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1.
溶剂效应对聚喹啉铝发光特性的影响   总被引:2,自引:0,他引:2       下载免费PDF全文
研究了非共轭聚喹啉铝(Palq)在氯仿和乙醇不同极性的溶剂下所获得的薄膜的吸收和发光光谱。由于溶剂性的不同,聚喹啉铝链在氯仿和乙醇溶液中表现出不同的聚集状态。当各种溶液分别旋涂成膜时,溶液中的聚喹啉铝的聚集态仍部分地保存下来,导致不同聚喹啉铝薄膜的电子结构状态的差别。结果,聚喹啉铝的薄膜表现出不同的发光特性。实验表明,在制作聚合物器件中,溶剂的选择对共轭聚合物的发光特性有着重要的影响。  相似文献   

2.
应用荧光光谱、紫外光谱对不同结构的含炔基有机硅共轭聚合物的发光性能进行了表征和研究。探讨了聚合物主链上Si原子取代基的结构以及主链中炔基单元结构对其发光性能的影响,研究结果表明,聚合物可在219~260 nm处有紫外吸收,随着Si原子上取代基共轭性能的增强,以及主链中炔基数目的增多、链段共轭程度的增大,最大吸收波长红移。取代基的影响较小,主链共轭结构对吸收光谱的影响明显。不同主链结构的共轭聚合物在320~353 nm处发出一定强度的荧光。结果显示,聚合物主链共轭基团的结构对发射光谱具有明显的影响,随着主链中炔基数目的增多,最大发射波长显著向长波方向移动。由于此类聚合物的特殊结构使得他们具有良好的热学稳定性,因此这类聚合物具有潜在的光学应用价值。  相似文献   

3.
番茄红素的紫外可见光谱和荧光光谱分析   总被引:1,自引:1,他引:0  
研究了番茄红素在不同溶剂中的紫外可见光谱图,对结果进行分析后发现番茄红素在正己烷、石油醚、丙酮、乙酸乙酯具有较低折光率的溶剂中的特征吸收带波长非常接近,但在较高折光率的溶剂苯、二硫化碳中的特征吸收带与以丙酮作为溶剂相比有不同程度的红移。番茄红素溶于丙酮与水的混合溶剂,当丙酮与水的体积比达到3∶2时,吸收光谱在紫外区出现一新的吸收峰,在可见区吸收光谱的精细结构消失。用荧光光度计采集不同溶液的番茄红素的荧光光谱,番茄红素的荧光峰位于580—590nm,在极性溶剂中荧光发射增强。  相似文献   

4.
徐征  章婷 《发光学报》2002,23(2):175-178
研究了3种非共轭PPV聚合物以及3种共轭PPV衍生物的吸收谱和发光光谱的特性。非共轭PPV聚合物上的侧链烷氧基团有着很强的供电子能力,对调节非共轭聚合物能带带隙有重要的影响,且离主链较近的碳原子对能带结构也有一定的影响。但当侧链上的碳原子数量很大,从7个小时一直变化到10小时,共轭PPV衍生物的吸收光谱和发光光谱变化较少,表明对能带结构影响小。  相似文献   

5.
采用红外光谱、热重分析、紫外光谱和荧光光谱对侧链含查尔酮基团的聚(4-甲基丙烯酰氧基-4'-二甲氨基查尔酮)(PMADMAC)和聚(4-丙烯酰氧基查尔酮)(PAC)的光交联特性进行了研究。随着光照时间的增加,PMADMAC和PAC聚合物光致环加成反应迅速进行,波长短的紫外线更易使得聚合物发生[2+2]环加成反应。与溶液状态相比,固体薄膜状态下的光交联反应速率较慢。PMADMAC聚合物更容易发生光致环加成反应,其光交联速率要比PAC聚合物快,环加成反应也更彻底。采用荧光光谱研究了聚合物的发光特性,发现PAC聚合物无荧光,而PMADMAC聚合物具有溶剂极性敏感的荧光特性。在PMADMAC聚合物的稀溶液中,随着365 nm紫外光照时间的增加,荧光强度迅速降低,其荧光特征波长在紫外光照射后发生蓝移。 PMADMAC和PAC聚合物的热稳定性较好,光交联后形成热不稳定的环丁烷结构,其热稳定性有所降低。  相似文献   

6.
纳米MEH-PPV阵列的光致发光   总被引:1,自引:1,他引:0  
以多孔氧化铝为模板,将可溶性发光聚合物聚(2-甲氧基-5-(2’-乙基己氧基)-1,4-对苯乙炔)(MEH-PPV)镶嵌在纳米孔中,制备出高发光效率的纳米发光聚合物阵列,其光学特性与MEH-PPV薄膜显著不同。纳米孔内的MEH-PPV分子链形成链束,链束中的分子链数目依赖于制备纳米MEH-PPV阵列所用溶液的浓度。相对于稀溶液,在由浓溶液制备的纳米MEH-PPV阵列中,MEH—PPV链束的分子链数目较多,链间作用使MEH-PPV的能带展宽,能隙减小,因而浓溶液获得的纳米MEH—PPV阵列的光致发光峰红移。热处理纳米MEH-PPV阵列的PL谱表明,纳米孔内的聚合物分子链的弛豫运动受到限制。  相似文献   

7.
通过掺杂不同的染料有机电致发光器件可以得到不同颜色的光发射。掺杂小分子有机材料苝酸四甲酯perylene-3,4,9,10-tetracarboxvlicacid(TMEP)到蓝色发光聚合物poly(N—vinyl—carbazole)聚乙烯基咔唑(PVK),得到了很好的绿光发射。TEMP掺杂质量分数为0.01时,295.5nm激发波长的荧光光谱可以明显观察到在420nm处PVK和530nm处TEMP的发射峰值;当TMEP掺杂质量分数达到0.05~0.10之间,器件的电致发光光谱和荧光光谱发射峰几乎完全被TEMP的绿光所占据。光谱的转移归因于从聚合物PVK到小分子有机材料TMEP的Foerster能量转移。荧光光谱中随着TMEP掺杂浓度的的增大发射峰值有明显的红移,这种现象被归因于在TMEP高浓度掺杂情况下激基缔合物的形成。激基缔合物的形成从TMEP在薄膜状态下与溶液状态下的荧光光谱的比较中得到证实。  相似文献   

8.
崔海宁  王文韵 《发光学报》1992,13(2):165-170
本工作对无长链天然血卟啉(HP),原叶啉(PP)和卟啉C行进了LB膜的成膜探索,制备了单层、多层以及与硬脂酸、卵磷脂混合后的复合LB膜.对它们进行了紫外——可见吸收光谱、荧光光谱和时间分辨荧光光谱的研究,发现在LB膜中荧光寿命是一个很好的表征手段.  相似文献   

9.
一种可溶喹吖啶酮衍生物LB膜的光谱特性   总被引:1,自引:0,他引:1  
采用表面压-分子面积(π~A)等温曲线、紫外-可见吸收谱和荧光光谱的方法研究了一种喹吖啶酮衍生物材料LB膜的制备及其光谱特性。实验表明,这种喹吖啶酮衍生物能够在水面上形成稳定的单分子膜,它与花生酸(AA)混合后不仅可以形成很好的单分子膜,而且可以较好的转移到固体基片上制备成LB膜多层膜。这种喹吖啶酮衍生物LB膜的紫外-可见吸收谱的吸收峰位较稀溶液发生了红移,这是由极性溶剂分子与其相互作用的结果。其溶液有很强的荧光效应,但LB膜没有荧光现象,原因是在LB膜中QAC16的浓度过高发生“自我猝息”而失光。它在溶液和LB膜中都是以单体的形式存在。  相似文献   

10.
纳米发光材料LnVO4:Eu(Ln=La,Gd,Y)的光谱研究   总被引:11,自引:0,他引:11  
采用络合溶胶 凝胶法制备了系列纳米发光材料LnVO4:Eu(Ln =La ,Gd ,Y) ,并采用X射线衍射(XRD)、红外光谱 (FTIR)、荧光光谱以及紫外 可见光谱 (UV Vis)对三种发光材料的结构以及发光性质进行研究。结果表明 :YVO4与GdVO4具有相同的结构 ,均属于四方晶系 ,二者具有相似的光谱性质 ;而LaVO4属于单斜晶系 ,受对称性的影响其光谱也相应的发生了变化 ,红外光谱和发射光谱的特征峰发生明显的宽化 ,紫外光谱峰的数目增多  相似文献   

11.
In this article, the historical development of spectroscopy is examined and the spectroscopy devices used today are described. Then, we focus on infrared (IR) spectroscopy, which cannot give valuable signal in aqueous solution. Attenuated total reflection (ATR)-IR technique solves the problem. In addition, we specifically mention newly developed disposable ATR-IR crystals and micromachined silicon (Si) ATR-IR. Disposable crystal systems and microfluidics systems can be integrated with existing miniature ATR analyzers. If the integration is successful, the technique might be used in biomedical measuring instruments, reactions' analyses, and ultra-high-pressure analyses.  相似文献   

12.
Various barium strontium titanate borosilicate glasses were prepared by a rapid melt-quench technique. Spectroscopic studies have been carried out on investigated glasses for their structural information. Infrared and Raman spectroscopic studies showed that these glasses are formed by glass-forming network of borate and silicate as well as network modifiers in the form of cations of alkaline earth atoms. The borate and silicate networks are modified by barium, strontium, titanium, and iron cations in glass matrix. The network of triborate unit is modified in tetraborate unit by adding ferric oxide in a glassy matrix. The optical studies are performed by ultraviolet-visible spectroscopy and it confirms that the band gap decreases with increase in the concentration of ferric oxide.  相似文献   

13.
Previous work involving the rotational spectrum of aniline was limited to the lower frequencies of 8-40 GHz with very few lines being assigned. This work extends the earlier studies. Here we present a much more extensive measurement and assignment of the rotational spectrum of aniline in the frequency range of 75-110 GHz. The observed frequencies have been assigned to the ground (0+), first (0), and second excited (1+) states in the inversion vibration. With the newly assigned lines, significantly improved rotational constants and all five centrifugal distortion constants have been obtained.  相似文献   

14.
The rotational spectra of 3-fluoropropyne in the ground and first excited acetylenic C-H stretch vibrational state have been measured. The pure rotational spectrum of the normal species and the 13C isotopomers were measured using FTMW-cwMW double-resonance spectroscopy based on the Autler-Townes (AC Stark) effect. The lineshape properties of this measurement make it possible to determine the transition strength, ΔJ-selection rules, and the relative energy ordering of the quantum states. The frequency accuracy of this technique is tested against a previous pure rotational study of 3-fluoropropyne. The rotational spectrum of vibrationally excited state was obtained through IR-FTMW-cwMW methods. In this technique a single-longitudinal-mode pulsed infrared laser source vibrationally excites the acetylenic C-H stretch with J-selectivity. The rotational spectrum of the excited state is then obtained by FTMW and FTMW-cwMW double-resonance methods. The excited-state measurements have a signal-to-noise ratio comparable to the pure rotational spectrum. The residuals in the excited-state fit are larger than those obtained in the ground-state fit. This greater deviation from a standard asymmetric top spectrum is most likely due to weak perturbations to the acetylenic C-H spectrum.  相似文献   

15.
Abstract: In the analysis of petroleum hydrocarbon–contaminated soils for total petroleum hydrocarbons (TPHs) and polycyclic aromatic hydrocarbons (PAHs), the roles of spectroscopic and nonspectroscopic techniques are inseparable. Therefore, spectroscopic techniques cannot be discussed in isolation. In this report, spectroscopic techniques including Raman, fluorescence, infrared, and visible and near-infrared (Vis-NIR) spectroscopies, as well as mass spectroscopy (coupled to a gas chromatograph) and nonspectroscopic techniques such as gravimetry, immunoassay, and gas chromatography with flame ionization detection are reviewed. To bridge the perceived gap in coverage of the quantitative applications of Vis-NIR spectroscopy in the rapid determination of TPHs and PAHs in soils, a detailed review of studies from the period 1999–2012 are presented. This report also highlights the strengths and limitations of these techniques and evaluates their performance from the perspective of their attributes of general applicability, namely economic portability, operational time, accuracy, and occupational health and safety considerations. Overall, the fluorescence spectroscopic technique had the best performance (85% total score) in comparison to the others, and the gravimetric technique performed the least (60% total score). Method-specific solutions geared toward performance improvement are also suggested.  相似文献   

16.
激光长程吸收光谱法测量高分辨率大气吸收光谱   总被引:11,自引:7,他引:4  
用脉冲可调谐光参量振荡器作光源 ,使用光程长达 1km的 8m长吸收池 ,采用分时复用的单探测器探测方法 ,组成测量系统 ,测量了一系列高分辨率的模拟和实际大气的吸收光谱。系统的灵敏度为 0 .5× 10 - 6cm- 1 ,分辨率为 0 .0 2cm- 1 。 1.315 μm附近实际大气的吸收光谱与HITRAN96模拟结果比较 ,强线符合得很好。水汽光谱的大多数强线的分子线强度相对误差在 10 %以下。  相似文献   

17.
18.
High-resolution spectra of VO have been reinvestigated in the 12 000-31 000 cm−1 region. VO was produced in a vanadium hollow cathode lamp by discharging 1.5 Torr of Ar and the spectra were recorded using a Fourier transform spectrometer. The oxygen needed to produce VO was present in the system as an impurity. Three new bands observed in the 21 000-22 100 cm−1 region have been attributed to a new 2Δ-12Δ electronic transition of VO. Two bands, with origins near 21 044 and 22 038 cm−1, have been assigned as the 0-1 and 0-0 bands of the 2Δ3/2-12Δ3/2 sub-band while a weak band with an origin near 21 975 cm−1 has been assigned as the 0-0 band of the corresponding 2Δ5/2-12Δ5/2 sub-band. A rotational analysis of these sub-bands has been obtained and spectroscopic constants have been extracted. The 12Δ state is known from the previous analyses of the doublet transitions of VO in the near infrared. The present observation has allowed the determination of the vibrational interval ΔG1/2 and the equilibrium rotational constants for the 12Δ3/2 state.  相似文献   

19.
The pure rotational spectra of the ground and five excited vibrational states of pyridine were measured, assigned and fit in the 75-110 and 260-370 GHz frequency bands. An improved set of spectroscopic constants was obtained for the ground state, and all the rotational and quartic centrifugal distortion constants were obtained for the excited vibrational states.  相似文献   

20.
Previous work involving the rotational spectrum of 2-aminopyridine was limited to the lower frequencies of 4-40 GHz with very few lines being assigned. This work extends this earlier study. Here we present a much more extensive measurement and assignment of the rotational spectrum of 2-aminopyridine in the frequency range of 75-110 GHz. The observed frequencies have been assigned to the ground (0+ state) and the first excited state in the inversion vibration (0 state). Measurements of these two states have been extended up to J=46. With the newly assigned lines, significantly improved rotational constants and all five centrifugal distortion constants have been obtained.  相似文献   

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