Global interconnects in VLSI complexity single flux quantum systems

Author(s):  
Tahereh Jabbari ◽  
Eby G. Friedman
2003 ◽  
Vol 13 (3) ◽  
pp. 3814-3816 ◽  
Author(s):  
N. Harada ◽  
N. Yoshikawa ◽  
K. Yoda ◽  
A. Yoshida ◽  
N. Yokoyama

1993 ◽  
Vol 163 (9) ◽  
pp. 1 ◽  
Author(s):  
B.D. Agap'ev ◽  
M.B. Gornyi ◽  
B.G. Matisov ◽  
Yu.V. Rozhdestvenskii

2018 ◽  
Vol 189 (05) ◽  
Author(s):  
Vladislav Yu. Shishkov ◽  
Evgenii S. Andrianov ◽  
Aleksandr A. Pukhov ◽  
Aleksei P. Vinogradov ◽  
A.A. Lisyansky

2020 ◽  
Vol E103.C (10) ◽  
pp. 547-549
Author(s):  
Yoshinao MIZUGAKI ◽  
Koki YAMAZAKI ◽  
Hiroshi SHIMADA

2011 ◽  
Vol E94-C (3) ◽  
pp. 254-259 ◽  
Author(s):  
Akira FUJIMAKI ◽  
Isao NAKANISHI ◽  
Shigeyuki MIYAJIMA ◽  
Kohei ARAI ◽  
Yukio AKITA ◽  
...  

1999 ◽  
Author(s):  
Konstantin K. Likharev ◽  
P. Bunyk ◽  
W. Chao ◽  
T. Filippov ◽  
Y. Kameda
Keyword(s):  

Author(s):  
Richard Healey

Often a pair of quantum systems may be represented mathematically (by a vector) in a way each system alone cannot: the mathematical representation of the pair is said to be non-separable: Schrödinger called this feature of quantum theory entanglement. It would reflect a physical relation between a pair of systems only if a system’s mathematical representation were to describe its physical condition. Einstein and colleagues used an entangled state to argue that its quantum state does not completely describe the physical condition of a system to which it is assigned. A single physical system may be assigned a non-separable quantum state, as may a large number of systems, including electrons, photons, and ions. The GHZ state is an example of an entangled polarization state that may be assigned to three photons.


Sign in / Sign up

Export Citation Format

Share Document