scholarly journals Comparison of cloud-based ion trap and superconducting quantum computer architectures

2021 ◽  
Vol 3 (3) ◽  
pp. 033801
Author(s):  
S. Blinov ◽  
B. Wu ◽  
C. Monroe
2020 ◽  
Vol 19 (10) ◽  
Author(s):  
Laszlo Gyongyosi

Abstract Superconducting gate-model quantum computer architectures provide an implementable model for practical quantum computations in the NISQ (noisy intermediate scale quantum) technology era. Due to hardware restrictions and decoherence, generating the physical layout of the quantum circuits of a gate-model quantum computer is a challenge. Here, we define a method for layout generation with a decoherence dynamics estimation in superconducting gate-model quantum computers. We propose an algorithm for the optimal placement of the quantum computational blocks of gate-model quantum circuits. We study the effects of capacitance interference on the distribution of the Gaussian noise in the Josephson energy.


Author(s):  
L. Riesebos ◽  
X. Fu ◽  
S. Varsamopoulos ◽  
C. G. Almudever ◽  
K. Bertels

2013 ◽  
Vol 88 (4) ◽  
Author(s):  
Yu Tomita ◽  
Mauricio Gutiérrez ◽  
Chingiz Kabytayev ◽  
Kenneth R. Brown ◽  
M. R. Hutsel ◽  
...  
Keyword(s):  
Ion Trap ◽  

2004 ◽  
Vol 4 (4) ◽  
pp. 237-251
Author(s):  
A.G. Fowler ◽  
S.J. Devitt ◽  
L.C.L. Hollenberg

Shor's algorithm, which given appropriate hardware can factorise an integer N in a time polynomial in its binary length L, has arguably spurred the race to build a practical quantum computer. Several different quantum circuits implementing Shor's algorithm have been designed, but each tacitly assumes that arbitrary pairs of qubits within the computer can be interacted. While some quantum computer architectures possess this property, many promising proposals are best suited to realising a single line of qubits with nearest neighbour interactions only. In light of this, we present a circuit implementing Shor's factorisation algorithm designed for such a linear nearest neighbour architecture. Despite the interaction restrictions, the circuit requires just 2L+4 qubits and to leading order requires 8L^4 2-qubit gates arranged in a circuit of depth 32L^3 --- identical to leading order to that possible using an architecture that can interact arbitrary pairs of qubits.


2020 ◽  
Vol 101 (3) ◽  
Author(s):  
Justin Loye ◽  
José Lages ◽  
Dima L. Shepelyansky

Author(s):  
G.P.T. Lancaster ◽  
S. Gulde ◽  
M. Riebe ◽  
C. Becher ◽  
H. Haffner ◽  
...  
Keyword(s):  
Ion Trap ◽  

Nature ◽  
2003 ◽  
Vol 421 (6918) ◽  
pp. 48-50 ◽  
Author(s):  
Stephan Gulde ◽  
Mark Riebe ◽  
Gavin P. T. Lancaster ◽  
Christoph Becher ◽  
Jürgen Eschner ◽  
...  
Keyword(s):  
Ion Trap ◽  

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