A Resol‐assisted Cationic Coordinative Co‐assembly Approach to Mesoporous ABO3 Perovskite Oxides with Rich Oxygen Vacancy for Enhanced Hydrogenation of Furfural to Furfuryl Alcohol

2020 ◽  
Author(s):  
Yuenan Zheng ◽  
Rui Zhang ◽  
Ling Zhang ◽  
Qinfen Gu ◽  
Zhen-An Qiao
2021 ◽  
Vol 542 ◽  
pp. 148706
Author(s):  
Chengsong Zhang ◽  
Yun Wang ◽  
Dazhi Chen ◽  
Yeqiong Wu ◽  
Guodong Cui ◽  
...  

2019 ◽  
Vol 99 (6) ◽  
Author(s):  
Naoki Tsunoda ◽  
Yu Kumagai ◽  
Masahiko Araki ◽  
Fumiyasu Oba

1995 ◽  
Vol 134 (1-4) ◽  
pp. 75-77 ◽  
Author(s):  
M. A. Bunin ◽  
S. A. Prosandeyev ◽  
I. I. Gegusin ◽  
I. M. Tennenboum

2019 ◽  
Vol 7 (11) ◽  
pp. 6099-6112 ◽  
Author(s):  
Zhenpan Chen ◽  
Qingqing Jiang ◽  
Feng Cheng ◽  
Jinhui Tong ◽  
Min Yang ◽  
...  

Sr- and Co-doped perovskite oxides La1−xSrxGa1−yCoyO3−δ (LSGC) with controllable oxygen vancancy formation energy (EV) and oxygen vacancy concentration (−) are successfully developed to exhibit high O2 and H2 yields when reduced at 1350 °C and re-oxidized at optimized 400−1100 °C.


1996 ◽  
Vol 79 (2) ◽  
pp. 536-538 ◽  
Author(s):  
William L. Warren ◽  
Karel Vanheusden ◽  
Duane Dimos ◽  
Gordon E. Pike ◽  
Bruce A. Tuttle

2009 ◽  
Vol 182 (7) ◽  
pp. 1713-1716 ◽  
Author(s):  
Y. Matsuda ◽  
M. Karppinen ◽  
Y. Yamazaki ◽  
H. Yamauchi

1986 ◽  
Vol 0 (6) ◽  
pp. 449-451 ◽  
Author(s):  
Kanamaluru Vidyasagar ◽  
Laxminarayana Ganapathi ◽  
Jagannatha Gopalakrishnan ◽  
C. N. Ramachandra Rao

Symmetry ◽  
2021 ◽  
Vol 13 (10) ◽  
pp. 1920
Author(s):  
Roberts I. Eglitis ◽  
Juris Purans ◽  
Anatoli I. Popov ◽  
Ran Jia

We computed the atomic shift sizes of the closest adjacent atoms adjoining the (001) surface F-center at ABO3 perovskites. They are significantly larger than the atomic shift sizes of the closest adjacent atoms adjoining the bulk F-center. In the ABO3 perovskite matrixes, the electron charge is significantly stronger confined in the interior of the bulk oxygen vacancy than in the interior of the (001) surface oxygen vacancy. The formation energy of the oxygen vacancy on the (001) surface is smaller than in the bulk. This microscopic energy distinction stimulates the oxygen vacancy segregation from the perovskite bulk to their (001) surfaces. The (001) surface F-center created defect level is nearer to the (001) surface conduction band (CB) bottom as the bulk F-center created defect level. On the contrary, the SrF2, BaF2 and CaF2 bulk and surface F-center charge is almost perfectly confined to the interior of the fluorine vacancy. The shift sizes of atoms adjoining the bulk and surface F-centers in SrF2, CaF2 and BaF2 matrixes are microscopic as compared to the case of ABO3 perovskites.


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