channel spin
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2019 ◽  
Vol 100 (7) ◽  
Author(s):  
G. G. Blesio ◽  
L. O. Manuel ◽  
A. A. Aligia ◽  
P. Roura-Bas
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2019 ◽  
Vol 28 (4) ◽  
pp. 040702
Author(s):  
Peng-Cheng Du ◽  
Jian-Jun Li ◽  
Si-Jia Yang ◽  
Xu-Tong Wang ◽  
Yan Zhuo ◽  
...  

2019 ◽  
Vol 28 (4) ◽  
pp. 040703 ◽  
Author(s):  
Jian-Jun Li ◽  
Peng-Cheng Du ◽  
Ji-Qing Fu ◽  
Xu-Tong Wang ◽  
Qing Zhou ◽  
...  
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2019 ◽  
Vol 27 (2) ◽  
pp. 597 ◽  
Author(s):  
Guiying Zhang ◽  
Shengjie Huang ◽  
Feixiang Xu ◽  
Zhenghui Hu ◽  
Qiang Lin

2018 ◽  
Vol 54 (7) ◽  
pp. 418-420 ◽  
Author(s):  
A. Acevedo ◽  
I. Gomez‐Arista ◽  
O. Kolokoltsev ◽  
M.H. Montiel Sánchez ◽  
R. Castañeda Guzmán

2015 ◽  
Vol 15 (10) ◽  
pp. 7518-7521
Author(s):  
Youn Ho Park ◽  
Hyung-Jun Kim ◽  
Joonyeon Chang ◽  
Heon-Jin Choi ◽  
Hyun Cheol Koo

In a semiconductor channel, spin-orbit interaction is divided into two terms, Rashba and Dresselhaus effects, which are key phenomena for modulating spin precession angles. The direction of Rashba field is always perpendicular to the wavevector but that of Dresselhaus field depends on the crystal orientation. Based on the individual Rashba and Dresselhaus strengths, we calculate spin precession angles for various crystal orientations in an InAs quantum well structure. When the channel length is 1 μm, the precession angle is 550° for the [110] direction and 460° for the [1–10] direction, respectively. Using the two spin transistors with different crystal directions, which play roles of n- and p-type transistors in conventional charge transistors, we propose a complementary logic device.


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