Lexow Matthias, Heller Bettina S J, Maier Florian, Steinrück Hans-Peter
Lehrstuhl für Physikalische Chemie 2, Friedrich-Alexander-Universität Erlangen-Nürnberg, Egerlandstr. 3, 91058, Erlangen, Germany.
Chemphyschem. 2018 Nov 19;19(22):2978-2984. doi: 10.1002/cphc.201800773. Epub 2018 Sep 24.
Thin ionic liquid (IL) films play an important role in many applications. To obtain a better understanding of the ion distribution within IL mixture films, we sequentially deposited ultrathin layers of two ILs with the same cation but different anions onto Ag(111), and monitored their dynamic behaviour by angle-resolved X-ray photoelectron spectroscopy. Upon depositing [C C Im][PF ] on top of a wetting layer of [C C Im][Tf N] at room temperature (RT), we found a pronounced enrichment of the [Tf N] anions at the IL/vacuum interface, due to a rapid anion exchange at the IL/solid interface. In contrast, at 90 K, the [Tf N] anions remain at the IL/solid interface. Upon heating, we observe a rearrangement of the cations between 140 and 160 K, such that the octyl chains preferentially point towards the vacuum. Above 170 K, the ions start to become mobile, and at 220 K, the anion exchange is completed, with the [Tf N] anions enriched at the IL/vacuum interface in the same way as found for deposition at RT. The temperature range for the anion exchange corresponds well to glass transition temperatures reported in literature. We propose two driving forces to be cooperatively responsible for the replacement/exchange of [Tf N] at the IL/solid interface and its enrichment at the IL/vacuum interface. First, the adsorption energy of [C C Im][PF ] is significantly larger than that of [C C Im][Tf N], and second, the surface tension of [C C Im][Tf N] is lower than that of [C C Im][PF ].
薄离子液体(IL)膜在许多应用中发挥着重要作用。为了更好地理解IL混合膜内的离子分布,我们将具有相同阳离子但不同阴离子的两种IL的超薄层依次沉积在Ag(111)上,并通过角分辨X射线光电子能谱监测它们的动态行为。在室温(RT)下将[C C Im][PF ]沉积在[C C Im][Tf N]的润湿层之上时,我们发现由于IL/固体界面处的快速阴离子交换,[Tf N]阴离子在IL/真空界面处显著富集。相比之下,在90 K时,[Tf N]阴离子保留在IL/固体界面处。加热时,我们观察到阳离子在140至160 K之间发生重排,使得辛基链优先指向真空。高于170 K时,离子开始变得可移动,在220 K时,阴离子交换完成,[Tf N]阴离子以与RT沉积时相同的方式在IL/真空界面处富集。阴离子交换的温度范围与文献报道的玻璃化转变温度很好地对应。我们提出两种驱动力共同负责IL/固体界面处[Tf N]的置换/交换及其在IL/真空界面处的富集。首先,[C C Im][PF ]的吸附能明显大于[C C Im][Tf N]的吸附能,其次,[C C Im][Tf N]的表面张力低于[C C Im][PF ]的表面张力。