A two-step linear inversion of two-dimensional electrical conductivity

1995 ◽  
Vol 43 (4) ◽  
pp. 405-415 ◽  
Author(s):  
C. Torres-Verdin ◽  
T.M. Habashy
2021 ◽  
Author(s):  
Tao Li ◽  
Xuefeng Chang ◽  
Lifang Mei ◽  
Xiayun Shu ◽  
Jidong Ma ◽  
...  

Ti3C2Tx is a promising new two-dimensional layered material for supercapacitors with good electrical conductivity and chemical stability. However, Ti3C2Tx has problems such as collapse of the layered structure and low...


2019 ◽  
Vol 1163 ◽  
pp. 012006
Author(s):  
Yuri Yu Tarasevich ◽  
Andrei V Eserkepov ◽  
Irina V Vodolazskaya ◽  
Petr G Selin ◽  
Valentina V Chirkova ◽  
...  

2021 ◽  
Author(s):  
Qizhi Xu ◽  
Boyuan Zhang ◽  
Yihang Zeng ◽  
Amirali Zangiabadi ◽  
Hongwei Ni ◽  
...  

Ultrathin porous films held together by non-covalent van der Waals interactions was obtained by a top-down approach, which is then utilized as channel material in a two-dimensional planar field-effect transistor device through easy stamp transfer.


1989 ◽  
Vol 67 (4) ◽  
pp. 212-217 ◽  
Author(s):  
W. Allegretto ◽  
A. Nathan ◽  
K. Chau ◽  
H. P. Baltes

We present results of electrothermal interactions in fine geometry contacts and vias. The results have been obtained using a two-dimensional model based on the finite-box procedure. For the contact geometry, large electric potential gradients and consequently high Joule-heating effects develop at the interface, which is relatively low in electrical conductivity. In the case of the via, however, temperature escalations result from singularities in the electric field at geometrically imperfect locations, owing to inadequate step coverage in the metallization process. In particular, we discuss the treatment of boundary conditions for the temperature equation.


Nano Letters ◽  
2018 ◽  
Vol 18 (9) ◽  
pp. 6030-6036 ◽  
Author(s):  
Shuai Zhang ◽  
Lei Gao ◽  
Aisheng Song ◽  
Xiaohu Zheng ◽  
Quanzhou Yao ◽  
...  

The network model of electron orbits coupled by magnetic breakdown is extended to a two dimensional metal containing dislocations. It is shown that the network is still likely to be a valid representation, but the phase lengths of the arms are altered, and a very low dislocation density (about one per electron orbit) is enough to produce almost complete randomization. The Bloch-like quasi-particles that can travel in straight lines on a perfect network are now heavily scattered, and it is preferable to think of electrons performing a random walk on the arms of the network, although the justification for this procedure is somewhat doubtful. A simpler alternative to Falicov & Sievert’s method is presented for calculating the electrical conductivity of a random-phase network, and is extended to cases where randomness affects only some of the phases, as is believed to be the situation in real metals like zinc and magnesium.


2008 ◽  
Vol 50 (4) ◽  
pp. 780-784 ◽  
Author(s):  
B. M. Askerov ◽  
G. I. Guseĭnov ◽  
V. R. Figarov ◽  
S. R. Figarova

2019 ◽  
Vol 13 (3) ◽  
pp. 427-443 ◽  
Author(s):  
Aswathy Vasudevan ◽  
Vasyl Shvalya ◽  
Aleksander Zidanšek ◽  
Uroš Cvelbar

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