Interface properties and electronic structure of ultrathin manganese oxide films on Ag(001)

2007 ◽  
Vol 601 (18) ◽  
pp. 4484-4487 ◽  
Author(s):  
M. Nagel ◽  
I. Biswas ◽  
H. Peisert ◽  
T. Chassé
2021 ◽  
Vol 13 (2) ◽  
pp. 2428-2436
Author(s):  
Paul Plate ◽  
Christian Höhn ◽  
Ulrike Bloeck ◽  
Peter Bogdanoff ◽  
Sebastian Fiechter ◽  
...  
Keyword(s):  

2004 ◽  
Vol 19 (8) ◽  
pp. 2421-2427 ◽  
Author(s):  
Shota Kobayashi ◽  
Tatsuya Usui ◽  
Hiromasa Ikuta ◽  
Yoshiharu Uchimoto ◽  
Masataka Wakihara

The microwave irradiation technique (MWIT) was applied to synthesize lithium manganese oxide having spinel structure using LiOH·H2O and ε–MnO2 as starting materials. The crystal and electronic structure depends on the irradiation time; x-ray diffraction patterns of the sample irradiated for 9 min were in good agreement with that of cubic structure without showing the peak of MnO2. The electronic structure of synthesized samples before and after lithium ion intercalation and/or deintercalation was investigated by Mn L-edge and O K-edge x-ray absorption spectroscopy.


ChemSusChem ◽  
2018 ◽  
Vol 11 (15) ◽  
pp. 2554-2561 ◽  
Author(s):  
Carsten Walter ◽  
Prashanth W. Menezes ◽  
Stefan Loos ◽  
Holger Dau ◽  
Matthias Driess

2013 ◽  
Vol 1537 ◽  
Author(s):  
Chenggong Wang ◽  
Irfan ◽  
Yongli Gao

AbstractWe have investigated the counter intuitive phenomenon of inserting a metal oxide layer to improve hole injection or extraction in organic semiconductor devices using ultraviolet photoemission, x-ray photoemission, and inverse photoemission spectroscopy (UPS, XPS and IPES). We observed that metal oxides, such as MoO3, substantially increase the work function when deposited on indium-tin-oxide (ITO). The increase lifts up the highest occupied molecular orbital (HOMO) of the hole transport layer, therefore reduces the energy barrier between the HOMO and the Fermi level of the anode. The uplift creates an interface band bending region that results in a drift electric field that encourages the collection of holes at the anode. The optimum thickness for the oxide layer is estimated to be 2 nm. We have also investigated the effects of ambient or O2 exposure of MoO3. We observed that while most of the electronic energy levels of the oxide remained largely intact, the work function reduction was significant. This opens a way for optimal energy level alignment by modifying the work function through exposure. Furthermore, we observed that the work function reduction by exposure could be reversed by proper annealing of the sample in vacuum. The investigations therefore point to manipulate the interface electronic structure and charge injection/extraction by thin metal oxide films.


2009 ◽  
Vol 203 (17-18) ◽  
pp. 2642-2645 ◽  
Author(s):  
N. Matsunami ◽  
O. Fukuoka ◽  
M. Tazawa ◽  
H. Kakiuchida ◽  
M. Sataka

2014 ◽  
Vol 926-930 ◽  
pp. 932-937 ◽  
Author(s):  
Wen Po Li ◽  
Xiu Li Zuo ◽  
Tang Man Lv ◽  
Sheng Tao Zhang

Nanostructured manganese oxide films were obtained by electro-oxidation of manganese films electrodeposited at two typical cathodic currents of 65 mA cm-2 (EDM-65 oxide) and 150 mA cm-2 (EDM-150 oxide) from sulfate solutions with additives. Obtained Mn oxide films were studied by scanning electron microscope, X-ray photoelectron spectroscopy, cyclic voltammetry and AC impedance. SEM study revealed that the Mn oxide films were mesoporous nanostructures on the EDM-150 oxide surface, while the EDM-65 oxide coating is homogeneous and compact. XPS results indicate that EDM-150 oxide had a higher content of anhydrous Mn oxide and structure water, which means that it had more anhydrous characteristics as compared to EDM-65 oxide. It was shown that porous nanostructured films showed good capacitive behavior for applications in electrochemical supercapacitors. The porous nanostructured films prepared at 150 mA cm-2 showed higher specific capacitance (SC) compared to the SC of the EDM-65 oxide films. The highest SC of 148 F g-1 in a voltage window of 0.8 V was obtained in 0.1 M Na2SO4 solutions at a scan rate of 25 mV s-1.


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