噻吩并[2,3-b∶3′,2′-d]噻吩不具有有效的共轭效应。浓度效应与温度效应进一步表明TPA-DCST分子易于产生分子间聚集态的发光。在THF-H_2O二元溶剂体系中呈现典型的聚集诱导(AIE)发光现象,发光峰位为692nm。随着TPA-DCST分子间的聚集程度的增加,聚集态的荧光出现大范围的红移,直至固体发光红移到710nm。TPA-DCST分子的聚集因素可能来自于疏脂作用、偶极-偶极相互作用等。     

我国海运出口贸易碳排放影响因素的对数指数分解研究

对2005-2013年我国的碳排放进行了对数指数分解,得出海运出口贸易规模、能源效率、能源结构、碳排放强度是构成碳排放的四个因素,其中海运出口规模和碳排放强度是碳排放的正向拉动关系,能源结构和能源效率是碳排放的负向抑制关系.运用协整检验证明四个因素与碳排放之间具有长期稳定的关系,运用Granger因果检验证明海运出口贸易规模、能源结构、能源效率是碳排放的Granger原因.在此基础上,提出减少海运业碳排放的政策建议.     

ICP–AES法测定铬镍不锈钢中锰、铬、镍、硅、磷、铜、钼的含量

建立电感耦合等离子体原子发射光谱(ICP–AES)法测定铬镍不锈钢中锰、铬、镍、硅、磷、铜、钼7种元素含量的方法。试样用盐酸与硝酸混合酸溶液溶解,采用溶解国家标准样品的方法制备校准曲线溶液,确定了元素最佳分析谱线。各元素的含量在其测试范围内与原子发射强度呈良好的线性关系,线性相关系数不小于0.999,7种元素的检出限在0.000 3%~0.003 0%之间。该方法应用于铬镍不锈钢标准样品的测定,测定值与认定值相符,测定值的相对标准偏差在0.12%~1.15%之间(n=8)。应用于铬镍不锈钢样品测定时,加标回收率在90%~110%之间。该方法操作简便、迅速,可满足日常铬镍不锈钢中多元素含量的检测需要。     

Precise Control of Metal Oxide Thin Films Deposition in Magnetron Sputtering Plasmas for High Performance Sensing Devices Fabrication

Magnetron sputtering deposition is a widely used technique to deposit thin film precisely at nanoscale level. During the deposition of metal oxide thin films, reactive oxygen gas is introduced into the deposition chamber. Pure metal and metal oxide materials can be used as sputter target, although the simplest way is by using a pure metal target. In such reactive process, the effect of target poisoning significantly influence the deposition process and the growth mechanisms of metal oxide thin films became very complex. In general, external parameters such as discharge power, working pressure, reactive gases ratio and substrate temperature are used to optimize the properties of deposited thin films. Then, ex-situ analyses such as scanning electron microscope and X-ray diffraction analysis are performed to obtain the optimized parameter. Sample depositions and ex-situ analyses consume time to achieve the goal through try and error. In this article, in-situ plasma diagnostics are reviewed focusing on an optical emission spectroscopy to precisely control and investigate the sputter target poisoning effect during the deposition of metal oxide thin films. The emission of atomic lines from several metal and oxygen atoms were used to discuss the deposition mechanisms and their correlation with the deposited thin films was observed. Finally, the deposited metal oxide thin films were proposed and tested for several applications such as gas sensor and frequency selective surface glass.     

Spectroscopic studies of sodium nitrate plasma produced by nanosecond laser ablation

We present the optical emission characteristics of the sodium plasma produced at the surface of sodium nitrate (NaNO₃) also known as Chile saltpeter. We used a Q-switched Nd:YAG (Quantel Brilliant) pulsed laser having a pulse duration of 5?ns and 10?Hz repetition rate which is capable of delivering 400?mJ at 1064?nm and 200?mJ at 532?nm. The target material was placed in front of laser beam in air (atmospheric pressure). The experimentally observed line profiles of neutral sodium have been used to extract the electron temperature using the Boltzmann plot method, whereas the electron number density has been determined from the Stark broadening. The electron temperature is calculated by varying the distance from the target surface along the line of propagation of the plasma plume and also by varying the laser irradiance. Besides, we have studied the variation of number density as a function of laser irradiance as well as its variation with the distance from the target surface. It is observed that electron temperature and electron number density increase as the laser irradiance is increased.     

基于有机半导体激光材料的高灵敏度溶液检测传感器件

采用光抽运有机激光增益材料产生的放大自发辐射(amplified spontaneous emission ASE), 实现了不同浓度液体的实时检测. 以两种聚合物poly(9, 9-dioctylfluorene-co-benzothiadiazole)和poly(3-hexylthiophene)共混的激光增益介质薄膜作为平面光波导, 观察在滴加少量溶液前后以及不同溶液浓度下, 由于光波导的相对折射率变化导致的放大自发辐射阈值及峰位的变化, 实现对溶液检测. 实验结果显示, 在常温常压下对25 wt.% NaCl溶液检测可得与纯水相比, 放大自发辐射光谱红移了4.5 nm, ASE阈值从0.579 μJ/pulse上升到1.447 μJ/pulse, 约2.5倍, 溶液检测灵敏度达到97.8 nm/RIU(refractive index unit), 精度达到141.9 nm/RIU, 充分说明上述方法能实现高灵敏度溶液检测.     

F8BT∶P3HT共混薄膜放大自发辐射的温度效应

研究了温度对聚合物poly(9,9-dioctylfluorene-co-benzothiadiazole)(F8BT)和poly(3-hexylthiophene)(P3HT)共混薄膜的放大自发辐射(ASE)的影响。在80~320 K温度范围测试了不同P3HT质量比的共混聚合物薄膜和纯F8BT薄膜的ASE特性。在室温条件下,共混聚合物的阈值随着P3HT所占比例的增加先降低后升高。当P3HT比例约为20%时,阈值最低约为2.59×10~3W/cm~2。当温度从320 K下降到80 K时,纯F8BT薄膜的ASE阈值光功率由5.36×10~3W/cm~2下降到4.15×10~3W/cm~2,P3HT质量比为20%的共混薄膜的ASE阈值光功率由2.84×10~3W/cm~2下降到2.03×10~3W/cm~2。在一特定泵浦光功率(5.29×10~3W/cm~2)下,当温度由320 K下降至80 K时,ASE强度约提高4倍。随着温度的降低,混合物薄膜的ASE峰位红移,移动达12 nm。     

不同结构六边形斑图演化过程光谱特性

采用发射光谱法,研究了水电极介质阻挡放电中具有相同对称性的3种不同结构的六边形斑图演化过程的光谱特性。实验结果表明,随着外加电压的增加,放电首先形成六边形点阵斑图,然后是空心六边形斑图,最后是蜂窝六边形斑图。利用氩原子696.5 nm(2P_2→1S_5)谱线的展宽、氩原子763.2 nm(2P_6→1S_5)与772.1 nm(2P_2→1S_3)两条谱线强度比法和氮分子第二正带系(C~3Π_u→B~3Π_g)的发射谱线,研究上述3种斑图的电子密度、电子激发温度及分子振动温度。结果发现,随着外加电压的升高,六边形点阵斑图、空心六边形斑图和蜂窝六边形斑图的电子密度逐渐减小,而电子激发温度和分子振动温度逐渐增加。等离子体状态的改变直接影响着斑图的自组织。