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Couches auto-assemblées comme interfaces des dispositifs électroluminescents organiques

机译:自组装层作为有机电致发光器件的界面

摘要

Organic light emitting devices (OLED) are among the most promising future technologies for the manufacture of flat and inexpensive displays. Although OLEDs provide already much higher brightness as compared to liquid crystals devices (LCD), they have a major drawback which limits their industrialisation; they are degrading too quickly. Among the factors acting on the performance of OLEDs, interfaces play an important role. The purpose of this work is to develop stable interfaces by using self-assembled monolayers at the device electrodes. Monolayers of para substituted benzoic acids, grown by the traditional method of self-assembly in solution, were characterised by Langmuir isotherms. The experiments showed that the layers are compact, but the binding between the surface and the adsorbed molecule is weak: -5,7 kJ·mole-1 on indium tin oxide (ITO) and -10,6 kJ·mole-1 on aluminium. These molecules allowed to increase the anode surface potential by 0,2 eV and to decrease the one of the cathode by -0,2 eV. Although giving encouraging results, this method has several disadvantages related to the use of a solvent. This is one reason why a new way of growing self-assembled monolayers was developed, the self-assembly from vapour phase. This new grafting method made it possible to increase the surface potential of ITO by 1,4 eV and to decrease the one of aluminium by 0,9 eV using the same molecules as in solution. Another advantage of this technique is the short growing time of the monolayers. Only one minute is necessary to graft the electrode which is considerably shorter than for the traditional technique where 12 hours are necessary. Moreover, it seems that under clean vacuum conditions, the effect on the surface potential depends only on the molecule and not on the surface composition, nor on the initial potential. Finally, this method allowed to discriminate between the different dipole contributions involved in the surface potential modification by the self-assembled monolayers. In a further step, the extended electrode interface consisting of the self-assembled layer covered by an electroactive material was studied. It appears that the organic material partly screens the monolayer dipole moment due to its polarisability. When the initial electrode surface potential of the modified electrode is far apart from the highest occupied or the lowest unoccupied molecular orbitals of the organic material, no charge transfer is expected and the variation in the surface potential comes only from the polarisability of the material. This variation is weaker in the case of a non-polar substituted diamine, α-NPD (the maximum is 0,3 eV) than in the case of the widely used aluminium complex, Alq3, which has a permanent electrical dipole and thus can induce shifts up to 0,7 eV. On the other hand, if the surface potential is close to the energy level of the occupied or unoccupied molecular orbitals, spontaneous charge transfer can occur between the electrode and the organic material. This increases considerably the measured potential variation during the deposition of the electroactive material. With α-NPD, variations of 0,6 eV are observed and in the case of Alq3 shifts are as important as 0,9 eV. Those negative effects can be decreased by the use of an aliphatic chain between the attachment group and the aromatic cycle in the adsorbed molecules. This positive effect is considerable: it can decrease the electrostatic screening of the adsorbed dipole layer by the electroactive material and prevent the charge transfer induced by the image force effect. Finally, homopolar and bipolar devices were studied to investigate the effect of self-assembled monolayers on the device characteristics. In particular, "electron-only" devices were studied using a grafted or a bare aluminium cathode. To study the injection of holes, homopolar and bipolar devices were conceived, having a grafted or a bare ITO anode. The results clearly demonstrate the decrease of the threshold voltage by using suitable self-assembled monolayers. The reasons for this decrease are numerous: improved alignment of the energy levels due to the permanent electrical dipole of the adsorbates, insulating spacer effect due to the aliphatic chains of some of the molecules and improvement of film morphology.
机译:有机发光器件(OLED)是用于制造平面和廉价显示器的最有前途的未来技术之一。尽管OLED与液晶设备(LCD)相比已经提供了更高的亮度,但它们的主要缺点限制了其工业化;他们的退化太快了。在影响OLED性能的因素中,接口扮演着重要角色。这项工作的目的是通过在器件电极上使用自组装单层膜来开发稳定的界面。通过传统的自组装方法在溶液中生长的对位取代的苯甲酸单层以朗缪尔等温线为特征。实验表明,这些层是致密的,但表面与吸附分子之间的结合较弱:在铟锡氧化物(ITO)上为-5,7 kJ·mole-1,在铝上为-10,6 kJ·mole-1 。这些分子允许将阳极表面电势提高0.2 eV,并使阴极之一降低-0.2 eV。尽管给出令人鼓舞的结果,但是该方法具有与使用溶剂有关的若干缺点。这就是为什么开发一种新的自组装单层生长方法的原因,即汽相自组装。使用与溶液中相同的分子,这种新的接枝方法可以将ITO的表面电势提高1.4 eV,将铝的电势降低0.9 eV。该技术的另一个优点是单层的生长时间短。嫁接电极只需要一分钟,这比需要12个小时的传统技术要短得多。而且,似乎在干净的真空条件下,对表面电势的影响仅取决于分子,而不取决于表面组成,也不取决于初始电势。最后,该方法可以区分由自组装单分子层引起的表面电势改性所涉及的不同偶极子贡献。在进一步的步骤中,研究了由被电活性材料覆盖的自组装层组成的扩展电极界面。看来有机材料由于其极化性而部分屏蔽了单层偶极矩。当改性电极的初始电极表面电势与有机材料的最高占据或最低未占据分子轨道相距较远时,则不会发生电荷转移,并且表面电势的变化仅来自于材料的极化率。在非极性取代的二胺α-NPD(最大值为0.3 eV)的情况下,这种变化要比在广泛使用的具有永久电偶极子的铝配合物Alq3的情况下弱。上移至0.7 eV。另一方面,如果表面电势接近于被占据或未被占据的分子轨道的能级,则在电极和有机材料之间会发生自发的电荷转移。这大大增加了电活性材料沉积过程中测得的电势变化。对于α-NPD,观察到0.6 eV的变化,在Alq3位移的情况下,其变化与0.9 eV一样重要。通过在连接基团和吸附的分子中的芳族环之间使用脂族链,可以减少那些负面影响。这种积极的作用是相当大的:它可以减少电活性物质对吸附的偶极子层的静电屏蔽,并防止像力效应引起的电荷转移。最后,对单极和双极器件进行了研究,以研究自组装单分子膜对器件特性的影响。特别是,使用接枝的或裸露的铝阴极研究了“纯电子”器件。为了研究空穴的注入,设想了具有接枝的或裸露的ITO阳极的单极和双极器件。结果清楚地表明,通过使用合适的自组装单分子层,阈值电压降低了。减少的原因很多:由于吸附物的永久电偶极子导致的能级排列改善,由于某些分子的脂肪族链引起的绝缘间隔效应以及膜形态的改善。

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    Carrara Michel;

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  • 年度 2002
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  • 原文格式 PDF
  • 正文语种 fre
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