Transcript Quantum versus Classical Correlations in Gaussian States

Quantum versus Classical
Correlations in Gaussian States
Gerardo Adesso
Imperial College London 10/08/2010
joint work with Animesh Datta (Imperial College / Oxford)
School of Mathematical Sciences
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Outline
• Quantum versus classical correlations
• Quantum discord
• Gaussian quantum discord
• Structure of Gaussian correlations
• Open problems
Quantum versus Classical Correlations in Gaussian States
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Correlations
Classical correlations
A
B
Quantum correlations
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Correlations
A
B
• Pure global composite states:
▫ entanglement = nonlocality
= nonclassicality (quantum correlations)
• Mixed global composite states:
▫ Werner 1989: separable = classically correlated
Quantum versus Classical Correlations in Gaussian States
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Quantumness in separable states
Nonorthogonal separable states cannot be
discriminated exactly
Measuring a local observable on a separable
bipartite state will perturb the state
The eigenvectors of a separable state can be
entangled superpositions
…
In general separable states have not
a purely classical nature
Quantum versus Classical Correlations in Gaussian States
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A new paradigm
M. Piani, P. Horodecki, R. Horodecki, PRL 2008
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Quantum discord
• A measure that strives at capturing all quantum correlations,
beyond entanglement, which can be nonzero also in separable states
• Introduced a decade ago in two independent works (Ollivier/Zurek
and Henderson/Vedral)
# preprints
• Recently became very popular: stats from arXiv:quant-ph…
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Quantum discord
• Almost all bipartite states have nonzero quantum discord (purely
classically correlated states are of zero measure) A. Ferraro et al. PRA 2010
• Reduces to the entropy of entanglement on pure bipartite states
• Quantum discord without entanglement may allow for a
computational speed-up in the DQC1 model of quantum
computation A. Datta et al. 2008-2010; experiment: M. Barbieri et al.
PRL 2008
discord
entanglement
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Mutual information: classical
H (A )
H (B )
measuring total
correlations…
I (A : B ) = H (A ) + H (B ) - H (A , B )
J (A : B ) = H (A ) - H (A | B )
all equal
(Bayes’ rule)
J (B : A ) = H (B ) - H (B | A )
Quantum versus Classical Correlations in Gaussian States
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Mutual information: quantum
H ® S ( ñ ) = - T r[ñ log ñ ]
S (ñA )
S (ñB )
I (ñA B ) = S (ñA ) + S (ñB ) - S (ñA B )
J
J
¬
®
(ñA B ) = S (ñA ) - S ( A | B )
w h a t a r e t h ese ? ?
(ñB A ) = S (ñB ) - S ( B | A )
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Conditional entropy
• Introduce POVM on B:
B
S (ñA )
{P i } ,
S (ñB )
å
P
B
= 1
i
i
• Posterior state of A after B
has been measured:
B
ñ A |i =
I (ñA B )
• looking for the “least
disturbing measurement”:
Quantum versus Classical Correlations in Gaussian States
T rB [ P i ñ A B ]
,
pi
B
w it h p i = T r[P i ñ A B ]
S ( A | B ) º in f
P
B
i
å
p i S ( ñ A |i )
i
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Bipartite correlations
A
• Total correlation
B
I (ñA B ) = S (ñA ) + S (ñB ) - S (ñA B )
• One-way classical correlation
J
¬
Henderson, Vedral, JPA 2001
^ñ
( A B ) = S ( ñ A ) - S ( A | B ) = S ( ñ A ) - in f
P
• Quantum discord
D
¬
^ñ
( A B ) = I (ñA B ) - J
å
p i S ( ñ A |i )
i
Ollivier, Zurek, PRL 2001
¬
(^ñ A B )
= S ( ñ B ) - S ( ñ A B ) + in f
P
Quantum versus Classical Correlations in Gaussian States
B
i
B
i
å
p i S ( ñ A |i )
i
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Quantum discord
• For classical states (classical probability distribution embedded into
density matrices) I=J hence the quantum discord vanishes
• Zurek introduced it in the context of environment-induced
selection, identifying classical states with the pointer states
• The optimization involved in the conditional entropy is hard. Closed
analytical formulas are available only for special families of twoqubit staes (X-shaped), not even for arbitrary states of two qubits
• Two recent independent works, including this one, defined a
Gaussian version of the quantum discord for bipartite Gaussian
states, where the optimization is restricted to Gaussian
measurements P. Giorda & M.G.A. Paris PRL 2010; GA & A. Datta PRL 2010
• We have solved the optimization problem and obtained a simple
formula for the Gaussian quantum discord of arbitrary two-mode
Gaussian states
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Gaussian states
 Very natural: ground and thermal states of all physical systems in the
harmonic approximation regime (M.S.Kim: like orange juice and sunshine)
 Relevant theoretical testbeds for the study of structural properties of
entanglement and correlations, thanks to the symplectic formalism
 Preferred resources for experimental unconditional implementations of
continuous variable protocols
 Crucial role and remarkable control in quantum optics
- coherent states
- squeezed states
- thermal states
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Gaussian operations
Gaussian states can be
efficiently:
 displaced
(classical currents)
 squeezed
(nonlinear crystals)
 rotated
(phase plates, beam splitters)
 measured
(homodyne detection)
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Gaussian operations
Gaussian states can be
efficiently:
 displaced
(classical currents)
 squeezed
(nonlinear crystals)
 rotated
(phase plates, beam splitters)
 measured
(homodyne detection)
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Gaussian operations
Gaussian states can be
efficiently:
 displaced
(classical currents)
 squeezed
(nonlinear crystals)
 rotated
(phase plates, beam splitters)
 measured
(homodyne detection)
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Gaussian operations
Gaussian states can be
efficiently:
 displaced
(classical currents)
 squeezed
(nonlinear crystals)
 rotated
(phase plates, beam splitters)
 measured
(homodyne detection)
Quantum versus Classical Correlations in Gaussian States
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Gaussian operations
Gaussian states can be
efficiently:
 displaced
(classical currents)
 squeezed
(nonlinear crystals)
 rotated
(phase plates, beam splitters)
 measured
(homodyne detection)
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Gaussian states: formalism
• Up to local unitaries, Gaussian states are completely
specified by the covariance matrix…
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s = s AB = ç T
= ç
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• … or equivalently by the
four symplectic invariants
A = d et a , B = d et b , C = d et g , D = d et s
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Gaussian POVMs
• All the measurements that can be done by linear optics
(appending Gaussian ancillas, manipulating with
symplectic transformations, plus homodyne detection):
- 1
0
†
†
*
P B ( h ) = p Wˆ B ( h ) P BWˆ B ( h ) , w h er e Wˆ B ( h ) = ex p ( hbˆ - h bˆ ) ,
p
- 1
ò
2
d h P B ( h ) = 1, a n d P
0
B
is t h e d en sit y m a t r ix of a
sin gle-m od e G a u ssia n st a t e w it h cov a r ia n ce m a t r ix s
0
• The posterior state ñ A | h of A after measuring B has a
covariance matrix e (independent of the measurement outcome)
e = a - g(b + s 0 )
Quantum versus Classical Correlations in Gaussian States
- 1
g
T
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Gaussian quantum discord
• The Gaussian quantum discord is the quantum discord
of a bipartite Gaussian state where the optimization in
the conditional entropy is restricted to Gaussian POVMs
D
¬
( ñ A B ) = S ( ñ B ) - S ( ñ A B ) + in f
P
B
(h)
ò dhp
B
( h )S ( ñ A | h )
• and can be rewritten as
D
¬
( s A B ) = f ( B ) - f ( n - ) - f ( n + ) + in f f ( d et e )
s
0
▫ where the symplectic eigenvalues are
2
2n ± = D ±
Quantum versus Classical Correlations in Gaussian States
2
D - 4D ,
D = A + B + 2C
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Gaussian quantum discord
• Optimal POVM: heterodyne for squeezed thermal states,
homodyne for another class of states, something inbetween for the other two-mode Gaussian states
ìï
ï 2C
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in f d et ( e ) = ïí
s0
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2
+ (- 1 + B
)(-
A + D )+ 2 |C |
(AB - C
2
C
2
+ (- 1 + B
)(-
A + D)
2
1+ B
+ D -
Quantum versus Classical Correlations in Gaussian States
,
(D
(A B
+ D)
- AB
2
)
£
(1 +
B )C
2
(A
+ D );
)
C
4
2
+ (- A B + D ) - 2C
2
,
o t h er w ise .
2B
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Discord/separability/entanglement
• By relating the nullity of discord with saturation of
strong subadditivity of entropy, we demonstrated
that (for finite mean energies) the only two-mode
Gaussian states with zero Gaussian discord
are product states
• All correlated Gaussian states (including all
entangled states and all non-product separable
mixed states) are quantumly correlated!
• This proves the truly quantum nature of Gaussian
states despite their positive Wigner function…
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Discord/separability/entanglement
• Consider this class of states (box=two-mode squeezing)
▫ s: initial entanglement; r: entanglement degradation
w h en s , r ® ¥
A
s
s
B
r
*
AB
D
D
¬
® 0
®
® 1
C
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Discord/separability/entanglement
m a x d iscor d is lim it ed t o 1
if D
Quantum versus Classical Correlations in Gaussian States
¬
> 1 Þ en t a n gled
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Discord/separability/entanglement
1
D
®
(s
*
AB
)
¬
D (s
*
AB
)
EG : G a u ssia n E n t a n glem en t of F or m a t ion
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Other results & comments
• Via the Koashi-Winter duality between entanglement and
one-way classical correlations we can derive a closed formula
for the Gaussian EoF of a family of three-mode Gaussian
states
• Only in very special cases we can prove that the Gaussian
quantum discord realizes the absolute minimum in the
conditional entropy optimization not constrained to Gaussian
POVMs (this is related to the problem of additivity of bosonic
channel capacity etc…)
• It would be interesting to prove, or show counterexamples to
it, that Gaussian POVMs are always optimal among all
continuous variable measurements (including photodetection
etc.)
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Summary
• The concept of quantum correlations goes beyond
entanglement
• Quantum discord is a bona fide measure of such general
quantum correlations
• Quantum discord can be computed for Gaussian states
under Gaussian measurements
• All correlated Gaussian states have quantum correlations
• They are limited for separable states
• They admit upper and lower bounds as a function of the
entanglement, for entangled states
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Open problems
• Maximum discord for separable states in any
dimension.
▫ known for qubits,
numerically, to be 1/3
Al-Qasimi & James, arXiv:1007.1814
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Open problems
• Operational interpretation of discord
• Usefulness of quantum correlations in separable
states for quantum information processing
• Understanding connection with other
nonclassicality indicators in continuous variable
systems (e.g. in terms of P function)
• Producing a theory of quantum correlations, with
axioms to be satisfied by any valid measure of
quantum correlations (e.g. nonincreasing under
local operations and classical communication…)
•…
Quantum versus Classical Correlations in Gaussian States
Imperial College London 10/08/2010
Thank you
Quantum versus Classical Correlations in Gaussian States
Imperial College London 10/08/2010