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首页> 外文期刊>Bulletin of the Korean Chemical Society >Carbon-13 Nuclear Magnetic Resonance Spectroscopic Studies of 13CO Adsorbed on Platinum Particles in L-Zeolites
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Carbon-13 Nuclear Magnetic Resonance Spectroscopic Studies of 13CO Adsorbed on Platinum Particles in L-Zeolites

机译:L-沸石中13CO吸附在铂颗粒上的碳13核磁共振光谱研究

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摘要

13CO chemisorbed on platinum particles in L-zeolite has been investigated by static and magic angle spinning NMR spectroscopy. The representative spectra are composed of a broad asymmetric peak with a center of gravity at 230【30 ppm and a sharp symmetric peak at 124【2 ppm which is tentatively assigned to physisorbed CO, on inner walls of L-zeolite. Overall, the broad resonance component is similar to our previous results of highly dispersed (80-96%) CO/Pt/silica or CO/Pt/alumina samples, still showing metallic characters. The principal difference is in the first moment value. The broad peak in the spectra is assigned to CO linearly bound to Pt particles in the L-zeolites, and indicates a distribution of isotropic shifts from bonding site to bonding site. The NMR results reported here manifest that the Pt particles inside of the L-zeolites channels are not collectively the same with the ones supported on silica or alumina with similar dispersion in terms of Pt particle shape and/or ordering of Pt atoms in a particle. As a result, Pt particles of CO/Pt/L-zeolite were agglomerated accompanying CO desorption upon annealing. There were no definite changes in the NMR spectra due to differences of exchanged cations. Comparison of our observation on CO/Pt/L-zeolite with Sharma et al.`s reveals that even when the first moment, the linewidtb, and the relaxation times of the static spectra and the dispersion measured by chemisorption are similar, the properties of Pt particles can be dramatically different. Therefore, it is essential to take advantage of the strengths of several techniques together in order to interpret data reliably, especially for the highly dispersed samples.
机译:通过静态和魔角旋转NMR光谱研究了化学吸附在L型沸石中铂颗粒上的13CO。代表性的光谱由L型沸石内壁上一个重心为230【30 ppm的宽不对称峰和一个124【2 ppm的尖锐的对称峰组成。总体而言,广泛的共振成分类似于我们先前对高度分散的(80-96%)CO / Pt /二氧化硅或CO / Pt /氧化铝样品的结果,但仍显示出金属特征。主要区别在于第一时刻的值。光谱中的宽峰归属于线性键合到L沸石中Pt颗粒的CO,表明从键合位点到键合位点的各向同性位移分布。此处报道的NMR结果表明,L-沸石通道内的Pt颗粒与Pt颗粒形状和/或颗粒中Pt原子的有序分散在二氧化硅或氧化铝上负载的颗粒具有相似的分散性。结果,伴随退火时CO的脱附,CO / Pt / L-沸石的Pt颗粒附聚。由于交换阳离子的差异,NMR光谱没有确定的变化。我们与Sharma等人在CO / Pt / L沸石上观察到的结果进行比较后发现,即使在第一时刻,线宽,静态光谱的弛豫时间和通过化学吸附法测得的分散度相似,铂粒子可能有很大的不同。因此,必须充分利用多种技术的优势才能可靠地解释数据,尤其是对于高度分散的样品。

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