Magnetic field effect on the low temperature triplet state population of an organic molecule

1977 ◽  
Vol 66 (1) ◽  
pp. 358-359 ◽  
Author(s):  
Richard H. Clarke ◽  
Robert E. Connors ◽  
Joseph Keegan
Keyword(s):  
Magnetic Field ◽  
Low Temperature ◽  
Triplet State ◽  
Field Effect ◽  
Organic Molecule ◽  
Magnetic Field Effect ◽  
State Population

Magnetic field effects of photocarrier generation in bulk heterojunctions at low temperature

2016 ◽  
Vol 45 (42) ◽  
pp. 16616-16623 ◽  
Author(s):  
H. Tajima ◽  
Y. Nishioka ◽  
S. Sato ◽  
T. Suzuki ◽  
M. Kimata
Keyword(s):  
Magnetic Field ◽  
Experimental Investigation ◽  
Low Temperature ◽  
Field Effect ◽  
Bulk Heterojunction ◽  
Magnetic Field Effect ◽  
Magnetic Field Effects ◽  
Bulk Heterojunctions ◽  
Polymer Bulk ◽  
The Magnetic Field

We report an experimental investigation of the magnetic field effect (MFE) in polymer bulk heterojunction devices at temperatures below 10 K using photocarrier extraction by linearly increasing voltages.

The Model for Calculation the Hall Effect Parameter

2004 ◽  
Vol 9 (2) ◽  
pp. 129-138
Author(s):  
J. Kleiza ◽  
V. Kleiza
Keyword(s):  
Magnetic Field ◽  
Field Effect ◽  
Magnetic Field Effect ◽  
Mapping Method ◽  
Sample Thickness ◽  
System Of Nonlinear Equations ◽  
Specific Resistivity ◽  
Conformal Mapping Method ◽  
Effect Parameter ◽  
The Magnetic Field

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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