Two-dimensional carrier transport in quantum nanostructures under non quantizing magnetic and high electric fields at low temperature

Author(s):  
K.S. Kumar ◽  
C.J.C. Singh ◽  
P.K. Datta ◽  
S.K. Sarkar
2009 ◽  
Vol 58 (4) ◽  
pp. 2692
Author(s):  
Zhu Yi-Ming ◽  
Kaz Hirakawa ◽  
Chen Lin ◽  
He Bo-Yong ◽  
Huang Yuan-Shen ◽  
...  

1993 ◽  
Vol 103-105 ◽  
pp. 437-442
Author(s):  
B.A. Akimov ◽  
A.V. Albul ◽  
E.V. Bogdanov

1993 ◽  
Vol 8 (1S) ◽  
pp. S447-S450 ◽  
Author(s):  
B A Akimov ◽  
A V Albul ◽  
E V Bogdanov

2010 ◽  
Vol 44-47 ◽  
pp. 2632-2636 ◽  
Author(s):  
Jia Qi Lin ◽  
Chen Wang ◽  
Jun Hui Shi

The EL intensity and the spectrum of the PET films were tested under the low temperature by home-made experimental set-up on the conditions of DC high electric fields and irradiated by xenon lamp. The result shows that there are emission peaks at about 350~450nm, 500~600nm and 750nm in the EL spectrum of the PET films. The intensity of light emission increases with the applied electric fields; the pre-breakdown field is about 3.3MV/cm, this threshold value is no significant change which compares with the normal temperature.


ACS Nano ◽  
2018 ◽  
Vol 12 (7) ◽  
pp. 7109-7116 ◽  
Author(s):  
Jinsu Pak ◽  
Yeonsik Jang ◽  
Junghwan Byun ◽  
Kyungjune Cho ◽  
Tae-Young Kim ◽  
...  

Author(s):  
J. J. Hren ◽  
S. D. Walck

The field ion microscope (FIM) has had the ability to routinely image the surface atoms of metals since Mueller perfected it in 1956. Since 1967, the TOF Atom Probe has had single atom sensitivity in conjunction with the FIM. “Why then hasn't the FIM enjoyed the success of the electron microscope?” The answer is closely related to the evolution of FIM/Atom Probe techniques and the available technology. This paper will review this evolution from Mueller's early discoveries, to the development of a viable commercial instrument. It will touch upon some important contributions of individuals and groups, but will not attempt to be all inclusive. Variations in instrumentation that define the class of problems for which the FIM/AP is uniquely suited and those for which it is not will be described. The influence of high electric fields inherent to the technique on the specimens studied will also be discussed. The specimen geometry as it relates to preparation, statistical sampling and compatibility with the TEM will be examined.


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