Laser properties of a conjugate polymer (MEH-PPV) in the liquid-excimeric state

We have studied the amplified spontaneous-emission characteristics (ASE) of conjugated poly[2-methoxy-5-(2-ethylhexyloxy)1,4-phenylenevinylene] MEH-PPV in a few organic solutions. The ASE of MEH-PPV appears to arise from its excimeric state. This is perhaps the first report, to the best of our knowledge, on an excimeric-liquid state laser. MEH-PPV in solutions of benzene or tetrahydrofuran (THF) was pumped by the second and third harmonics of an Nd:YAG (532 and 355 nm) for different pump-pulse energies. The ASE of MEH-PPV was compared with the conventional laser dyes Rhodamine B (Rh B) and Rhodamine 6G (Rh 6G). The most important and distinguishing features are: (a) MEH-PPV has a four-times better photochemical stability than Rh B or Rh 6G; (b) the threshold and concentration for the laser action in MEH-PPV is far less than Rh B or Rh 6G.     

Excimer state of a conjugate polymer (MEH-PPV) in liquid solutions

The conjugated polymer poly[2-methoxy-5-(2-ethylhexyloxy)-1,4-phenylenevinylene] (MEH-PPV) is an important electrooptical material, which is useable as an excellent laser media. In this paper, we present the absorption and fluorescence spectral characteristics of MEH-PPV in a few organic solvents. The paper shows that MEH-PPV exists in an excimeric state in benzene, and that the laser action as shown here arises from a liquid excimeric state.     

Amplified spontaneous emission from internal energy transfer process in the copolymer BEHP-co-MEH-PPV

We have studied the Amplified Spontaneous Emission (ASE) characteristics of the conjugated copolymer poly{[2-[2′,5′-bis(2″-ethylhexyloxy)phenyl]-1,4-phenylenevinylene]-co-[2-methoxy-5-(2′-ethylhexyloxy)-1,4-phenylenevinylene]} (BEHP-co-MEH-PPV) in a few organic solutions under optical pumping by the third harmonic of Nd:YAG (355 nm). The results show that in BEHP-co-MEH-PPV, the BEHP-PPV component is capable of forcing MEH-PPV to produce ASE at 560 nm, which appears to arise out of the non-excimeric state of MEH-PPV.The ASE of BEHP-co-MEH-PPV was also compared with the conventional laser dyes Rhodamine B (Rh B), Rhodamine 6G (Rh 6G), and also the new laser material MEH-PPV.     

Laser from external energy transfer of MEH–PPV conjugated polymer

Mixtures made of poly[2-methyl-5-(2-ethyl-hexyloxy)-1,4-phenylene vinylene] (MEH–PPV) conducting polymer and cresyl violet 670 have been utilized for studying the amplified spontaneous emission characteristics (ASE) in an organic solution under laser excitation. In our earlier communication, we had shown that MEH–PPV alone could produce ASE under pulsed Nd: YAG laser excitation only in its excimeric state. In a follow up study reported here, a mixture of MEH–PPV and cresyl violet in benzene at different ratios were prepared. The results showed that when the mixture was pumped by the third harmonic of Nd: YAG (355 nm), MEH–PPV as a part of the mixture could get excited by pump laser pulse excitation, and transfer its excitation energy externally to cresyl violet to produce ASE. However, MEH–PPV represents here as a donor while CV served as an acceptor.     

Role of aggregation in the amplified spontaneous emission of [2-methoxy-5-(2′-ethylhexyloxy)-1,4-phenylenevinylene] in solution and films

The amplified spontaneous emission (ASE) spectra of the conjugated polymer [2-methoxy-5-(2′- ethylhexyloxy)-1,4-phenylenevinylene] (MEH-PPV) is investigated under different conditions such as thin film and solution, solvent type and concentration. Results indicate that aggregation has a pronounced effect on ASE spectra. In solution form, as concentration was increased and thus the proportion of aggregates, a decrease in the ASE emission bandwidth and a red shift of the ASE peak was observed. For the thin film samples, the ASE spectra show two emission bands which were assigned to the first and second vibronic transition of the polymer chains.     

Effect of different metal-backed waveguides on amplified spontaneous emission

We investigate the effect of a metallic electrode on the ability for poly[2-methoxy-5-(2’-ethylhexyloxy)-1,4phenylene vinylene](MEH-PPV) film to undergo amplified spontaneous emission(ASE).The threshold of the device with Ag cladding is about 10 times greater than that of a metal-free device,but metal such as Al completely shuts off ASE.The ASE recurs when a thin spacer layer,such as a few nanometers of SiO 2,is introduced between the MEH-PPV film and the Al cladding.Compared with the Cu or Al electrode,the Ag cladding is most suited to serve as an electrode with its low optical loss due to its high work-function and reflectivity.     

Ground state of π-conjugated polymer chains forming an intermolecular charge-transfer complex as probed by Raman spectroscopy

The intermolecular charge-transfer complex (CTC) between the conjugated polymer MEH-PPV and the low-molecular organic acceptor trinitrofluorenone (TNF) has been studied by Raman and optical absorption spectroscopy. On mixing MEH-PPV with TNF, an absorption band due to the CTC appeared in the optical gap of the polymer, whereas, in the Raman spectra, characteristic bands of the polymer are shifted and their widths and intensities change. The low-frequency shift of the strongest band at 1580 cm^?1 in the Raman spectrum of the polymer, assigned to the symmetric stretching vibration of the phenyl group, is shown to be due to electron density transfer from the π-conjugated system of the polymer to the acceptor and is as large as 5 cm^?1, which corresponds to a charge transfer on the order of 0.1e ^?1. Even at a low acceptor concentration (one TNF molecule per 10 monomer units of the polymer), most Raman-active conjugated chains are involved in the CTC. It is suggested that conjugated segments of the polymer can form a CTC of variable composition MEH-PPV: TNF = 1: X, where 0.1 ≤ X ≤ 0.5 (for each monomer unit of the polymer), and one TNF molecule can thereby interact with two conjugated segments of MEH-PPV. The conjugated polymer chains involved in the CTC can become more planar, and their interaction with the local environment can noticeably change; however, their conjugation length, most likely, remains unaltered.     

The dependence of the ideality factor on the charge density of a conjugated polymer (MEH-PPV) doped with some laser dyes

Blends made of poly[2-methyl-5-(2-ethyl-hexyloxy)-1,4-phenylene vinylene] (MEH-PPV) conducting polymer and cresyl violet 670 (CV) and coumarin 460 (C₄₆₀) have been utilized for preparation of organic Schottky diodes. The I–V characteristics of these diodes are then determined and interpreted in terms of thermoionic emission (TIE) conduction process. Upon blending MEH-PPV with CV and C₄₆₀ dyes, the conduction is seen to completely be through TIE conduction. The turn on voltage for MEH-PPV diode is found to be 2.0 V and decreases with CV blending in contrast to the blend of MEH-PPV-C₄₆₀. The Schottky parameters are determined where the potential barrier is found to be around 0.75 V which is consistent with reported values. The charge densities of the respective blends are calculated and found to reduce by in MEH-PPV-C₄₆₀ blends while it has been enhanced in the CV samples by an order of magnitude compared that of MEH-PPV. The correlation between the ideality factor with the dielectric constant and the charge density is inspected. It is found that the ratio between the charge density of the polymeric blend and the charge density of the Al-electrode is crucial for obtaining low ideality factor.     

Photoinduced C70 radical anions in polymer:fullerene blends

Photoinduced polarons in solid films of polymer:fullerene blends were studied by photoluminescence (PL), photoinduced absorption (PIA) and electron spin resonance (ESR). The donor materials used were P3HT and MEH‐PPV. As acceptors we employed PC₆₀BM as reference and various soluble C₇₀‐derivates: PC₇₀BM, two different diphenylmethano‐[70]fullerene oligoether (C₇₀‐DPM‐OE) and two dimers, C₇₀–C₇₀ and C₆₀–C₇₀. Blend films containing C₇₀ revealed characteristic spectroscopic signatures not seen with C₆₀. Light‐induced ESR showed signals at g ≥ 2.005, assigned to an electron localized on the C₇₀ cage. The formation of C₇₀ radical anions also leads to a subgap PIA band at 0.92 eV, hidden in the spectra of C₇₀‐based P3HT and MEH‐PPV blends, which allows for more exact studies of charge separated states in conjugated polymer:C₇₀ blends. (© 2011 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)     

高分子发光二极管载流子注入过程研究

采用交流阻抗谱，电容-电压，电容-频率等实验方法，研究了共轭高分子MEH-PPV(poly［2-methoxy，5-(2-ethylhexoxy)-1，4-phenylene vinylene］)发光二极管的载流子注入过程.对于结构为ITO/PEDOT/MEH-PPV/Ba/Al的发光器件，实验结果表明，电极界面是欧姆接触的，载流子的注入是非平衡的，器件薄膜中存在陷阱容易俘获注入电荷，形成空间电荷区，陷阱密度约为3.75×10¹⁶cm^-3. 关键词： 高分子发光二极管 交流阻抗谱 cole-cole图 载流子注入     

基于TiO_2纳米粒子薄膜的低阈值随机激光器的动力学研究

本文利用共轭聚合物(MEH-PPV)覆盖TiO_2纳米粒子薄膜制作随机激光器。随机TiO_2纳米粒子薄膜的激光辐射阈值比平面MEH-PPV薄膜的放大自发辐射阈值缩小了9倍。这是由于TiO_2纳米粒子诱导的多重散射造成的。进一步的飞秒荧光上转换实验表明,随机激光器中,光在增益介质里的停留时间有所增加,这直接证实了光在随机激光器结构中的多重散射引起光的传播路径增加。因此,这会促进更多的光发生辐射,从而降低随机激光器的阈值。     

MEH-PPV与TiO2共混体系太阳电池性能分析

以MEH-PPV(poly(2-methoxy-5-(2′-ethylhexoxy)-1,4-phenylene vinylene)为电子给体材料(Donor,D), TiO₂纳米线为电子受体材料(Acceptor,A),制成了共混体系太阳电池. 从D/A材料共混体系的紫外可见吸收光谱(UV-vis)、光荧光谱(PL)、器件的电荷传输的光导J-V图等方面,分析了MEH-PPV∶TiO₂体系器件性能变化的原因. 得出了当在纯MEH-PP 关键词： 太阳电池 聚合物 性能     

富勒烯C60掺杂的共轭高聚物混合薄膜的光谱性质

测量了不同富勒烯C60掺杂浓度的聚对亚苯基亚乙烯衍生物（MEH-PPV）混合薄膜的紫外-可见吸收光谱、稳态荧光和时间分辨荧光光谱。观察到MEH-PPV吸收峰受到明显的抑制以及荧光峰的猝灭。证明混合薄膜内，由于л-л共轭体系的强相互作用在基态发生MEH-PPV向C60的电子转移、形成电荷转移络合物。在光激发下会发生MEH-PPV向C60的激发传递进一步抑制了发光跃迁过程，导致了MEH-PPV荧光的强猝灭效应。     

Amplified spontaneous emission from metal-backed poly[2-methoxy-5-(2’-ethylhexyloxy)-1,4-phenylenevinylene] film

We investigate the amplified spontaneous emission (ASE) from an Ag-backed poly[2-methoxy-5-(2’-ethylhexyloxy)1,4-phenylenevinylene] (MEH-PPV) film with different film thicknesses.The ASE characteristics of Ag-backed MEHPPV films with different thicknesses show that increasing the film thickness can reduce the influence of the Ag cladding.The threshold,the gain,and the loss of the device with a thickness of 170 nm are comparable to those of a metal-free device.The lasing threshold of this device is about 7.5 times that of a metal-free device.Our findings demonstrate that Ag-backed MEH-PPV film with an appropriate thickness can still be a good polymer gain material for the fabrication of solid-state lasers.     

Enhanced luminance efficiency of polymer light emitting diode by blending with ionic solid electrolytes

In this letter, we demonstrate that luminance efficiency of polymer light emitting diode can be significantly enhanced by adding a small amount of ionic solid electrolytes. Heterojunction polymer device, consist of MEH-PPV, C₆₀, methanofullerene([6,6}-phenyl C61-butyric acid methyl ester) PCBM and/or PEO as the active materials. It has been found that blending of ionic solid electrolytes, such as polyethylene oxide into active layer, enhances the luminance efficiency of polymer device. It is believed that the optimized polymer morphology improves carrier mobility of MEH-PPV. Paper presented at the Third International Conference on Ionic Devices (ICID 2006), Chennai, Tamilnadu, India, Dec. 7–9, 2006.     

Study of the sensing characteristics of light emitting conjugated polymer MEH-PPV for nitro aromatic explosives

The sensing characteristics of light emitting conjugated polymer MEH-PPV for nitro aromatic explosives were studied in this paper. MEH-PPV was deposited on the surface of U-shaped plastic optical fiber (POF) using dip-coating techniques. The influences of MEH-PPV concentrations and bending radius of the U-shaped sensor heads on the sensitivity of the sensor were studied. The sensor was found to be most sensitive to TNT range from 0 to 4 mg/100 ml and the sensitivity was about 4 ng/ml. The limit of detections was around 1–10 ng/ml. It was also found that the conjugated polymer changes color from red to brownish black when the sensor head was put into TNT solution which provided high selectivity for sensing TNT at room temperature.     

聚合物发光二极管中的负电容效应

采用交流阻抗谱技术,研究了以共轭聚合物(poly［2-methoxy,5-(2′-ethylhexoxy)-1,4-phenylenevinylene］)(MEH-PPV)为发光层,以带有胺基的聚芴共聚物poly［(9,9-bis(3′-(N,N-dimethylamino)propyl)-2,7-fluorene)-alt-2,7-(9,9-dioctylfluorene)］ (PF-NR₂)为电子传输层的发光二极管的交流响应特性. 对于结构为ITO/P 关键词： 2')" href="#">PF-NR₂ 聚合物发光二极管 交流阻抗谱 负电容效应     

MEH-PPV薄膜的放大自发发射特性

研究了MEH-PPV薄膜的放大自发发射特性。当激发强度增加时,从样品边缘发射的光谱发生增益窄化现象并具有明显的阈值特性。我们发现随着薄膜厚度的增加,MEH-PPV薄膜的阈值有所降低,而其增益系数则随之增加。在150nm厚时测得最大净增益系数为25.03cm^-1,最低阈值为2.2μJ/pulse。结果表明MEH-PPV是一种优良的激光和光放大材料。     

Raman spectroscopic identification of fullerene inclusions in polymer/fullerene blends

Thin films of the conjugated polymer poly(3‐hexylthiophene) (P3HT) and blends of the soluble fullerene derivative[6,6]‐phenyl C₆₁‐butyric acid methyl ester (PCBM) with P3HT—a well studied but not completely understood donor–acceptor system for organic solar cells—have been studied by means of UV–visible absorption and resonant Raman spectroscopy. Additionally, we have employed atomic force microscopy phase imaging to characterize the nanomorphology of the P3HT : PCBM thin film, revealing a close intermixing of two phases with domain sizes ranging from a few to several tens of nanometers. A systematic analysis of pristine polymer and blend Raman spectra provides evidence that features attributable to PCBM, possibly even depending on the charge state of the fullerene molecule, can be observed. Hence our results suggest that fullerene inclusions in polymer/fullerene blends can be identified via Raman spectroscopy. Copyright © 2011 John Wiley & Sons, Ltd.     

The stimulated Raman scattering competition between solute and solvent in Rhodamine B solution

The competition between the stimulated resonance Raman scattering (SRRS) of Rhodamine B (RhB) and the stimulated Raman scattering (SRS) of ethanol (C₂H₅OH) is observed at the RhB in C₂H₅OH solution. For different concentrations of the solution, the peak wavelengths of the SRRS, the amplified spontaneous emission (ASE), the fluorescence and the absorption of RhB are different. The SRRS of RhB and the SRS of C₂H₅OH are simultaneously generated when the concentration of the solution is 10^-5 mol/L and the energy of the excitation laser is 20.4 mJ. Otherwise, only either the SRRS of RhB or the SRS of C₂H₅OH is generated. The SRRS can be amplified by the ASE gain when the SRRS is near the peak of the ASE, and the peak wavelength of the SRRS coincides with the wavelength of the maximal intensity ASE.