(Invited) Toward Si/SiGe Quantum Dot Spin Qubits: Gated Si/SiGe Single and Double Quantum Dots

2019 ◽  
Vol 33 (6) ◽  
pp. 639-647
Author(s):  
Christie Simmons ◽  
J. R. Prance ◽  
Madhu Thalakulam ◽  
B. M. Rosemeyer ◽  
B. J. Van Bael ◽  
...  
2019 ◽  
Vol 100 (3) ◽  
Author(s):  
F. A. Calderon-Vargas ◽  
George S. Barron ◽  
Xiu-Hao Deng ◽  
A. J. Sigillito ◽  
Edwin Barnes ◽  
...  

Open Physics ◽  
2012 ◽  
Vol 10 (5) ◽  
Author(s):  
Cheng-Zhi Fu ◽  
Ming-Yu Song

AbstractWe propose an alternative scheme for one-step implementing three-qubit controlled phase-flip gate of spin qubits in spatially separated double quantum dots with a superconducting stripline resonator (SSR). Due to the switchable coupling effect between the double quantum dots and SSR, the present scheme could be easily generalized for multi-qubits. The feasibility of the present scheme is characterized by exact numerical simulations that incorporate various sources of experimental noise. Our results show the possibility to realize this proposed scheme within current experimental technologies.


2006 ◽  
Vol 74 (24) ◽  
Author(s):  
A. Ramšak ◽  
J. Mravlje ◽  
R. Žitko ◽  
J. Bonča

2004 ◽  
Vol 22 (1-3) ◽  
pp. 518-521 ◽  
Author(s):  
T. Kodera ◽  
W.G. van der Wiel ◽  
K. Ono ◽  
S. Sasaki ◽  
T. Fujisawa ◽  
...  

2016 ◽  
Vol 30 (22) ◽  
pp. 1650266 ◽  
Author(s):  
Yan-Hua Liao ◽  
Jin Huang ◽  
Wei-Zhong Wang

We study the transport properties in double quantum dots asymmetrically coupled to leads in magnetic field. We focus on the situation in which the second dot (QD2) couples with the leads with a weak hybridization function. The results shows that by tuning the energy level [Formula: see text] of QD2 one can control the conductance and its spin polarization of the system. In the absence of magnetic field [Formula: see text], with increasing [Formula: see text], the conductance shows a dip structure. This behavior of conductance results from a continuous triplet–doublet quantum phase transition. In the presence of magnetic field [Formula: see text], we obtain a perfect spin filtering with a fully-polarized conductance of up-spin or down-spin.


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