To investigate the redox properties of fresh and K-poisoned catalysts, XPS was applied to probe the electron states of V and O on the surface of catalysts. As shown in
Fig. 2c, the XPS spectra of V 2p show two characteristic binding energies of V 2p
3/2 and V 2p
1/2, where the peaks around 516 and 524 eV are attributed to V
4+ species while the peaks around 517 and 525 eV are ascribed to V
5+ [
23]. It can be found that the V
4+/(V
4++V
5+) ratio (47.5%) on CeSV/Ti is higher than that (40.0%) on V/Ti, evidencing the strong interaction between Ce and V species over CeSV/Ti. The lower valence of V over CeSV/Ti indicates that the electron could transfer from Ce to V. After K-poisoning, the V
4+/(V
4++V
5+) of K-V/Ti increases markedly to 72.4% while that (50.3%) of K-CeSV/Ti hardly changes compared to the fresh catalysts. The significant increase in V
4+ fraction of K-V/Ti is attributed to the electron-donating effects of K that increase the electron density of V species. This also demonstrates that K strongly interacts with V species after K-poisoning. Differently, the maintenance of V valence over K-CeSV/Ti implies that K strongly interacts with Ce(SO
4)
2 rather than V. The O 1s XPS spectra were used to investigate the varieties and contents of surface oxygen species. The surface oxygen atomic percent (53.8%) of CeSV/Ti is much higher than that (27.0%) of V/Ti, which is attributed to the oxygen species of Ce(SO
4)
2 (Table S3 in Supporting information). After K-poisoning, the surface oxygen atomic percent of K-CeSV/Ti slightly decreases to 46.5% while that of K-V/Ti increases to 45.6%. These results imply that K
2O is mainly bonded on Ce(SO
4)
2 sites of K-CeSV/Ti but cover on the surface of K-V/Ti. As shown in
Fig. 2d, there are adsorbed oxygen (O
α) species around 531 eV and lattice oxygen (O
β) species around 530 eV [
24-
31]. Ce(SO
4)
2 modification increases the O
α fraction of V/Ti from 18.1% to 27.8%, likely due to the contribution of surface SO
42−. After K-poisoning, the O
α species of K-CeSV/Ti decrease notably to 16.3% while that of K-V/Ti keeps unchanged at 18.9%, respectively. It can be inferred that SO
42− of Ce(SO
4)
2 strongly interacts with K over K-CeSV/Ti, which leads to the decrease of O
α species. By the contrast, K
2O covers on the surface of K-V/Ti that results in the unchanged amount of O
α species because of the O
α species of K
2O. In order to probe the interaction between Ce and K species on the K-CeSV/Ti catalysts, the XPS spectra of Ce 3d and K 2p are investigated over CeSV/Ti, K-CeSV/Ti and K-V/Ti catalysts (
Figs. 2e and
f). The peaks labelled as
v,
v'',
v''' and
u,
u'' and
u''' at 882, 888.9, 898, 901, 907 and 916.8 eV are attributed to the 3d
104f
0 Ce
4+ state, while the peaks labeled
v′ and
u′ observed at 885 and 903 eV are ascribed to the 3d
104f
1 Ce
3+ state (
Fig. 2e) [
28]. It can be found that the ratio of Ce
3+/(Ce
3++Ce
4+) (31.1%) of K-CeSV/Ti is higher than that (27.8%) of CeSV/Ti, indicating the more electron-rich state of Ce in K-CeSV/Ti. On the other hand, the XPS spectra of K 2p were also investigated over K-CeSV/Ti and K-V/Ti catalysts. As seen in
Fig. 2f, the binding energy of K on K-CeSV/Ti is higher than that on K-V/Ti, indicating the electron deficient state of K on the former one. Based on these results, it can be inferred that K is bonded on Ce(SO
4)
2 sites, leading to the transfer of electron from K to Ce species.