entanglement for two qubits interacting with a thermal field mikhail mastyugin the xxii...
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Entanglement for two qubits interacting with a thermal field
Mikhail Mastyugin
The XXII International Workshop High Energy Physics and Quantum Field Theory
June 24 – July 1, 2015 Samara, Russia
• The magnetic flux through the hole superconductor takes discrete values
• Josephson tunneling contact - two superconductors S1 and S2, which separated by a thin dielectric layer
7 20 2 10
2
hcФ Гс см
e
Josephson predicted 2 effects: • The dependence of the superconducting current through the tunneling
barrier of the phase difference at the contact
Ic – The critical current • Feedback voltage at the contact with the derivative of the phase
difference time
Alternating current oscillates at a frequency
sincI I
2
h dV
e dt
2eV
Concepts of superconducting qubits
• Josephson coupling energy
• Josephson inductance
• The charge (Coulomb) energy
2c
j
IE
e
2 cosjc
LeI
2(2 )
2c
eE
C
• one-contact flux qubit and his basic
state
The potential energy U (φ) when β <1, the potential has a minimum;
when β> 1 - two minimums
2( )( ) [(1 cos ) ]
2e
jU E
0
2 cLI
Ф
Main characteristics of Josephson junctions:
Flux qubits:
• three-contact flux qubit
the potential energy U (φ) in the case of low inductance
β << 1 and f = 0, then the potential has two minimums at the points:
Standing in the local minima correspond to the two currents
1( , ) {2 2cos cos cos(2 ( ) 2 )}
2jU E f
0
1/ 2еФf
Ф
0; arccos1/ 2
2, 1 1/ (2 )L R cI I
Superconducting qubit stream with Josephson junctions :
• Two superconducting qubits interact with a superconducting
electric "resonator" (LC-circuit)
The scheme transitions in a three-level artificial atom Δ-type and effective
two-level atom with degenerate two-photon transition.
• A qubit interact with a superconducting electric
"resonator" (LC-circuit), the second qubit is outside the cavity
= 2eg
The Hamiltonian interaction
The evolution operator
The reduced density matrix
Initially, the resonator field is in single-mode thermal field
The atoms are in the form of coherent states
22 2
1 2 2 1=1
= ( ) ( ), (1)i ii
H g a R a R R R R R
Influence of atomic coherence and dipole-dipole interactionon the entanglement of two qubits induced by thermal noise
11 12 13 14
21 22 23 24
31 32 33 34
41 42 43 44
( ) = .(2)
U U U U
U U U U
U t U U U U
U U U U
( ) = ( ) (0) (0) ( ).A F F At Tr U t U t
(0) = ( ) | |,Fn
P n n n ( ) =(1 )
n
n
nP n
n
1 21 1 1 2 2 21) | (0) = cos | sin | , | (0) = cos | sin | .
i ie e
2) | (0) = cos | , sin | , ,ie
The matrix elements of the evolution operator
criterion Perez Horodetskih or "negative" = 2 ,i
i
2 2 2 2 2 211 14 41= 1 2 , = 2 , = 2 ,
A A AU a a U a a U a a
2 2 2 244 12 13 21 31= 1 2 , = = , = = ,
A B BU a a U U a U U a
2 224 34 42 43= = , = = ,
B BU U a U U a
22 33= =U Uexp ( )
2= [1 exp( )] 2 exp( (3 ) ] [1 exp( )] ,
4 2
gi t
gig t i t ig t
23 32= =U U
exp ( )2
= [1 exp( )] 2 exp( (3 ) ] [1 exp( )] ,4 2
gi t
gig t i t ig t
= exp cos sin 1,2 2 2
g g gA i t t i t
= exp ( ) 1 exp( )
2
gB i t ig t
2 2 2 2 2 2 2 2 2= , = 2( ), = 8( ) .a a a a a a a ag
1
11 12 13 14*12 22 2 24* *13 23 33 34* * *14 24 34 44
( ) ( ) ( ) ( )
( ) ( ) ( ) ( )( ) (4)
( ) ( ) ( ) ( )
( ) ( ) ( ) ( )
TA
t t t t
t t t tt
t t t t
t t t t
The initial coherent atomic not entangled statesThe initial coherent atomic not entangled states
Fig. 1. Time-dependent parameter entanglement for different initial coherent atomic states: , (dashed line) and
(solid line). The average number of photons in the mode . The constant dipole-dipole interaction of atoms .
1 21 1 1 2 2 21) | (0) = cos | sin | , | (0) = cos | sin | .
i ie e
1 2 / 4 1 2 0 1 2 1 2 / 4, / 4, 0
= 0,01n0,1
Fig.2. The time dependence of the parameter for the entanglement
of incoherent and coherent the initial states of atoms. The first case corresponds to the dashed, and the second - a solid line. The average number of photons in the mode . The constant dipole-dipole interaction of atoms . Phase states of atoms in both cases are the same .
1 2/ 2, 0 1 2/ 4, / 4
= 5n0,1 1 2 0
Figure 3. The time dependence of the parameter entanglement for coherent initial states of atoms
and different values of the constant dipole-dipole interaction: α = 0 (dashed line) and α = 0,1 (solid line). The average number of photons in the mode
Figure 4. The time dependence of the parameter entanglement for coherent initial states of atoms
and different values of the relative phase of the atomic states (solid line) and (dashed line). The average number of photons in the mode
The constant dipole-dipole interaction of atoms α = 0,1.
1 2 1 2 / 4, / 4, 0
= 0,1n
1 2/ 4, / 4
0 / 2
= 0,05n
2) | (0) = cos | , sin | , ,ie
The initial coherent atomic entangled statesThe initial coherent atomic entangled states
Fig.5. Time-dependent parameter entanglement for initial entangled states (solid line), (dashed line), (dotted). The average number of photons in the mode , constant dipole-dipole interaction α=0,1 and
Fig.6. Time-dependent parameter entanglement for initial entangled states (solid line), (dashed line), (dotted). The average number of photons in the mode , constant dipole-dipole interaction α=0,1 and
/ 4 cos 0.4 / 2
= 0,1n3 / 3
/ 3
0 / 2
= 0,1n
Hamiltonian
starting the atomic density matrix
Initially, the resonator field is in single-mode thermal field
Atoms are in coherent states
eigenfunctions
Entanglemen of two supercondacted qubets one of wich is a traped in a cavity
(0) = ( ) | |,Fn
P n n n ( ) =(1 )
n
n
nP n
n
1 21 1 1 2 2 21) | (0) = cos | sin | , | (0) = cos | sin | .
i ie e
1 2 3 4| = ( | , , 2 | , , 1 | , , 1 | , , ) ( = 1, 2,3,4).in in i n i n i n i nC X n X n X n X n i
1 2 1 1 1 2 1 2= (1/ 2) ( ) ( ) ( ),z zH a a g a a J
1 2 1 2(0) =| (0) | (0) (0) | (0) | .A
( ) ( )kiE t
k kk
t C t e Ф
Here
Where
energy eigenvalues
Where
2 2 2 21 2 3 4= 1/ | | | | | | | |in i n i n i n i nC X X X X
21
11
1= ;
2 2 1 2
n n
nXn n
2
12
1= ;
2 1n
nXn
2
13
3 2= ;
2 1n
n
nX
n
14 = 1;nX 2
1
21
1= ;
2 2 1 2
n n
nXn n
2
22
1= ;
2 1n
nXn
2
23
3 2= ;
2 1n
n
nX
n
24 = 1;nX 22
31
1= ;
2 2 1 2
n n
nXn n
2
32
1= ;
2 1n
nXn
2
33
3 2= ;
2 1n
n
nX
n
34 = 1;nX 22
41
1= ;
2 2 1 2
n n
nXn n
2
42
1= ;
2 1n
nXn
243 = ;
2 1n
nXn
44 1nX
2 21 2
2 2 2 4
3 2 , 3 2 ,
1 6 4 , 1 (6 4 )
n n n n
n n
n n
n n
1 2/ = ( 1) / 2, / = ( 1) / 2,n n n n n nE n A B E n A B
3 4/ = ( 1) / 2, / = ( 1) / 2.n n n n n nE n A B E n A B 2 2 2= 4 6 2 , = 2 4( 1) ( 1),n nA n B n = /J g
reduced atomic density matrix
criterion Perez Horodetskih or "negative"
21 1| = ( / )[| , ,1 (1/ ) | , ,0 ], = 0;E
2 2| = (1/ 2)[(1/ ) | , ,1 | , ,0 ( / ) | , ,0 ], / = ;E
3 2| = (1/ 2)[ (1/ ) | , ,1 | , ,0 ( / ) | , ,0 ], / = ,E 2= 1
0 =| , ,0 , 0 =E
11 12 13 14*12 22 23 24* *13 23 33 34* * *14 24 34 44
( ) = .A t
= 2 ,ii
* *11 12 13 23* * *12 22 14 241
13 14 33 34*
23 24 34 44
( ) = .T
A t
Fig. 1. The time dependence of the parameter ɛ(t) with and . The initial atomic states: (a) , (b) and (c)
= 0.01n = 0,1| , | ,
1 2| (0) = (1/ 2(| | ), | (0) = (1/ 2(| | )A A
Fig. 2. The time dependence of the parameter ɛ(t) for and α = 1. The initial atomic state .
Fig. 3. The time dependence of the parameter ɛ(t) for
and α = 1. The initial atomic state .
= 0.1n
= 10n
,
,