bipolaron model
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2019 ◽  
Vol 31 (02) ◽  
pp. 1950006
Author(s):  
Gonzalo A. Bley

In the context of the massless Nelson model, we prove that two non-relativistic nucleons interacting with a massless meson field do not bind when a sufficiently strong Coulomb repulsion between the nucleons is added to the Hamiltonian. The result holds for both the renormalized and unrenormalized theories, and can also be applied to the so-called piezoelectric polaron model, which describes an electron interacting with the acoustical vibrational modes of a crystal through the piezoelectric interaction. The result can then be interpreted as well as a no-binding statement about piezoelectric bipolarons. The methods used allow also for a significant reduction of about 30% over previously known no-binding conditions for the optical bipolaron model of H. Fröhlich.





2015 ◽  
Vol 3 (46) ◽  
pp. 12056-12060 ◽  
Author(s):  
Lixiang Chen ◽  
Yanlian Lei ◽  
Qiaoming Zhang ◽  
Zuhong Xiong

We developed the bipolaron model to explain the negative MC in an ITO/CuPc/Al single layer device, suggesting that traps existing in CuPc thin film can assist the formation of bipolarons through lowering the formation energy.



SPIN ◽  
2014 ◽  
Vol 04 (02) ◽  
pp. 1440010 ◽  
Author(s):  
R. GENG ◽  
R. C. SUBEDI ◽  
S. LIANG ◽  
T. D. NGUYEN

We report studies of magnetic field effect (MFE) in polymer light-emitting electrochemical cells (PLEC) using the "super-yellow" poly-(phenylene vynilene) (SY-PPV) polymer in vertical and planar device configurations. The purpose is to discern the existing MFE mechanisms in organic light emitting diodes (OLEDs) where the current and electroluminescence are strongly modulated by a small applied magnetic field. In particular, we investigate the mutual relationship between magneto-conductance (MC) and magneto-electroluminescence (MEL) by studying the role of polaron density dissociated from polaron pairs (PP) on these magnetic responses. In general, the dissociated polaron density is determined by the PP dissociation rate and the PP density. For the planar PLEC, which possesses a small dissociation rate, we observe small and negative MC at all applied voltages regardless of the emission intensity, while MEL becomes positive when electroluminescence quantum efficiency increases. The MC has a much narrower width than the MEL, indicating that the MC and MEL do not share a common origin. However, MC reverses and has the same width as MEL when the device is exposed to a threshold laser power. For the vertical PLEC, characterized by a large dissociation rate, MC and MEL are positive and have the same width. We discuss the results using the existing MFE mechanism in OLEDs. We show that the PP model can explain the positive MEL and MC, while the negative MC can be explained by the bipolaron model. Finally, we present a possibility to complete an all-organic PLEC magnetic sensor by using an inkjet printer.



2013 ◽  
Author(s):  
M. K. Ben Salem ◽  
Y. Slimani ◽  
E. Hannachi ◽  
A. Hamrita ◽  
F. Ben Azzouz ◽  
...  


2011 ◽  
Vol 24 (8) ◽  
pp. 2237-2242 ◽  
Author(s):  
A. Esmaeili ◽  
H. Sedghi ◽  
M. M. Golzan ◽  
M. Amniat-Talab


2010 ◽  
Vol 23 (4) ◽  
pp. 045003 ◽  
Author(s):  
S Aghabagheri ◽  
M R Mohammadizadeh
Keyword(s):  


2008 ◽  
Vol 103 (7) ◽  
pp. 07F303 ◽  
Author(s):  
W. Wagemans ◽  
F. L. Bloom ◽  
P. A. Bobbert ◽  
M. Wohlgenannt ◽  
B. Koopmans




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