Internal magnetic field effect of transition metal ions on the photochemical reaction of naphthoquinone in micelles

1992 ◽  
Vol 162 (1) ◽  
pp. 119-129 ◽  
Author(s):  
Yoshio Sakaguchi ◽  
Hisaharu Hayashi
2007 ◽  
Vol 310 (2) ◽  
pp. 1162-1164 ◽  
Author(s):  
K. Noda ◽  
M. Akaki ◽  
F. Nakamura ◽  
D. Akahoshi ◽  
H. Kuwahara

2001 ◽  
Vol 105 (17) ◽  
pp. 3343-3345 ◽  
Author(s):  
M. Fujiwara ◽  
D. Kodoi ◽  
W. Duan ◽  
Y. Tanimoto

ChemInform ◽  
2010 ◽  
Vol 32 (39) ◽  
pp. no-no
Author(s):  
M. Fujiwara ◽  
D. Kodoi ◽  
W. Duan ◽  
Y. Tanimoto

Author(s):  
R. Ai ◽  
H.-J. Fan ◽  
L. D. Marks

It has been known for a long time that electron irradiation induces damage in maximal valence transition metal oxides such as TiO2, V2O5, and WO3, of which transition metal ions have an empty d-shell. This type of damage is excited by electronic transition and can be explained by the Knoteck-Feibelman mechanism (K-F mechanism). Although the K-F mechanism predicts that no damage should occur in transition metal oxides of which the transition metal ions have a partially filled d-shell, namely submaximal valence transition metal oxides, our recent study on ReO3 shows that submaximal valence transition metal oxides undergo damage during electron irradiation.ReO3 has a nearly cubic structure and contains a single unit in its cell: a = 3.73 Å, and α = 89°34'. TEM specimens were prepared by depositing dry powders onto a holey carbon film supported on a copper grid. Specimens were examined in Hitachi H-9000 and UHV H-9000 electron microscopes both operated at 300 keV accelerating voltage. The electron beam flux was maintained at about 10 A/cm2 during the observation.


2004 ◽  
Vol 9 (2) ◽  
pp. 129-138
Author(s):  
J. Kleiza ◽  
V. Kleiza

A method for calculating the values of specific resistivity ρ as well as the product µHB of the Hall mobility and magnetic induction on a conductive sample of an arbitrary geometric configuration with two arbitrary fitted current electrodes of nonzero length and has been proposed an grounded. During the experiment, under the constant value U of voltage and in the absence of the magnetic field effect (B = 0) on the sample, the current intensities I(0), IE(0) are measured as well as the mentioned parameters under the effect of magnetic fields B1, B2 (B1 ≠ B2), i.e.: IE(β(i)), I(β(i)), i = 1, 2. It has been proved that under the constant difference of potentials U and sample thickness d, the parameters I(0), IE(0) and IE(β(i)), I(β(i)), i = 1, 2 uniquely determines the values of the product µHB and specific resistivity ρ of the sample. Basing on the conformal mapping method and Hall’s tensor properties, a relation (a system of nonlinear equations) between the above mentioned quantities has been found.


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