Yamazaki Suzuko, Isoyama Koki
Department of Chemistry, College of Science, Graduate School of Sciences and Technology for Innovation, Yamaguchi University, Yamaguchi 753-8512, Japan.
Langmuir. 2023 Jul 25;39(29):10240-10248. doi: 10.1021/acs.langmuir.3c01227. Epub 2023 Jul 11.
Tungsten oxide (WO) has been extensively studied for various photochromic applications. Blue coloration of WO is explained in terms of the intervalence charge transfer (IVCT) transition of electrons between W and W. However, various absorption spectra with different shapes have been reported. Herein, a transparent film was prepared by drying aqueous solutions containing polyvinyl alcohol, WO nanoparticles and ethylene glycol (EG). For comparison, the photochromic behavior of an aqueous WO colloidal solution containing EG was also investigated. Under UV irradiation, a single intense peak was always observed at ca. 777 nm in the colloidal solution, but the absorption spectra of the film changed from a peak at 770 nm to two distinct peaks at 654 and 1003 nm. All absorption spectra observed with the film and the colloidal solution were deconvoluted into five peaks at 540, 640, 775, 984, and 1265 nm. Kinetic studies using the colloidal solution indicated that the coloration rates () estimated at the deconvoluted peaks of 640, 775, and 984 nm followed the same rate law. On the other hand, in the case of the film, evaluated at 640 or 984 nm was independent of the water amounts but increased proportionally to the EG amounts and the light intensity, although at 775 nm significantly increased with the increasing amounts of water and EG. Raman and electron spin resonance spectroscopic observations of the film revealed that the photogenerated electrons migrated toward the terminal W═O moiety to accumulate and then a small anisotropic electron spin resonance signal appeared. Our study demonstrates that the absorption at 775 nm is due to IVCT between W and W, which is stabilized with water in the bulk and the absorption peaks at 640 and 984 nm are attributable to IVCT on the WO surface.
氧化钨(WO)已针对各种光致变色应用进行了广泛研究。WO的蓝色是根据W与W之间电子的价间电荷转移(IVCT)跃迁来解释的。然而,已报道了各种形状不同的吸收光谱。在此,通过干燥含有聚乙烯醇、WO纳米颗粒和乙二醇(EG)的水溶液制备了透明薄膜。为作比较,还研究了含有EG的WO水性胶体溶液的光致变色行为。在紫外线照射下,胶体溶液中始终在约777nm处观察到一个单一的强峰,但薄膜的吸收光谱从770nm处的一个峰变为654和1003nm处的两个不同峰。用薄膜和胶体溶液观察到的所有吸收光谱都被解卷积为540、640、775、984和1265nm处的五个峰。使用胶体溶液的动力学研究表明,在640、775和984nm的解卷积峰处估计的着色速率()遵循相同的速率定律。另一方面,在薄膜的情况下,在640或984nm处评估的与水量无关,但与EG量和光强度成比例增加,尽管在775nm处随着水和EG量的增加而显著增加。薄膜的拉曼光谱和电子自旋共振光谱观察表明,光生电子向末端W═O部分迁移并积累,然后出现一个小的各向异性电子自旋共振信号。我们的研究表明,775nm处的吸收是由于W与W之间的IVCT,其在本体中用水稳定,而640和984nm处的吸收峰归因于WO表面上的IVCT。