|
2000Q
|
D-Wave
|
Los Alamos National Laboratory
|
|
|
|
2000Q
|
D-Wave
|
2017
|
annealing
|
superconducting
|
2000
|
Chimera
|
|
|
|
2X
|
D-Wave
|
|
|
|
|
2X
|
D-Wave
|
2015
|
annealing
|
superconducting
|
1000
|
Chimera
|
|
|
|
Acorn
|
Rigetti
|
|
2017
|
|
|
Acorn
|
Rigetti
|
2017
|
circuit
|
superconducting
|
19
|
square lattice
|
|
|
|
Advantage
|
D-Wave
|
|
|
|
|
Advantage
|
D-Wave
|
2020
|
annealing
|
superconducting
|
5000
|
Pegasus
|
|
|
|
Agave
|
Rigetti
|
|
2017
|
|
|
Agave
|
Rigetti
|
2017
|
circuit
|
superconducting
|
8
|
ring
|
|
|
|
Algiers
|
IBM
|
|
|
|
|
Falcon r5.11
|
IBM
|
|
circuit
|
superconducting
|
27
|
heavy-hex lattice
|
|
X, SX, RZ, CX
|
|
Ankaa-2
|
Rigetti
|
|
2023
|
|
|
Ankaa-2
|
Rigetti
|
2023
|
circuit
|
superconducting
|
84
|
square lattice
|
|
X, SX, RZ, CZ, SXdg, CPHASE, XY
|
|
Ankaa-9Q-1
|
Rigetti
|
|
2023
|
|
|
Ankaa-9Q-1
|
Rigetti
|
2023
|
circuit
|
superconducting
|
9
|
square lattice
|
|
X, SX, RZ, CZ, SXdg, CPHASE, XY
|
|
Aspen-1
|
Rigetti
|
|
2018
|
|
|
Aspen-1
|
Rigetti
|
2018
|
circuit
|
superconducting
|
16
|
octagon lattice
|
|
|
|
Aspen-10
|
Rigetti
|
|
2021
|
|
|
Aspen-10
|
Rigetti
|
2021
|
circuit
|
superconducting
|
32
|
octagon lattice
|
|
|
|
Aspen-11
|
Rigetti
|
|
2021
|
|
|
Aspen-11
|
Rigetti
|
2021
|
circuit
|
superconducting
|
40
|
octagon lattice
|
|
|
|
Aspen-4
|
Rigetti
|
|
2019
|
|
|
Aspen-4
|
Rigetti
|
2019
|
circuit
|
superconducting
|
13
|
octagon lattice
|
|
|
|
Aspen-7
|
Rigetti
|
|
2019
|
|
|
Aspen-7
|
Rigetti
|
2019
|
circuit
|
superconducting
|
28
|
octagon lattice
|
|
|
|
Aspen-8
|
Rigetti
|
|
2020
|
|
|
Aspen-8
|
Rigetti
|
2020
|
circuit
|
superconducting
|
31
|
octagon lattice
|
|
|
|
Aspen-9
|
Rigetti
|
|
2021
|
|
|
Aspen-9
|
Rigetti
|
2021
|
circuit
|
superconducting
|
32
|
octagon lattice
|
|
|
|
Aspen-M-1
|
Rigetti
|
|
2022
|
|
|
Aspen-M-1
|
Rigetti
|
2022
|
circuit
|
superconducting
|
80
|
octagon lattice
|
|
|
|
Aspen-M-2
|
Rigetti
|
|
2022
|
|
|
Aspen-M-2
|
Rigetti
|
2022
|
circuit
|
superconducting
|
80
|
octagon lattice
|
|
|
|
Aspen-M-3
|
Rigetti
|
|
2022
|
|
|
Aspen-M-3
|
Rigetti
|
2022
|
circuit
|
superconducting
|
80
|
octagon lattice
|
|
|
|
Brisbane
|
IBM
|
|
|
|
|
Eagle r3
|
IBM
|
|
circuit
|
superconducting
|
127
|
heavy-hex lattice
|
|
X, SX, RZ, ECR
|
|
Cairo
|
IBM
|
|
|
|
|
Falcon r5.11
|
IBM
|
|
circuit
|
superconducting
|
27
|
heavy-hex lattice
|
|
X, SX, RZ, CX
|
|
Cleveland
|
IBM
|
|
|
|
|
Eagle r3
|
IBM
|
|
circuit
|
superconducting
|
127
|
heavy-hex lattice
|
|
X, SX, RZ, ECR
|
|
Cusco
|
IBM
|
|
|
|
|
Eagle r3
|
IBM
|
|
circuit
|
superconducting
|
127
|
heavy-hex lattice
|
|
X, SX, RZ, ECR
|
|
DW_2000Q_2_1
|
D-Wave
|
|
|
|
|
2000Q
|
D-Wave
|
2017
|
annealing
|
superconducting
|
2000
|
Chimera
|
|
|
|
DW_2000Q_6
|
D-Wave
|
|
|
|
|
2000Q
|
D-Wave
|
2017
|
annealing
|
superconducting
|
2000
|
Chimera
|
|
|
|
H1-1
|
Quantinuum
|
|
|
|
|
System Model H1
|
Quantinuum
|
2020
|
circuit
|
trapped ion
|
20
|
all-to-all
|
|
U1q, ZZ, RZZ
|
|
H2-1
|
Quantinuum
|
|
|
|
|
System Model H2
|
Quantinuum
|
2023
|
circuit
|
trapped ion
|
32
|
all-to-all
|
|
U1q, ZZ, RZZ
|
|
H2-1
|
Quantinuum
|
|
|
|
|
System Model H2
|
Quantinuum
|
2023
|
circuit
|
trapped ion
|
32
|
all-to-all
|
|
U1q, ZZ, RZZ
|
|
Hanoi
|
IBM
|
|
|
|
|
Falcon r5.11
|
IBM
|
|
circuit
|
superconducting
|
27
|
heavy-hex lattice
|
|
X, SX, RZ, CX
|
|
Ising
|
D-Wave
|
Los Alamos National Laboratory
|
|
|
|
2X
|
D-Wave
|
2015
|
annealing
|
superconducting
|
1000
|
Chimera
|
|
|
|
Kawasaki
|
IBM
|
|
|
|
|
Eagle r3
|
IBM
|
|
circuit
|
superconducting
|
127
|
heavy-hex lattice
|
|
X, SX, RZ, ECR
|
|
Kolkata
|
IBM
|
|
|
|
|
Falcon r5.11
|
IBM
|
|
circuit
|
superconducting
|
27
|
heavy-hex lattice
|
|
X, SX, RZ, CX
|
|
Kyiv
|
IBM
|
|
|
|
|
Eagle r3
|
IBM
|
|
circuit
|
superconducting
|
127
|
heavy-hex lattice
|
|
X, SX, RZ, ECR
|
|
Kyoto
|
IBM
|
|
|
|
|
Eagle r3
|
IBM
|
|
circuit
|
superconducting
|
127
|
heavy-hex lattice
|
|
X, SX, RZ, ECR
|
|
Mumbai
|
IBM
|
|
|
|
|
Falcon r5.10
|
IBM
|
|
circuit
|
superconducting
|
27
|
heavy-hex lattice
|
|
X, SX, RZ, CX
|
|
Nazca
|
IBM
|
|
|
|
|
Eagle r3
|
IBM
|
|
circuit
|
superconducting
|
127
|
heavy-hex lattice
|
|
X, SX, RZ, ECR
|
|
Osaka
|
IBM
|
|
|
|
|
Eagle r3
|
IBM
|
|
circuit
|
superconducting
|
127
|
heavy-hex lattice
|
|
X, SX, RZ, ECR
|
|
Peekskill
|
IBM
|
|
|
|
|
Falcon r8
|
IBM
|
|
circuit
|
superconducting
|
27
|
heavy-hex lattice
|
|
X, SX, RZ, CX
|
|
Poughkeepsie
|
IBM
|
|
|
|
|
Q 20
|
IBM
|
|
circuit
|
superconducting
|
20
|
heavy-hex lattice
|
|
|
|
Quebec
|
IBM
|
|
|
|
|
Eagle r3
|
IBM
|
|
circuit
|
superconducting
|
127
|
heavy-hex lattice
|
|
X, SX, RZ, ECR
|
|
Sherbrooke
|
IBM
|
|
2022
|
|
|
Eagle r3
|
IBM
|
|
circuit
|
superconducting
|
127
|
heavy-hex lattice
|
|
X, SX, RZ, ECR
|
|
Torino
|
IBM
|
|
2023
|
|
|
Heron r1
|
IBM
|
|
circuit
|
superconducting
|
133
|
heavy-hex lattice
|
|
X, SX, RZ, CZ
|